1982 Recent references (cumulation)

NucZeav

Data

Sheets

37,

1

(1983)

1982 Recent References" (Cumulation) S. R A M A V A T A R A M Brookhaven

National

Laboratory,

Upton,

New

York

11973,

USA

In support of a continuing program of systematic evaluation of nuclear structure data, the National Nuclear Data Center maintains a complete computer f i l e of r e f e r e n c e s to the nuclear physics literature. Each reference is t a g g e d by a keyword string, which indicates the kinds of d a t a w h i c h a r e c o n t a i n e d in the article. A complete master file of Nuclear Structure References ( N S R ) is m a i n t a i n e d by the National Nuclear Data Center. Complete keyword indexes are available to literature published since 1969, a n d some indexing is p r e s e n t with older references. T h e NSR f i l e is u s e d as requested to provide special bibliographies for nuclear physics topics. Any reader who finds errors in the keyword descriptions is u r g e d to r e p o r t them to t h e N a t i o n a l Nuclear Data Data Center so that the master NSR f i l e c a n b e c o r r e c t e d . Requests for special searches of the complete NSR f i l e m a y also be d i r e c t e d to t h e N a t i o n a l N u c l e a r Data C e n t e r . In October 1980 the maintenance of the NSR f i l e became the continuing responsibility of the (US) National Nuclear Data Center (NNDC) a t B r o o k h a v e n National Laboratory. Before that transfer, responsibility for the file resided with its originators, the Nuclear Data Project (NDP) a t O a k R i d g e N a t i o n a l L a b o r a t o r y . tn

1966,

Nuclear nuclear

the

Data

collection of Recent RefeTences Every four months since 1970, has been prepared and published.

first

Sheets.

experiments

was published as a similar indexed

a separate bibliography

issue of to new

The four-month indexes are prepared from additions to t h e N u c l e a r S t r u c t u r e References (NSR) file. I n 1975 a c o m p l e t e index to t h e n u c l e a r physics literature for the years 1969 t h r o u g h 1974 was prepared by the Nuclear Data Project from t h e NSR f i l e a n d published as a s u p p l e m e n t to Volume 16 o f N u c L e a r Data S h e e t s , a n d a s e c o n d cumulation (1975-1977) was published as Volume 24, N u m b e r 4, o f N u c l e a r Data S h e e t s . B e g i n n i n g i n 1978, R e c e n t R e f e r e n c e s is c u m u l a t e d annually, with the third issue of each year completely superseding the two issues previously published d u r i n g t h e s a m e y e a r . A c c o r d i n g l y t h e p r e s e n t i s s u e i n c o r p o r a t e s all r e f r e n c e a n d i n d e x i n g i n f o r m a t i o n from:

N u c L e a r Data S h e e t s V o l u m e N u c l e a r Data S h e e t s V o l u m e

THESE TWO

ISSUES M A Y

35, N u m b e r 36, N u m b e r

1 1

BE D I S C A R D E D

starting with t h e 1981 C u m u l a t i v e Edition, the KEY NUMBERS September to D e c e m b e r will be u n d e r l i n e d . The Volume a n d issue issues p u b l i s h e d to date since 1978 are given o n the n e x t page.

of e n t r i e s for number for the

the period cumulative

NNDC w i l l c o n t i n u e to respond to individual requests for bibliographies on special topics, in addition to t h o s e easily obtained from Recent References. if the required information is a v a i l able from the keyword string, a reference l i s t c a n be p r e p a r e d automatically from the computer files. This service c a n be p r o v i d e d on request, in exchange for the timely communication of new nuclear physics results (e.g., p r e p r i n t s ) . A current c o p y o f t h e NSR f i l e m a y a l s o be o b t a i n e d in a standard format on magnetic t a p e f r o m NNDC.

Acknowledgments: Since 1964 each report of n e w e x p e r i m e n t a l nuclear physics results published in the journal Nuclear Physics has been accompanied by a descriptive keyword string, which was prepared by the report's authors and edited by the Nuclear Structure References compiler. In more recent years, keyword strings have also been published with ex~Serimental reports in Physical Review C, J o u r n a l of Physics (London) G, a n d t h e P r o c e e d i n g s (Izvestia) of the USSR A c a d e m y of Sciences. The inclusion of keyword strings with published articles has greatly simplified the task of maintaining an indexed file of nuclear structure references. The author wishes to a c k n o w l e d g e the contribution o f T. D a w s o n , P. D i x o n , A, F u o c o , J. R o y s a n d S. S a n t o s (NNDC) i n p r e p a r i n g the data base from which this publication was made.

*Research sponsored by the Division of Basic Energy Sciences, US D e p a r t m e n t of Energy, u n d e r c o n t r a c t No. DE-AC02-76CH00016 with A~sociated Universities, Inc.

NUCLEAR

DATA

SHEETS

Introduction

Recent References is a current guide to experimental nuclear physics papers, and is three times per year as part of the Nuclear Data Sheets. The information is described keyword string as explained on the next page. From the keywords, a user should be able whether the indexed paper contains results that are relevant to his interests.

Coverage

issued by a to tell

Organization

Each Recent References issue is a supplement to earlier issues published in Nuclear Data Sheels.~ The present issue covers literature received by the National Nuclear Data Center or assigned key numbers between January and December 1982. For several 'core' journals, the last issue scanned for this edition of Recent References is given in the following table: Recent

References coverage (partial list) Last Issue Scanned

Journals Acta Phys. Acta Phys.Pol.B§ Ann.Nucl.Energy Ann.Phys.(N.Y.) At.Energ. Atomkernenergie Aust.J.Phys. Can.J.Phys. Chin.J.Nucl.Phys. Czech.J.Phys.B Helv.Phys.Acta Hyperfine Interactions Indian J.Pure Appl.Phys. Int,J.Appl.Radiat.lsotop. I z v , A k a d . N a u k SSSR, S e r . F i z . J.Inorg.Nucl.Chem. J.Phys.(London),G J.Phys.Soc.Jpn. J.Phys.(Paris) J.Phys.(Paris),Lett. Lett.Nuovo Cim. Nucl.lnstrum.Methods Nucl.Phys.A Nuel.Sci.Eng. Nuovo Cim.A Phys.Lett.B Phys.Rev.C Phys,Rev.Lett. Phys.Scr. Pisma Zh.Eksp.Teor.Fiz. Progr.Theor.Phys. Progr.Theor.Phys.,Suppl. Radiochem,Radioanal.Lett. Radiochim.Acta Ukr.Fiz.Zh. Yad.Fiz. Z.Phys.A Zh.Eksp.Teor.Fiz.

Volume 52 13 9 143 51 34 35 60 3 32 55 11 20 33 46 43 8 51 43 43 35 201 389 82 70 117 26 49 26 35 68 65 52 30 27 36 308 82

Number 1 2 10 1 6 4 3 10 4 10 1 3 4 10 9 12 10 8 10 20 2 3 3 3 3 2 4 20 3 8 1 1 2 4 6 1 1 6

t978 Recent References (Cumulation) (Nuclear Data S h e e l s , V o l u m e 26, N u m b e r 4); 1979 R e c e n t R e f e r e n c e s ( C u m u l a t i o n ) (Nuclear Data Sheets, Volume 29, N u m b e r 2); 1980 Recent R e f e r e n c e s ( C u m u l a t i o n ) (Nuclear Data Sheets, Volume 31, Number 4); and 1981 Recent References (Cumulation) (Nuclear Data Sheets, Volume 34, N u m b e r 2) p r o v i d e concise c u m u l a t e d coverage for the years specified. These issues together w i t h the 1969-1974, 1975-1977 c u m u l a t i v e issues r e f e r e d to on the p r e v i o u s pages m a y be obtained f r o m the p u b l i s h e r , Academic Press, Inc., 111 F i f t h Avenue, New York, NY 10003. :~ J o u r n a l a b b r e v i a t i o n s are in a g r e e m e n t w i t h those f r o m Chemical A b s t r a c t s for 1979. See also TID-4579-Rg. § One or m o r e issues not y e t received

Recent

References

contains

four

major

sections:

KEY NUMBERS AND KEYWORDS is an index to all experimental papers which contain information about specific nuclei. The index is ordered by increasing atomic number within each A-value. Radioactivity papers are listed under the parent, and the daughter nucleus. Reaction papers are listed under the nucleus for which level properties were determined. Each entry contains a key number (70Ma29,70Pe04) which identifies the article in the REFERENCES section, and a string of keywords which describe the experimental results contained in the article. The reference is also identified by the CODEN d e s c r i p t i o n attached to the end of the keyword string. REACTION INDEX is an index to all experimental papers which contain results from nuclear reactions. The reactions are ordered by increasing A and Z of the incoming and outgoing particle or particles. Within each reaction, the entries are listed according to the Z and A of the target nucleus. Natural targets appear be£ore enriched targets of the same element. Each entry contains an abbreviated string of keywords describing the experiment and a key number which identifies the article in the REFERENCES section. REFERENCES is a bibliography of experimental nuclear reaction and structure articles, ordered by year of publication and last name of the first author. SECONDARY SOURCES is a section containing an index to the non journal literature. Organization is as described a b o v e f o r KEY N U M B E R S AND KEYWORDS, except that no REFERENCES section is given.

Scope References are given only for papers that report experimental data on nuclear reactions and nuclear structure. However, the National Nuclear Data Center does scan and assign keywords to papers dealing with theoretical studies of specific nuclei and nuclear reactions. Computerized searching of the Nuclear Structure References file by specific nuclei and by a selection of specific nuclear properties is available on request to the National Nuclear Data Center.

NUCLEAR

Explanation

SHEETS

DATA

of the K E Y W O R D S

The KEYWORDS are designed to tell a reader what experimental results are reported in an article and what the authors have concluded from those results. The conventions used here are generally the same as those used since 1964 in the journal Nuclear Physics. A few minor changes have been forced by the limitations of the computer printout, A list is given below of several symbols that may cause confusion. This list supplements the table on the inside back cover. The KEYWORDS are given as a 'string' of words and symbols. Each string begins with a 'data category,' NUCLEAR MOMENTS, RADIOACTIVITY, or NUCLEAR REACTIONS. There follows a 'measured' sentence which gives the nucleus (for MOMENTS, RADIOACTIVITY), or reaction (for NUCLEAR REACTIONS) and the physical quantities actually measured. Properties of the nucleus (for MOMENTS), the decay (for RADIOACTIVITY) or the reaction (for REACTIONS) which can be deduced from the experiment are added to this first sentence after a semicolon (;). Additional 'deduced' sentences list other nuclei for which level properties can be deduced and give a description of those properties. A final sentence is sometimes added to give particular details about the experiment. A coded REFERENCE has been added at the end of each KEYWORD string. Journal names are indicated by the ASTM 'CODEN' abbreviations. The abbreviations can be identified by referring to page vi or by occasional checking of the reference list, where all references are given in detail.

EXAMPLES Several

keyword

strings

are

printed

below

along

with

translations

into

'plain

English.'

75Di09 R A D I O A C T I V I T Y 1°aAg(EC),(p+); m e a s u r e d E~/,17,'y~/-eoin,Tz/~; deduced log ft. t°3Pd deduced levels,J,~r. P H S T B 12 80. Through

the electron

capture,

fl+-decay

of l°3Ag p r o p e r t i e s

o f t°aPd l e v e l s w e r e d e d u c e d .

75Di09 N U C L E A R REACTIONS l°aRh(p,n~/),E=6.3-12 MeV; m e a s u r e d o(E,E3,,0), I(ce),-yT-coin,~/(t). 1°aPd deduced levels,Jjr,T~/e,ICC,X. P H S T B 12 80. Through observation over the incident

of the angular particle energy

75Ac01 N U C L E A R M O M E N T S quadrupole moment. Nuclear moments constants.

Symbol a, b, c ABMR B(A) delay DSD E Eg,, Ea, Ep', Et, E{SHe) EC ENDOR EPR, ESR EWSR fragment gK, gR HFB

la1,1aZ,laeCs;m e a s u r e d N U P A B A 2 4 8 157.

o f 131,132,136Cs w e r e

Explanation dipole, quadrupole, octupole hyperfine interaction constants atomic-beam magnetic resonance B{EL) o r B(ML) delayed coincidence, sometimes written as 7 7 ( 0 , ~ 7 ( t ) direct-semidireet model {without subscript) energy of incoming p a r t i c l e i n a n u c l e a r r e a c t i o n (MeV) ~'t, Ea, Ep E t, E(3He) electron capture electron-nucleus double resonance electron paramagnetie, spin resonance energy-weighted sum rule f i s s i o n or h e a v y ion r e a c t i o n f r a g m e n t gK, gR Hartree-Foek-Bogo|iubov

distribution of "),-rays from r a n g e 6 . 3 - 1 2 MeV, p r o p e r t i e s

deduced

from

hfs,a,b; deduced IZ,

measurements

Symbol l(Auger) 17, lfl IB ICC P(n), P ( a )

P(~+) Q, Off RPA S (7 TDA TDHF width X -),-branching

t h e ( p , n T ) r e a c t i o n on l°3Rh o f l°3Pd l e v e l s w e r e d e d u c e d .

of hyperfine

structure

Explanation lea 17, I,~ internal bremsstrahlung internal-conversion coefficient neutron-, a-polarization p r o b a b i l i t y of f l + - d e c a y indicates angular dependence reaction, fl-disintegration energy random-phase approximation s p e c t r o s c o p i c f a c t o r , r e l a t i v e or a b s o l u t e c r o s s s e c t i o n , r e l a t i v e or a b s o l u t e Tamm-Daneoff approximation time-dependent Hartree-Fock p - w i d t h ~ Fp, n - w i d t h z- Fn, 9 ' - w i d t h -= F 7 X - r a y i n X(K) or X T - c o i n ; a n u n s p e c i f i e d reaction p r o d u c t in (a,X), (laC,X) relative ~/-ray branching from a level

NUCLEAR

DATA

SHEETS

.~

o

Z •

o~

m

~ .

~

oC~C~

2; 0

5~ >.<

CC <

0 C~ C~ C~ ~u

Z

.,5 0

L

<

0 .,S

.~

~

-~

~

"~

~ .,4

.~

~

~

~

~

<

~

~

<

~

--~

•

-,S m

~

~

<

•

o

<

~

C

<

~

~

>

~

¢~

C

C

0

"

~"~o

~

~

~

,..~ ~n ,~ --'- o - " - ~

.

.

.

.

.

.

KEY

NUMBERS

AND

A

2H

R 83Ro15: 82Va13:

D

81Lu07

81Si18 82Di01 R

82BelO 82Se03

3He

D

82Di01

J

82Blli

R 82Ca15 83Ja06

R

80Go21

81Ar23 81Gr23 82Bot9

R 80Ma48 80Yall

D

6Li

82A117 R 79Su14

81Bail8

80Zh05 82Ar08 83Bell

=

4

=

5

NUCLEAR REACTIONS ? L i ( d , n ) , E = 1 3 . 3 MeV; 7 L i ( d , 2 a ) , E = 9 - 1 3 . 5 MeV; m e a s u r e d a ( E n ) . 8Be,5He levels deduced neutron branching. YTHLD 2 239. NUCLEAR REACTIONS 7 L i ( d , n ) , E = 4 0 0 , 6 8 0 , 1 0 2 0 keV; measured a(En); deduced reaction m e c h a n i s m . 8Be,SHe l e v e l s d e d u c e d n e u t r o n b r a n c h i n g . C o m p o u n d n u c l e u s f o r m a l i s m . YTHLD 2 137.

A

6He

3

NUCLEAR REACTIONS 4He(e,e'p),E=974,1186 MeV; m e a s u r e d ~ ( 0 ( e ) , e p , E p ) , e p - c o i n . 4He d e d u c e d proton momentum distribution. Coplanar kinematics. DWBA a n a l y s i s , q u a s i e l a s t i c scattering. IANFA 4 4 2655. NUCLEAR REACTIONS 4 H e ( T , n ) , E = t h r e s h o l d - 4 5 MeV; m e a s u r e d G(E). 4He d e d u c e d r e s o n a n c e s , J jr, T. I n t e g r a l e q u a t i o n approach. UFZHA 26 1774. NUCLEAR REACTIONS 2 H ( p o l a r i z e d d , p ) , E = l - 1 3 MeV; m e a s u r e d a(O),vector,tensor a n a l y z i n g p o w e r s . 4He d e d u c e d l e v e l s , J , T r . HPACA 54 649. NUCLEAR REACTIONS 3 H e ( n , p ) , E = 0 . 1 5 - 1 5 0 ke V ; m e a s u r e d ~(E); d e d u c e d d e v i a t i o n s f r o m v -I l a w . 4He r e s o n a n c e deduced parameters. Y A F I A 35 532.

A

5He

=

R A D I O A C T I V I T Y 3H; m e a s u r e d Efl,Ifl; d e d u c e d n e u t r i n o r e s t m a s s l i m i t , f l - d e c a y e n e r g y . H ig h precision measurement. ZETFA 81 1158. R A D I O A C T I V I T Y 3H; m e a s u r e d f l - s p e c t r u m , f l - e n d p o i n t e n e r g i e s ; d e d u c e d a t o m i c e f f e c t s i n 3H, 3He m a s s d i f f e r e n e e , a n t i n e u t r i n o mass. Tritium implantation. P R V D A 23 6 4 9 . R A D I O A C T I V I T Y 3H; m e a s u r e d f l - e n d p o i n t e n e r g y ; d e d u c e d r a d i a t i o n d a m a g e r o l e . aH,3He deduced mass difference. Tritium-implanted S i - L i d e t e c t o r s . PYLBB 108 265. NUCLEAR REACTIONS 3H(e,t),E=77-147 MeV; m e a s u r e d G(Et,Ot). 3H d e d u c e d c h a r g e f o r m f a c t o r , r a d i u s . PRVCA 25 1152. NUCLEAR REACTIONS 9 1 Z r ( p o l a r i z e d d , t ) , E = 5 MeV; 1 4 7 S i n ( p o l a r i z e d d,t ),E=6.5 MeV; m e a s u r e d Ta0(0),Tel(0),Te2(0). 3H d e d u c e d D - s t a t e p a r a m e t e r . E n r i c h e d t a r g e t s . DWBA a n a l y s i s . PRVCA 26 257. R A D I O A C T I V I T Y all; m e a s u r e d f l - e n d p o i n t e n e r g y ; d e d u c e d r a d i a t i o n d a m a g e r o l e . 3H,3He deduced mass difference. Tritium-implanted S i - L i d e t e c t o r s . PYLBB 108 365. NUCLEAR MOMENTS 3He; m e a s u r e d h f s . D o p p l e r f r e e f l u o r e s c e n c e s p e c t r o s c o p y , c w d y e l a s e r s . P L R A A 26 713. NUCLEAR REACTIONS 3 H e ( e , e ) , E = 2 0 0 - 7 0 0 MeV; m e a s u r e d cr(0=155°); d e d u c e d m e s o n e x c h a n g e r o l e . 3He d e d u c e d m a g n e t i c form factor. High accuracy DWBA a n a l y s i s . P RL T A 4 9 986. NUCLEAR REACTIONS 3 H e ( e , e ' p ) , E a t 310 M e V / c ; m e a s u r e d c r ( E ( e ' ) , 0 ( e ' ) , e p ) . 3He d e d u c e d proton momentum distribution. Two-,three-body disintegration,eoplanar geometry,different kinematic conditions. Faddeev,variational calculations. PRLTA 49 9 7 4 .

A

4He

2

NUCLEAR REACTIONS a ° s p b ( d , d ) , E = 3 - 7 MeV; m e a s u r e d ~(0) v s E , d e v i a t i o n s f r o m R u t h e r f o r d scattering. ZH d e d u c e d e l e c t r i c p o l a r i z a b i l i t y . P R LTA 49 909. NUCLEAR REACTIONS I H ( n , 7 ) , E = t h e r m a l ; m e a s u r e d ET; d e d u c e d n e u t r o n , p r o t o n atomic mass difference,Q-values for 1H(n,7),ZH(n,7),laC(n,7),13C(n,7) and 14N(n,7) reactions, aH deduced binding e n e r g y . Gold,48V,144Ce s t a n d a r d s . NUPAB 380 261.

A 3H

=

KEYWORDS

=

6

R A D I O A C T I V I T Y SHe [ f r o m 7Li(TLi,8Be)3; m e a s u r e d T1/a. E n r i c h e d target,tested fitting procedure. NUPAB 372 45. R A D I O A C T I V I T Y 6He [ f r o m 9Be(n,a)3; measured f l - d e e a y TI/ 2. P R V C A 36 253. NUCLEAR REACTIONS 6 L i ( d , 2 d ) , E = 9 MeV; 6 L i ( a , 2 a ) , ( a , 2 d ) , E = 1 8 MeV; m e a s u r e d momemtum s p e c t r a . 6Li d e d u c e d a,d cluster momemtum distribution. PWIA. YTHLD 1 1. NUCLEAR REACTIONS 8,TLi(a,2c~),E=18 MeV; m e a s u r e d c~(0); deduced quasifree scattering e f f e c t . 6,?Li d e d u c e d c l u s t e r probalities. PWIA,on-shell approximation. YTHLD 2 219. NUCLEAR REACTIONS ? L i ( t , d ~ ) , E = 2 . 5 , 5 MeV; m e a s u r e d cr(0d,0~) v s a r e l e n g t h . SLi d e d u c e d level,width,configuration. NCLTA 34 97. NUCLEAR REACTIONS 6 L i ( e , e ' ) , E = 8 0 - 3 0 0 MeV; m e a s u r e d a(E,E(e'),O). 6Li d e d u c e d M1 f o r m factor,ground state current density. Cluster model,exchange currents. P RV CA 25 1156.

KEY

NUMBERS

A SLi

R

82Br09

6Be

R

82Br04

J

81Ru12

R 8OZhO5 81ErlO 82Bu09: 82Gi01: 82La09 82Mo13

82Mo17

7Be

R 82Do02 82Ta03

R 82A108:

aLl aBe

D 82Fi03: R 80Ma48: 80Ya11:

81Be53: 81Do15: 82La09: 8B

R 82As01:

82Do01:

R 81Gu12:

continued

=

7

=

8

NUCLEAR REACTIONS 12C,6Li(6Li,SB),E=72 MeV; '2C,gBe(TLi,aB),E=83 MeV; m e a s u r e d a(E(SB)), a ( 0 ) . 8He d e d u c e d l e v e l , p o s s i b l e J,Tr. YAF1A 35 277. RADIOACTIVITY aLl [ f r o m 7Li(d,p),E=0.772 MeV]; m e a s u r e d f l - d e l a y e d Ea,I~. PRVCA 25 2174. NUCLEAR REACTIONS 7Li(d,n),E=13.2 MeV; 7 L i ( d , 2 ~ ) , E = 9 - 1 3 . 5 MeV; m e a s u r e d a ( E n ) , aBe,SHe levels deduced neutron branching. YTHLD 2 239. NUCLEAR REACTIONS 7 L i ( d , n ) , E : 4 0 0 , 6 8 0 , 1 0 2 0 keV; m e a s u r e d a(En); deduced reaction m e c h a n i s m , aBe,5He levels d e d u c e d n e u t r o n b r a n c h i n g . C o m p o u n d n u c l e u s f o r m a l i s m . YTHLD 2 137. NUCLEAR REACTIONS 9Be(p,d),E=14.3,26.2 MeV; m e a s u r e d G(0,Ed). 8Be r e s o n a n c e s d e d u c e d F,S, L,~-reduced width. Finite-range D W B A , l i n e s h a p e a n a l y s e s . PRVCA 24 2401. NUCLEAR REACTIONS 1 2 C ( d , 6 L i ) , E = 1 2 . 7 , 1 3 . 2 , 1 3 . 6 MeV; ~3C(d,7Li),E=13.6 MeV; m e a s u r e d o ( E ( 6 L i ) ) , a ( E ( T L i ) ) , a ( 0 ) . 8Be d e d u c e d l e v e l . PZETA 34 624. NUCLEAR REACTIONS OBe(d,t~),E=2.5 MeV; m e a s u r e d o(Et,0t,0a); deduced no quasifree e f f e c t s . 7Li,UBe l e v e l s d e d u c e d F , d e c a y m e c h a n i s m . NCLTA 33 433. NUCLEAR REACTIONS 6Li,9Be,J°B(d,Tr-),E-300,600 MeV; m e a s u r e d a(0) v s p i o n m o m e n t u m . SB levels deduced production a(0). S c i n t i l l a t i o n hodoscopes,Cerenkov c o u n t e r s . PYLBB 108 91. NUCLEAR REACTIONS 12,1aC,160(Tr+,p),(Tr+,d),TLi,l°B,laO(Tr+,d),E=32-81 MeV; m e a s u r e d (~(Ep), a(Ed),(~(0), aB,1°,11C,14,160 l e v e l s d e d u c e d L , r e l a t i v e t w o - n u c l e o n pickup strength. High purity Ge d e t e c t o r s . B e t z - K e r m a n m o d e l . PRVCA 25 962.

A

9Be

6

NUCLEAR MOMENTS 7Li; m e a s u r e d m u o n i c X - r a y s , h f s ; d e d u c e d m u o n - n u c l e o n axial vector interaction. HPACA 54 6 4 4 . NUCLEAR REACTIONS 6,TLi(a,2a),E=18 MeV; m e a s u r e d atx(0); d e d u c e d q u a s i f r e e s c a t t e r i n g e f f e c t . 6,7Li d e d u c e d c l u s t e r p r o b a l i t i e s . P W I A , o n - s h e l l a p p r o x i m a t i o n . YTHLD 2 219. NUCLEAR REACTIONS 7Li,12C(p,pd),E=670 MeV; m e a s u r e d a ( E ( m i s s i n g ) , E p ) . 7Li,12C d e d u c e d w a v e function parameters. NUPAB 372 317. NUCLEAR REACTIONS 7 L i ( e , e ' ) , E = 4 0 - 7 4 MeV; m e a s u r e d a(0),transverse f o r m f a c t o r s . 7Li d e d u c e d M1 t r a n s i t i o n w i d t h . PRVCA 26 713. NUCLEAR REACTIONS 7Li(Tr+,Tr+),(Tr+,~r+'),(Tr-,vr-),(Tr-,Tr-'),E=143 MeV; m e a s u r e d cr(0),a(E~). 7Li deduced neutron,proton radii,deformations. E n r i c h e d t a r g e t . NUPAB 377 389. NUCLEAR REACTIONS 9 B e ( d , t a ) , E = 2 . 5 MeV; m e a s u r e d (;(Et,0t,0a); deduced no quasifree e f f e c t s . 7Li,SBe l e v e l s d e d u c e d F , d e c a y m e c h a n i s m . NCLTA 33 433. NUCLEAR REACTIONS S S N i ( p o l a r i z e d 7Li,TLi),E=14.2,18,20.3,22 MeV; m e a s u r e d a(0),Ta0,T21,Ta2 vs 0,spin-independent a n a l y z i n g p o w e r v s 0. 5 a N i ( p o l a r i z e d ~Li,VLi'),E=20.3 MeV; m e a s u r e d a ( O ) , T e o ( O ) , s p i n - d e p e n d e n t a n a l y z i n g p o w e r v s 0. 7Li d e d u c e d s p e c t r o s c o p i c d e f o r m a t i o n . D i f f r a c t i o n , o p t i c a l , D W B A m o d e l s . NUPAB 381 294. NUCLEAR REACTIONS 5 I V ( p o l a r i z e d 6Li,X),(polarized ~Li,X)55Fe/56Fe/SZCr/SaCr/SSMn,(polarized 7Li,TLi),E=10-20 MeV; 5 I V ( p o l a r i z e d 6Li,6Li),E=9.8,12,14 MeV; m e a s u r e d E%I%a(reaction), a ( e l a s t i c ) , t e n s o r a n a l y z i n g p o w e r v s E,0; d e d u c e d p r o d u c t i o n a(E) for residuals,entrance c h a n n e l e f f e c t s . 7Li d e d u c e d s p e c t r o s c o p i c d e f o r m a t i o n . S h a r p c u t o f f m o d e l . ZPAAD 306 335. NUCLEAR REACTIONS 7Li,12C(~r+,rr°),E=70,100,150,165,180 MeV; m e a s u r e d a(0),a(E(Tr°)). 13N,TBe d e d u c e d IAS e x c i t a t i o n d e p e n d e n c e o n p i o n e n e r g y . PRLTA 48 989. NUCLEAR REACTIONS 7Li,la,14C,Z6Mg,aTC1,42Ca(p,n),E=60-200 MeV; m e a s u r e d a ( 0 = 0 ° ) ; d e d u c e d isovector effective interaction strength r a t i o . 7Be,13,14N,26A1,37Ar,42Sc l e v e l s d e d u c e d Gamow-Teller transition s t r e n g t h s . PRVCA 25 1094.

A SHe

=

KEYWORDS

NUCLEAR REACTIONS 2H(tx,tx),E=6-14 MeV; m e a s u r e d a ( E d ) , a d - c o i n , a ( E ) , a ( 0 ) . SLi r e s o n a n c e s deduced F,a,proton,neutron reduced widths. Faddeev formalism,multi-channel,multi-level R-matrix a n a l y s e s . NCIAA 68 35. NUCLEAR REACTIONS 6Li,12C,28Si(n,p),E=60 MeV; m e a s u r e d a(Ep),a(0); deduced effective isovector spin-flip nucleon-nucleon i n t e r a c t i o n . 6Be,~2N,ZaAl l e v e l d e d u c e d G a m o w - T e l l e r transition s t r e n g t h . PRLTA 48 860.

A ~Li

AND

=

9

NUCLEAR REACTIONS l a C ( n , n ) , ( n , n ' ) , ( n , n a ) , E = 1 4 . 7 MeV; m e a s u r e d level

deduced

neutron

emission

probability.

Natural

target.

(7(En,0),integrated PRVCA 24 2458.

or. 9Be

KEY

NUMBERS

A 9B e

R

82Lall

82Pe03

R

81Br28

82Ro04: 82Zu03

lo B

R

81Br28

82Ri04

82Vell

=

9

KEYWORDS

continued

NUCLEAR REACTIONS 9Be(p,da),E=30 MeV; m e a s u r e d a(0d,Ed,0a); d e d u c e d r e a c t i o n m e c h a n i s m . ~Be d e d u c e d ~ - , S H e - c l u s t e r momentum distribution width. Quasifree scattering,DWIA a n a l y s i s . NCIAA 69 1. NUCLEAR REACTIONS 9 B e ( ~ , a ) , ( a , a ' ) , E = 3 5 . 5 MeV; m e a s u r e d ~ ( 0 ) . ~Be l e v e l s d e d u c e d deformation parameters. NUPAB 377 41.

A lOBe

AND

=

10

NUCLEAR REACTIONS I~B(7,p),E=15-31 MeV b r e m s s t r a h l u n g ; m e a s u r e d ~(Ep) v s 0; ~ B ( 7 , n ) , E=15-31 MeV b r e m s s t r a h l u n g ; m e a s u r e d y i e l d s ; d e d u c e d or(total). HB d e d u c e d GDR i s o s p i n s p l i t t i n g , l°Be,l°B d e d u c e d IAS e x c i t a t i o n . FZKAA 13 36. NUCLEAR REACTIONS l°B(%Tr+),(%Tr-),E=lT,19,42 MeV; m e a s u r e d if(0), l°Be,~°C l e v e l d e d u c e d ( r ( r a t i o ) . DWIA a n a l y s i s . PRVCA 25 2652. NUCLEAR REACTIONS l ° B ( e , e ' T r + ) , E = 1 5 8 . 5 - 1 6 5 MeV; m e a s u r e d cr(0(rr),E(?r)); deduced photoproduetion a(0(Tr)), l°Be l e v e l d e d u c e d M1 f o r m f a c t o r c o n v e c t i v e t e r m . PRVCA 26 1610. NUCLEAR REACTIONS llB(%p),E=15-31 MeV b r e m s s t r a h l u n g ; m e a s u r e d a ( E p ) v s 0; 11B(7,n), E=15-31 MeV b r e m s s t r a h l u n g ; m e a s u r e d y i e l d s ; d e d u c e d a ( t o t a i ) , liB d e d u c e d GDR i s o s p i n s p l i t t i n g . ' ° B e , ' ° B d e d u c e d IAS e x c i t a t i o n . FZKAA 13 36. NUCLEAR REACTIONS 9Be(p,7),E=320 keV; m e a s u r e d cr(ET),IT, lab d e d u c e d i s o s c a l a r E2 transition strength upper limit,v-branching r a t i o . N a t u r a l t a r g e t , C e ( L i ) d e t e c t o r . ZPAAD 306 67. NUCLEAR REACTIONS 208Pb(l°B,l°B'),(l°B,gB),(l°B,UB),E=32-38 MeV; m e a s u r e d cr(E(I°B)),tr(E(gB)), cr(E(ltB)),projectile Coulomb excitation, l°B d e d u c e d v i r t u a l GDR e x c i t a t i o n . A U J P A 35 283.

toC

R 82Do0i

82Ro04

NUCLEAR REACTIONS ta,13C,t60(Tr+,p),(rr+,d),TLi,lOB,~80(rr+,d),E=32-81 MeV; m e a s u r e d cr(Ep), g ( E d ) , G ( 0 ) . SB,l°,liC,l~,l~O l e v e l s d e d u c e d L , r e l a t i v e t w o - n u c l e o n pickup strength. High purity Ge d e t e c t o r s . B e t z - K e r m a n m o d e l . PRVCA 25 962. NUCLEAR REACTIONS ~°B(7,Tr+),(7,Tr-),E=17,19,42 MeV; m e a s u r e d ~(0). ~°Be,l°C l e v e l d e d u c e d o r ( r a t i o ) . DWIA a n a l y s i s . PRVCA 25 2652.

A tlBe

D 82Mi08 82Wa18

iI B

D 82Mi08 R 81Br28

82Zw02

JiC

R 82Do01

R 82Be42

la B

R 81Ro15

82De16 la C

J

81Ru13

R 81Erl0

11

R A D I O A C T I V I T Y llBe [ f r o m 9Be(t,p)]; m e a s u r e d E T , I T , T T - c o i n ; d e d u c e d log f t . lib l e v e l s deduced fl-,7-branching,B(X). S h e l l m o d e l . PRVCA 26 1167. RADIOACTIVITY t l B e ( f l - ) [ f r o m 9Be(t,p)]; rrieasured fiT-coin,Doppler shift; deduced flu-asymmetry,meson e x c h a n g e e f f e c t s . S h e l l m o d e l . PRVCA 26 1186. RADIOACTIVITY llBe [ f r o m 9Be(t,p)]; m e a s u r e d E T , 1 7 , 7 7 - c o i n ; d e d u c e d log ft. 11B l e v e l s deduced fl-,7-branching,B(X). S h e l l m o d e l . PRVCA 26 1167. NUCLEAR REACTIONS I t B ( % p ) , E = 1 5 - 3 1 MeV b r e m s s t r a h l u n g ; m e a s u r e d g ( g p ) v s 0; ~lB(7,n), E=15-31 MeV b r e m s s t r a h l u n g ; m e a s u r e d y i e l d s ; d e d u c e d ~ ( t o t a l ) . nB d e d u c e d GDR i s o s p i n s p l i t t i n g , l°Be,l°B d e d u c e d IAS e x c i t a t i o n . FZKAA 13 36. NUCLEAR REACTIONS 9Be(3He,p),E=38 MeV; 9Be(a,d),E=48 MeV; m e a s u r e d o'(E(p),O),o'(E(d)), lib deduced levels,widths,isospin purity,L,normalization f a c t o r s . DWBA a n a l y s i s , s h e l l - m o d e l f o r m f a c t o r s . N a t u r a l t a r g e t s . NUPAB 389 301_ NUCLEAR REACTIONS la,lac,160(rr+,p),(rr+,d),TLi,~°B,laO(rr+,d),E=32-81 MeV; m e a s u r e d cr(Ep), cr(Ed),cr(0). 8B,1°,11C,'4,i60 l e v e l s d e d u c e d L , r e l a t i v e t w o n u c l e o n pickup strength. High purity Ge d e t e c t o r s . B e t z - K e r m a n m o d e l . PRVCA 25 962.

A 1aBe

=

=

12

NUCLEAR REACTIONS 14C(14C,teBe),E 5 0 - 6 3 MeV; m e a s u r e d ~r(0) v s E,a(E(fZBe)); d e d u c e d multi-step p r o c e s s , e n t r a n c e c h a n n e l e f f e c t s , laBe d e d u c e d level. DWBA a n a l y s i s . PYLBB 116 7. NUCLEAR REACTIONS lZC(/x ,u),E a t r e s t ; m e a s u r e d capture r a t i o s , lab l e v e l s d e d u c e d alignment,recoil polarization correction factors. Doppler shape analysis,angular correlation techniques. PYLBB 107 31. NUCLEAR REACTIONS taC(polarized n,p),E=18 MeV; m e a s u r e d d - a s y m m e t r y ; d e d u c e d a n a l y z i n g e f f i c i e n c y , lab d e d u c e d p o l a r i z a t i o n . PRVCA 25 2883. NUCLEAR MOMENTS 12C; m e a s u r e d m u o n i c X - r a y s ; d e d u c e d r m s r a d i u s . C r y s t a l s p e c t r o m e t e r . HPACA 54 6 4 4 . NUCLEAR REACTIONS ?Li,tZC(p,pd),E=670 MeV; m e a s u r e d ~(E(missing),Ep). 7Li?aC d e d u c e d w a v e function parameters. NUPAB 372 317.

KEY

NUMBERS

A ta C

R 81Ey02: 81KhO8: 81Ma38: 82Ca08:

82De02:

82En01: 82Gu03: 82Gu12: 82Ha12: 82In01:

82Mo01:

82Re12: 82We08:

82WrOl: aa N

R

82An08:

82Br04:

82Ta05:

R 82Co08: 82Hi07: 82Ju01: 82Ri05: 82Sa24: 82Se04:

13 N

R

82Do02:

82Do10:

82Sa24:

=

13

KEYWORDS

continued

NUCLEAR REACTIONS 12C(a,a'),E=104 MeV; m e a s u r e d a ( E a ) , a ( 0 ) , laC d e d u c e d n o m o n o p o l e r e s o n a n c e . PRVCA 24 3720. NUCLEAR REACTIONS iac(7,np),E n o t given; m e a s u r e d a ( e ) vs total m o m e n t u m . 1~C d e d u c e d p-shell quasideuteron momentum distribution. YAFIA 34 1425. NUCLEAR REACTIONS leC(T,3(~),leO(7,4a),E=42 MeV b r e m s s t r a h l u n g ; m e a s u r e d a; d e d u c e d reaction mechanism, laC l e v e l s d e d u c e d d e c a y m e c h a n i s m . FZKAA 13 46. NUCLEAR REACTIONS l a C ( p o l a r i z e d p , p ' ) , E = l h 0 MeV; m e a s u r e d p o l a r i z a t i o n , a n a l y z i n g p o w e r difference v s 0. laC l e v e l d e d u c e d t r a n s i t i o n density matrix e l e m e n t s . Q2DM m a g n e t i c spectrometer. PRLTA 49 266. NUCLEAR REACTIONS 2 4 M g ( p , p ' 7 ) , E = 1 4 . 5 - 4 1 . 1 MeV; 32S(p,p'7),E=15.5-40.9 MeV; *aC(p,p'T), E=41.1 MeV; 2 S S i ( p , p ' 7 ) , E = 3 5 . 3 , 4 0 . 9 MeV; m e a s u r e d a(Ep',0p',~T=90°),spin-flip probability v s E,0. a4Mg,3as,2Ssi,iac l e v e l d e d u c e d ,82. D W B A , c o u p l e d - c h a n n e l s a n a l y s e s . PRVCA 25 107. NUCLEAR REACTIONS 12C(p,p'),E=12 MeV; m e a s u r e d ( e + ) ( e - ) - c o i n . iac level d e d u c e d p a i r d e c a y branching ratio. Intermediate image pair spectrometer. PRVCA 25 1047. NUCLEAR REACTIONS i a C ( p , p ' 7 ) , E = 2 4 - 4 4 MeV; m e a s u r e d ET,IT,T(0). laC t r a n s i t i o n s d e d u c e d t e n s o r e f f e c t s . DWBA a n a l y s i s . NCLTA 33 359. NUCLEAR REACTIONS 13C(SHe,a),E=lS-23 MeV; m e a s u r e d ¢(0),a7(0); deduced r e a c t i o n m e c h a n i s m , spin tensor component, iaC l e v e l s d e d u c e d So. DWBA. IANFA 46 897. NUCLEAR REACTIONS nB(p,7),E=0.82-2.83 MeV; m e a s u r e d a(0) v s E,7(0). tac l e v e l s d e d u c e d J, 7 r , t r a n s i t i o n s t r e n g t h s , F T . S h e l l m o d e l . PRVCA 25 1179. NUCLEAR REACTIONS aasr(ieC,IaC),(teC,IaC'),(~aC,13C),E=80 MeV; m e a s u r e d a(0),a(E(laC)), cr(E(13C)): d e d u c e d o p t i c a l m o d e l p a r a m e t e r s , laC l e v e l d e d u c e d s p i n a l i g n m e n t . S?Sr l e v e l s d e d u c e d L , C a S , c o n f i g u r a t i o n s . ZPAAD 305 135. NUCLEAR REACTIONS 12C(~+,~r+'),(Tr-,~r-'),E=100,180,230 MeV; m e a s u r e d a(0,E(~r)), laC l e v e l deduced isobar-hole configuration component. DWlA,Cohen-Kurath transition densities, Fermi momentum c o r r e c t i o n s . PYLBB 108 172. NUCLEAR REACTIONS laC(e,e),E=100-30O MeV; m e a s u r e d a b s o l u t e a(0). laC d e d u c e d r m s r a d i u s , charge distribution. PRVCA 26 806. NUCLEAR REACTIONS ~ B ( p , 7 ) , E = 2 3 - S O MeV; m e a s u r e d ¢(E). U B ( p o l a r i z e d p,7),E=28.7 MeV; measured a(O),A(O). *aC d e d u c e d p o s s i b l e g i a n t r e s o n a n c e s . D i r e c t c a p t u r e c a l c u l a t i o n s . PRVCA 25 2921. NUCLEAR REACTIONS * I B ( p , 7 ) , E = 2 . 9 - 4 . 6 MeV; m e a s u r e d E T , I T , a ( 0 ) v s E. tZC t r a n s i t i o n d e d u c e d M1 q u e n c h i n g . Continuum shell model comparison. PRVCA 25 2823. NUCLEAR REACTIONS *aC,160,a4,aSMg,eeSi,48Ca(p,n),E=62-160 MeV; m e a s u r e d a(O=O°) v s E. 'aN, a4, eSAI,~SF,asp,~SSe l e v e l d e d u c e d a / B ( M t ) s p i n , c u r r e n t contribution dependence~ Inelastic e l e c t r o n s c a t t e r i n g d a t a i n p u t . PRVCA 26 8. NUCLEAR REACTIONS 6 L i , ' a c , a S S i ( n , p ) , E = 6 0 MeV; m e a s u r e d a(Ep),a(0); deduced effective isovector spin-flip nucleon-nucleon i n t e r a c t i o n . ~Be,'2N,aeA1 l e v e l d e d u c e d G a m o w - T e l l e r transition strength. PRLTA 48 860. NUCLEAR REACTIONS iac,i60,a?Al,aeSi,4°Ca,46Ti,9°Zr(3He,t),(aHe,aHe'),E=130,170 MeV; m e a s u r e d a ( E t ) , a ( E ( S H e ) ) , a ( O ) . 160,aTAl,asSi,4°Ca,4°Ti,~°Zr d e d u c e d T=0,GQR. taN,~6F,eTsi,aSP,4°Sc,4Sv, ~°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253.

A ,3 C

AND

=

13

NUCLEAR REACTIONS '3C(p,p),(p,p'),E=135 MeV; m e a s u r e d a(0). 13C l e v e l s d e d u c e d p o s s i b l e configuration. O p t i c a l m o d e l , D W B A a n a l y s e s . NUPAB 380 445. NUCLEAR REACTIONS 13C(e,e),E=80-338 MeV; m e a s u r e d ~(E,0). laC d e d u c e d M1 f o r m f a c t o r . S h e l l m o d e l . PRVCA 26 339. NUCLEAR REACTIONS 2 H , l a C ( n , 7 ) , E = t h e r m a l ; m e a s u r e d E~/,I-y,a. laC t r a n s i t i o n s d e d u c e d I7. PRVCA 25 2810. NUCLEAR REACTIONS iaC(p,p'),E-135 MeV; m e a s u r e d a(0). ~3C s t a t e d e d u c e d t o t a l a n g u l a r momentum transfer,configuration. M i c r o s c o p i c DWBA a n a l y s i s . A U J P A 35 9. NUCLEAR REACTIONS 160(p,pd),(p,pt),E=lO1.3 MeV; * S O ( a , d a ) , ( a , t a ) , ( a , S H e a ) , E = 1 3 9 . 2 MeV; measured a(E1,Ea,0p0a). 14,13N,IsC l e v e l s d e d u c e d L,S. DWIA a n a l y s i s . PRVCA 26 1379. NUCLEAR REACTIONS 13C(~r+,Tr+'),(Tr-,Tr-'),E=162 MeV; m e a s u r e d or(0), t3C l e v e l s d e d u c e d L. M i c r o s c o p i c DWIA a n a l y s i s , s h e l l model wave functions. PRVCA 26 594. NUCLEAR REACTIONS 7Li,lZC(Tr+,TrO),E=70,100,150,165,180 MeV; m e a s u r e d a(0),a(E(Tr°)), iSN,?Be d e d u c e d IAS e x c i t a t i o n d e p e n d e n c e o n p i o n e n e r g y . PRLTA 48 989. NUCLEAR REACTIONS 13C,15N(w+jr%,E=164 MeV; m e a s u r e d ~(0). '3N,150 d e d u c e d IAS e x c i t a t i o n . Enriched targets. Semiphenomenological isobar doorway,second-order coupled-channels c a l c u l a t i o n s . PRVCA 26 189. NUCLEAR REACTIONS ~ S O ( p , p d ) , ( p , p t ) , E = l O l . 3 MeV; l S o ( ~ , d a ) , ( a , t a ) , ( a , 3 H e a ) , E = 1 3 9 . 2 MeV; measured a(EI,Ee,Oi,0a). 14,13N,13C l e v e l s d e d u c e d L,S. DWIA a n a l y s i s . PRVCA 26 1379.

KEY

NUMBERS

A 13 N

R 82Ta03:

R

82Fo01:

82Ne04: 14N

R 81Bi17:

82B108: 82Pe05: 82Sa24: 82Ta03:

82Wa16: 14 0

D 82Wa16: R 82Do01:

R

150

R 82Do10:

82Ju03:

82Vi05:

D 82Ga05:

R 82Ma~5: 82Ne04: 16 0

R 82Ab02:

82A119:

82Am02: 82C101:

continued

=

14

=

15

NUCLEAR REACTIONS 15N(7,n),(7,2n),E=10.8-38 MeV; m e a s u r e d a ( E ) , t e t a l f f ( p h o t o p r o d u c t i o n ) . 15N d e d u c e d r e s o n a n c e s , d e c a y characteristics. PRVCA 26 777. NUCLEAR REACTIONS mC,ihN(Tr+,rr°),E=164 MeV; m e a s u r e d (;(0). 13N,150 d e d u c e d IAS e x c i t a t i o n . Enriched targets. Semiphenomenological isobar doorway,second-order coupled-channels c a l c u l a t i o n s . PRVCA 26 189. NUCLEAR REACTIONS 14C(p,~r-),E=183 MeV; i S O ( p j r - ) , E = t 9 1 MeV; 4e,4eCa,SgY,9°Zr(p,n-),E=206 MeV; m e a s u r e d a(0,E(Tr)),a(0). 150,19Ne,4a,¢OTi,O°Nb,gtMo d e d u c e d h i g h - s p i n state excitation mechanism. PRLTA 49 1314.

A is N

13

NUCLEAR REACTIONS 12C(t,p),E=18 MeV; m e a s u r e d G(0). 14C level deduced w a v e f u n c t i o n . DWBA a n a l y s i s . PRVCA 25 1. NUCLEAR REACTIONS 14N,tSO(n,p),E=60 MeV; m e a s u r e d ~(0). 14c,IsN d e d u c e d GDR a n a l o g e x c i t a t i o n . N a t u r a l t a r g e t s . DWBA a n a l y s i s . NUPAB 385 349. NUCLEAR REACTIONS 13C(p,7),(p,p),E=l.75 MeV; m e a s u r e d a(E,Ep,0). 14N d e d u c e d l e v e l s , J jr,F, FT. E n r i c h e d t a r g e t s , r e s o n a n c e a b s o r p t i o n , r e s o n a n c e fluorescence techniques,transmission a n a l y s i s . PRVCA 24 2 4 4 3 . NUCLEAR REACTIONS 1 4 N ( p , p ' ) , E = 0 . 8 GeV; m e a s u r e d a(0),a(Ep'). 14N l e v e l s deduced deformation l e n g t h s . DWBA a n a l y s i s . PRVCA 25 2550. NUCLEAR REACTIONS 14N(a,a),(a,a'),E=34.85 MeV; m e a s u r e d a ( E a ) , ~ ( 0 ) . 14N l e v e l s d e d u c e d deformation parameter fl,configuration. M i c r o s c o p i c DWBA a n a l y s i s . ZPAAD 305 275. NUCLEAR REACTIONS l e o ( p , p d ) , ( p , p t ) , E = 1 0 1 . 3 MeV; 160(a,da),(a,ta),(c(,aHea),E=139.2 MeV; measured (~(E,,Ea,0p0a). 14,1aN,13C l e v e l s d e d u c e d L,S. DWIA a n a l y s i s . PRVCA 26 1379. NUCLEAR REACTIONS 7Li,la,14c,2sMg,37C1,42Ca(p,n),E=60-200 MeV; m e a s u r e d a(0=O°); d e d u c e d isovector effective interaction strength r a t i o . 7Be,13,14N,Z6AI,37Ar,4ZSc l e v e l s deduced Gamow-Teller transition s t r e n g t h s . PRVCA 25 1094. NUCLEAR REACTIONS mC(aHe,n),E=3.2 MeV; m e a s u r e d ET; deduced f l + - e n d p o i n t energy. 14N level deduced e n e r g y . NUPAB 385 189. R A D I O A C T I V I T Y 140(fl+) [ f r o m laC(3He,n),E=3.2 MeV3; m e a s u r e d ET; deduced f l + - e n d p o i n t energy, f t . NUPAB 385 189. NUCLEAR REACTIONS 1z,laC,160(~+,p),(Tr+,d),VLi,l°B,180(Tr+,d),E=32-81 MeV; m e a s u r e d a(Ep), a ( E d ) , a ( 0 ) . 8B,1°,11C,14,160 l e v e l s d e d u c e d L , r e l a t i v e t w o - n u c l e o n pickup strength. High purity Ge d e t e c t o r s . B e t z - K e r m a n m o d e l . PRVCA 25 962.

A 15N

=

KEYWORDS

NUCLEAR REACTIONS 7Li,la,14C,aSMg,aTCl,aeCa(p,n),E=60-200 MeV; m e a s u r e d q(0=O°); d e d u c e d isovector effective interaction strength r a t i o . 7Be,la,14N,ZeAl,a7Ar,4USc l e v e l s d e d u c e d Gamow-Teller transition s t r e n g t h s . PRVCA 25 1094.

A 14C

AND

=

16

R A D I O A C T I V I T Y 16N [ f r o m aSN(d,p),E=3.4 MeV]; m e a s u r e d E f l , E % I % f l - d e c a y r a t e ; d e d u c e d p s e u d o s c a l a r , a x i a l v e c t o r c o u p l i n g c o n s t a n t r a t i o , p i o n e x c h a n g e c u r r e n t e v i d e n c e . PRLTA 48 914. NUCLEAR REACTIONS ' e c , l S o , S 4 S ( p o l a r i z e d d , a ) , E = 5 2 MeV; m e a s u r e d a(O),iTll(O ). 3ZP,16N d e d u c e d levels,J,Tr. E n r i c h e d t a r g e t s . NUPAB 382 173. NUCLEAR REACTIONS 1 4 N , l S 0 ( n , p ) , E = 6 0 MeV; m e a s u r e d (;(0). 14C,16N d e d u c e d GDR a n a l o g e x c i t a t i o n . N a t u r a l t a r g e t s . DWBA a n a l y s i s . NUPAB 385 349. NUCLEAR REACTIONS 13C(SLi,t),E=24-Z6 MeV; m e a s u r e d a(O,E),a(O),a(Et); l a C ( S L i , t ) , E = 9 - 3 5 MeV; m e a s u r e d a ( f u s i o n , E ) ; SLi(laC,t),E=54.2 MeV; m e a s u r e d G(Et),a(O); d e d u c e d c o m p o u n d n u c l e u s c o n t r i b u t i o n s . 160 l e v e l s d e d u c e d L,S. F i n i t e - r a n g e DWBA a n a l y s i s . NUPAB 377 281. NUCLEAR REACTIONS ahMg(p,7),E=resonance; m e a s u r e d E7,I7; d e d u c e d Q. aSAl d e d u c e d levels, 7-branching u p p e r l i m i t , l a C ( a , n ) , E = 5 . 4 9 8 MeV; m e a s u r e d E7,I7. iSo d e d u c e d t r a n s i t i o n energy. High precision measurements,238pu source,19SAu standard. NUIMA 197 383. NUCLEAR REACTIONS l e C ( a , a ) , ( a , a ' ) , ( a , p ) , E = 1 0 . 5 - 2 0 MeV; m e a s u r e d a ( E a ) , ( ; ( E p ) , o ' ( O ) v s E. 160 l e v e l s d e d u c e d J , T r , F , P a / P , a l p h a c l u s t e r s t r u c t u r e . PRVCA 25 729. NUCLEAR REACTIONS 16,1s0,a4Mg,aSSi,a2S,asAr,4OCa,54Cr,144,152,154Sm,2°spb,2aZTh(polarized d,d), (polarized d , d ' ) , E = 1 8 - E 3 MeV; m e a s u r e d a ( O ) , i T n ( 0 ). 16,1SO,24Mg,28Si,3as,aSAr,4°Ca,54Cr,144, t52,1S4Sm,a°sPb,~a~Th I e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition s t r e n g t h . 154 15a,144Sm,eaaTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082.

KEY

A 16 0

R 8~Do01:

82FrlO: 82Ka12: 82KelO:

822e06: 82Sa19:

82Ta05

82Ve04 t6 F

R 82An08

82Fa06 82Mall 820h03

820r04: 82Ta05:

R 82Fi10:

170

R 82Ku14:

17 F

R 82Se01:

R 8~FilO: 82Na04:

Is N

D 820101:

180

D 820101: R 78Pr10:

16

continued

=

17

NUCLEAR REACTIONS 48Ca(*80,*SC),4SCa(iSo,17C),E=l12 MeV; m e a s u r e d a(E(isC)),cr(E('7C)), lSC, 17C d e d u c e d m a s s e x c e s s e s , l e v e l s . E n r i c h e d t a r g e t . NUPAB 385 505. NUCLEAR REACTIONS Z o S p b ( 1 7 0 , ' 7 0 ' ) , E = 6 6 - 8 8 MeV; m e a s u r e d a(E(l~O)),projectile Coulomb excitation probability, i70 l e v e l d e d u c e d GDR c o n t r i b u t i o n parameter. Modified hydrodynamic m o d e l , a°spb(170,160) ( 1 7 0 , 1 8 0 ) , E = 6 6 - 8 8 MeV; m e a s u r e d a(E(160)),a(E(lS0)). PYLBB 115 437. NUCLEAR REACTIONS * 6 0 ( p o l a r i z e d p , p ) , E = 6 . 4 6 1 - 6 . 4 8 7 MeV; m e a s u r e d a ( E ) , a ( 0 ) , P ( e ) . 17F l e v e l d e d u c e d J j r , F , F p . PRVCA 25 1054.

A 18C

=

NUCLEAR REACTIONS '2,13C,160(~r+,p),(~r+,d),TLi,l°B,tsO(~r+,d),E=32-81 MeV; m e a s u r e d ~(Ep), a ( E d ) , a ( O ) . 6B,10,11C,141160 l e v e l s d e d u c e d L , r e l a t i v e t w o - n u c l e o n pickup strength. High purity Ge d e t e c t o r s . B e t z - K e r m a n m o d e l . PRVCA 25 962. NUCLEAR REACTIONS 'eC(a,(~),E=3.5-3.62 MeV; m e a s u r e d a ( 0 ) v s E. 160 d e d u c e d level,J,~T. R-matrix a n a l y s i s . PRVCA 25 2935. NUCLEAR REACTIONS iTO(polarized 3He,a),E=33 MeV; m e a s u r e d f f ( 0 ) , a n a l y z i n g p o w e r vs 0. 160 levels deduced L,j-transfer,C2S,configurations. DWBA a n a l y s i s . PYLBB 112 433. NUCLEAR REACTIONS 4He(IaC,12C),E=5.6-13.7 MeV; m e a s u r e d if(E,0). 160 r e s o n a n c e d e d u c e d parameters. 4He(laC,?),E(cm)=l.44-3.38 MeV; m e a s u r e d a(E,E(T)),ET,IT; deduced astrophysical S-factor,reaction mechanism. 160 r e s o n a n c e s d e d u c e d F T , a - r e d u e e d widths. ZPAAD 308 73. NUCLEAR REACTIONS 1SN(p,a),E=78-810 keV; m e a s u r e d a(E,0); d e d u c e d a s t r o p h y s i c a l S - f a c t o r . 160 r e s o n a n c e s d e d u c e d F , F p , F a . ZPAAD 305 325. NUCLEAR REACTIONS 's~a4Mg~28Si~46Ar'46'4~4~Ca~46~4~5oTi'~'56Fe'~8'6~62~64Ni'69Y~9~Zr~9e~o~M~' 1 4 4 S m , 2 ° s P b , 2 ° 9 B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d (r(O),A(0); d e d u c e d optical model parameters. 160,a4Mg,26Si,4°A Y,40,44,46Ca,46,46,56Ti,S4,56Fe,58,6°,62,64 Ni,89 Y,9°Zr,96,1°6Mo,l 4 4 S m , 2°6Pb,2°gBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944. NUCLEAR REACTIONS 12C,160,aTAl,asSi,4°Ca,46Ti,9°Zr(3He,t),(3He,3He'),E=130,170 MeV; m e a s u r e d a ( E t ) , f f ( E ( 3 H e ) ) , a ( 0 ) . 160,27Al,assi,4°Ca,46Ti,9°Zr d e d u c e d T=0,GQR. leN,'6F,aTsi,aSP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253. NUCLEAR REACTIONS 1 9 F ( p , a ) , E = 7 . 4 MeV; m e a s u r e d ET,I%aT-coin. 160 l e v e l s d e d u c e d transition strength,7-branching,6. JPHGB 8 743. NUCLEAR REACTIONS 12C,160,24,26Mg,a6Si,46Ca(p,n),E=62-160 MeV; m e a s u r e d a(O=Os) v s E. leN,e4, e6AI,16F,msP,4eSc l e v e l d e d u c e d a / B ( M 1 ) s p i n , c u r r e n t contribution dependence. Inelastic e l e c t r o n s c a t t e r i n g d a t a i n p u t . PRVCA 26 8. NUCLEAR REACTIONS ~ 6 0 ( p , n ) , E = 9 9 . 1 , 1 3 5 2 MeV; m e a s u r e d ( r ( E n ) v s 0; d e d u c e d 6(0). 16F levels deduced J,rr,analog character. Tof. S h e l l m o d e l . PRVCA 25 1760. NUCLEAR REACTIONS 1 6 0 ( p o l a r i z e d p , n ) , E = 1 3 4 MeV; m e a s u r e d a ( 0 ) , a ( E n ) , A ( 0 ) , t6F l e v e l deduced configuration. DWIA,effeetive nucleon-nucleon interaction. PRVCA 25 1715. NUCLEAR REACTIONS 1 6 0 ( p , n ) , E = 3 5 MeV; m e a s u r e d ff(En),a(0); deduced giant multipole resonance virtual e x c i t a t i o n . I6F l e v e l d e d u c e d J,~,T. D W B A , s h e l l m o d e l , o t h e r available d a t a a n a l y z e d . PYLBB 112 206. NUCLEAR REACTI0NS 160(p,n),E=35 MeV; m e a s u r e d a ( E n ) , a ( 0 ) ; d e d u c e d p i o n f i e l d e f f e c t s , isovector transition. ~6F l e v e l s d e d u c e d J j r . DWBA a n a l y s i s . PRLTA 46 1318. NUCLEAR REACTIONS laC,t~O,aTAI,2sSi,4°Ca,~6Ti,9°Zr(~He,t),(aHe,3He'),E=130,170 MeV; m e a s u r e d a ( E t ) , ~ r ( E ( a H e ) ) , a ( 0 ) , t60,aTAl,e6Si,4°Ca,46Ti,g°zr d e d u c e d T=0,GQR. 'eN,16F,eTSi,esp,4OSc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253.

A Iv C

AND KEYWORDS

NUMBERS

=

18

NUCLEAR REACTIONS 4eCa(180,iaC),4SCa('SO,17C),E=l12 MeV; m e a s u r e d a(E('sc)),cr(E(17C)), laC, 17C d e d u c e d m a s s e x c e s s e s , l e v e l s . E n r i c h e d t a r g e t . NUPAB 385 505. NUCLEAR REACTIONS 4SCa(ISO,'sC),E=100 MeV; m e a s u r e d 6(E(18C)),Q. iSC d e d u c e d m a s s . E n r i c h e d t a r g e t . PRVCA 25 1074. RADIOACTIVITY iON; m e a s u r e d ET,IT,Ti/a; d e d u c e d log ft. 180 d e d u c e d l e v e l s , f l - b r a n c h e s . He t r a n s p o r t , G e ( L i ) d e t e c t o r s . S h e l l m o d e l . NUPAB 373 13. RADIOACTIVITY iON; m e a s u r e d ET,I7,Tl/a; d e d u c e d log ft. JSO d e d u c e d l e v e l s , f l - b r a n e h e s . He transport,Ce(Li) d e t e c t o r s . S h e l l m o d e l . NUPAB 373 13. NUCLEAR REACTIONS J g F ( n , a n T ) , ( n , n ' 7 ) , ( n , d T ) , E = 7 , 1 6 - 2 2 MeV; m e a s u r e d a , E 7 . lSO,18,19F deduced transitions. Ge(Li) d e t e c t o r . PIFLD 8 76.

10

KEY

NUMBERS

A 160

R 82Al15

82Ba03

82Ba06 82C101

82Cu01

82G108

82No04 82Re14

~sF

D 82He04: R 78Pr10: 82Ba40: 82Fr15: 82Ko24: 82Mo09:

laNe

D 82He04:

R 82Na08:

190

D 820102:

19p

D 820102: R 78Pr10 82Dill 82Ve05

19No

D 82Ma39 R 82Vi05

D 82De08

18

continued

=

19

NUCLEAR REACTIONS 180(180,tgN),E-100 MeV; 180(ISO,alO),E=92 MeV; m e a s u r e d ff(E(19N)), a ( E ( z I O ) ) , i9N d e d u c e d l e v e l s , m a s s , aid d e d u c e d l e v e l s . JPSLB 43 L - 2 9 . R A D I O A C T I V I T Y 190 [ f r o m lsO(d,p)]; m e a s u r e d EV,Iv; d e d u c e d log ft. 19F l e v e l s d e d u c e d Ifl, v-branching. NUPAB 378 539. RADIOACTIVITY 190 [ f r o m 180(d,p)]; m e a s u r e d EV,IV; d e d u c e d log ft. 19F l e v e l s d e d u c e d ! B, v-branching. NUPAB 378 539. NUCLEAR REACTIONS 1 9 F ( n , 2 n T ) , ( n , n ' 7 ) , ( n , d v ) , E = 7 , 1 6 - 2 2 MeV; m e a s u r e d g , E v . 180,18,19F deduced transitions. Ge(Li) d e t e c t o r . PIFLD 8 76. NUCLEAR REACTIONS JSO(p,p'7),(p,nT),(p,c~7),E=4.4-4.62,4.75-4.83,5-5.66 MeV; m e a s u r e d y i e l d s , G ( E ) , v ( 0 ) . 19F d e d u c e d r e s o n a n c e s , J , w , I A S . NUPAB 385 256. NUCLEAR REACTIONS 19F(a,n),(~,a'),E=5 MeV; m e a s u r e d 7 T - c o i n . tgF d e d u c e d v - b r a n c h i n g u p p e r l i m i t s . 2eNa t r a n s i t i o n deduced branching r a t i o , B ( E 2 ) . JPHGB 8 851. R A D I O A C T I V I T Y 19No [ - f r o m 19F(p,n),E=12 MeV3; n l e a s u r e d NMR; d e d u c e d /~. P o l a r i z e d s o u r c e . PRVCA 26 1753. NUCLEAR REACTIONS 14C(p,~r-),E=183 MeV; lSO(p,~r-),E=191 MeV; 4a,48Ca,SOY,9°Zr(p,~r-),E=206 MeV; m e a s u r e d cr(0,E(Tr)),a(0). 150,19Ne,43,49Ti,g°Nb,91Mo d e d u c e d h i g h s p i n s t a t e e x c i t a t i o n mechanism. PRLTA 49 1314,

A ao F

=

KEYWORDS

NUCLEAR REACTIONS 3He(24Mg,n),E=50 MeV; m e a s u r e d 7V-coin,DSA. 26Si l e v e l s d e d u c e d Tl/e, B ( E 2 ) , n e u t r o n to p r o t o n t r a n s i t i o n m a t r i x e l e m e n t s . 180,a°Mg t r a n s i t i o n s d e d u c e d i s o c a l a r transition strengths,neutron to p r o t o n transition matrix elements. Electromagnetic transition,pion s c a t t e r i n g d a t a i n p u t . PYLBB 113 132. NUCLEAR REACTIONS 180(V,p),(v,d),(V,t),(V,a),E=24,32 MeV b r e m s s t r a h l u n g ; m e a s u r e d (r(Ep), (r(Ed),(r(Et),(7(Ea); d e d u c e d G(Ev,0) f o l l o w i n g t , a e m i s s i o n . 160 d e d u c e d g i a n t r e s o n a n c e decay characteristics. NUPAB 376 15. NUCLEAR REACTIONS 4He(180,a),E=34 MeV; ~H(180,p),E=47 MeV; m e a s u r e d D S A , ( p a r t i c l e ) v - c o i n . leD l e v e l d e d u c e d TI/e,B(E2). NUPAB 377 268. NUCLEAR REACTIONS 16,180,24Mg,28Si,32S,36Ar,4°Ca,54Cr,144,152,154Sm,2°sPb,232Th(polarized d,d), (polarized d , d ' ) , E = 1 8 - 2 3 MeV; m e a s u r e d (7(0),iT11(0). Id,1So,a4Mg,28Si,aZs,seAr,4°Ca,64Cr,t44, la2,tS4Sm,2°sPb,Za2Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition s t r e n g t h , t54 15e,144Sm,232Th d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082. NUCLEAR REACTIONS 14C(dLi,d),E=34 MeV; m e a s u r e d cr(Ed),dc~-coin,da(O),a(O). 180 l e v e l s d e d u c e d J,vr. E x a c t f i n i t e - r a n g e DWBA c a l c u l a t i o n s . PYLBB 112 121. NUCLEAR REACTIONS 1 8 0 ( p o l a r i z e d p,p'),E=800 MeV; m e a s u r e d c r ( 0 ) , a n a l y z i n g p o w e r v s 0; d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 1SO d e d u c e d fle,fl4,Bd. C o u p l e d - c h a n n e l s a n a l y s i s . PYLBB 116 215. NUCLEAR REACTIONS l S O ( e , e ' ) , E = 9 0 - 3 7 0 MeV; m e a s u r e d a ( E ( e ' ) ) , f o r m f a c t o r s . 180 l e v e l s deduced transition eharge densities. Shell model,coexistence m o d e l . PRVCA 25 1778. NUCLEAR REACTIONS 4°Ca(lSO,lsO),(180,160'),(160,170),(lSOJgF),E=62.14 MeV; m e a s u r e d or(O), ~(E(170)),cr(E(19F)). 180,4°Ca t r a n s i t i o n deduced deformation l e n g t h s . 4~Ca l e v e l s d e d u c e d spectroscopic factors. Optical model,DWBA,coupled-ehannels c a l c u l a t i o n s . PRVCA 26 I010. RADIOACTIVITY ~SNe [ f r o m ~60(aHe,n)]; m e a s u r e d EV,Iv f o l l o w i n g B - d e c a y ; d e d u c e d f t , p a r i t y nonconserving force parameter, laF l e v e l s d e d u c e d a b s o l u t e Ifl. PRVCA 25 2957. NUCLEAR REACTIONS igF(n,2nv),(n,n'v),(n,dv),E=7,16-22 MeV; m e a s u r e d cr,Ev. 1~0,16,19p deduced transitions. Ge(Li) d e t e c t o r . PIFLD 8 76. NUCLEAR REACTIONS 3He(160,p),E=19.4 MeV; m e a s u r e d D S A , p v - c o i n . lSF l e v e l s d e d u c e d Tl/a. NUPAB 386 333. NUCLEAR REACTIONS 6Li(160,a),E=24 MeV; m e a s u r e d E v , 1 7 , a V - c o i n , a v ( 0 ) . lSF d e d u c e d level,T, T~/a,J,rr. E n r i c h e d t a r g e t s . NUPAB 385 516. NUCLEAR REACTIONS laC(nB,n~),E=33 MeV; m e a s u r e d E%I%DSA,recoil. ~SF level d e d u c e d TI/~, B(E2). Ge(Li) d e t e c t o r . PRVCA 26 1750. NUCLEAR REACTIONS 3He(~O,p),E=15,18,£1 MeV; m e a s u r e d DSA. ~dF level d e d u c e d Tl/2,cascade f e e d i n g e f f e c t . NCLTA 33 407. RADIOACTIVITY ~SNe [ f r o m lsO(3He,n)]; m e a s u r e d E%I7 f o l l o w i n g B - d e c a y ; d e d u c e d f t , p a r i t y nonconserving force parameter. 18F l e v e l s d e d u c e d a b s o l u t e Ifl. PRVCA 25 2957.

A ~9N

AND

=

[ f r o m ~7AI, 19F, 37CI, S7Rb(d,p),E=l 6.5 MeV]; m e a s u r e d Eft, energies,Qfl. H y p e r p u r e Ge d e t e c t o r , o n - l i n e s e p a r a t i o n . NUIMA 192 261,

RADIOACTIVITY 28AI,Z°F,38Cl,SSRb flV-coin,fl e n d p o i n t

20

11

KEY

NUMBERS

A a0Ne

R 81Bu27: 81Ga35: 81Ta23: 82Ev01:

82Sp02: ZONa

J

82To05:

R 82Na08:

~Ne

D 81Mc14: R 81An31:

ZlNa

J

82To05:

D 82Mu08:

ZZNe

R 82G107: 82Ta15:

aaNa

J

82To05:

R 83Go11:

82Ve05: 2aMg

D 82Ca16:

ZZA1

D 82Ca16:

R 83Goll

83Is01 82MaZ0

continued

=

21

=

22

RADIOACTIVITY ZZO,ZSNe,ZT,ZSNa,Z%a°Mg,al,aZA1 l - f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 GeV]; m e a s u r e d f l - d e c a y Ti/z. PRLTA 49 455. NUCLEAR REACTIONS ZeNa(n,p),E=0.02-1000 eV; m e a s u r e d a(E). ZZNe d e d u c e d r e s o n a n c e , P n , F p . Tof. ZPAAD 308 57. NUCLEAR REACTIONS 180(%i,d),E=72 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . ZZNe l e v e l s d e d u c e d Sa. DWBA a n a l y s i s . PRVCA g6 524. NUCLEAR MOMENTS 2°,al,az,z4,31Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). 2o,21,22,e4, 31Na d e d u c e d /~. 21Na,25,a6,zT,zs,29Na measured hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756. NUCLEAR REACTIONS z i , Z a N e ( p , y ) , E = 7 0 - 3 5 5 k e V ; m e a s u r e d a(Ey,E),ET,Iy(E,0); deduced astrophysical reaction r a t e . ZZNa d e d u c e d resonances,Fw,J,rr,resonance strengths, aaNa deduced resonance strength u p p e r l i m i t s . E n r i c h e d gas t a r g e t s , G e ( L i ) d e t e c t o r s . NUPAB 385 57. NUCLEAR REACTIONS 19F(a,n),((x,a'),E=5 MeV; m e a s u r e d 7 T - c o i n . 19F d e d u c e d 7 - b r a n c h i n g u p p e r l i m i t s . ZZNa t r a n s i t i o n deduced branching r a t i o , B ( E Z ) . JPHGB 8 851. RADIOACTIVITY ZaAl(fl+),(p) [ f r o m a4Mg(aHe,4np),E=110 MeV]; m e a s u r e d f l - d e l a y e d Ep,lp,T1/z. aaMg l e v e l d e d u c e d m a s s e x c e s s , l f i . PRVCA 26 1778. RADIOACTIVITY ZZAl(fl+),(p) [ f r o m Z4Mg(3He,4np),E=110 MeV]; m e a s u r e d f i - d e l a y e d Ep,Ip,T1/z. aZMg l e v e l d e d u c e d m a s s e x c e s s , I f l . PRVCA 26 1778.

A Z3Na

20

NUCLEAR REACTIONS i80(180,19N),E=100 MeV; 180(180,alO),E=92 MeV; m e a s u r e d cr(E(lUN)), cr(E(210)). 19N d e d u c e d l e v e l s , m a s s , alO d e d u c e d l e v e l s . JPSLB 43 L - E g . RADIOACTIVITY ZlNe [ f r o m 180(a,n),E=4.48,4.85,4.95 MeV]; m e a s u r e d p a i r e m i s s i o n r e l a t i v e b r a n c h i n g r a t i o s , alNe t r a n s i t i o n deduced ~/-multipolarity,6 l o w e r l i m i t . PRLTA 47 1720. NUCLEAR REACTIONS IeC(IuC,a~/),E=19.7 MeV; m e a s u r e d a~/-coin,DSA. ZlNe d e d u c e d levels J,Tr,T~/ 2. N a t u r a l t a r g e t s . NUPAB 372 281. NUCLEAR MOMENTS a°,al,a~,24,alNa; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). 20ziaz,a4, 31Na d e d u c e d /~. ~lNa,ZS,zs,a~,za,agNa m e a s u r e d hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756.

A z2 0

=

KEYWORDS

NUCLEAR REACTIONS ~°O(a,a),E=3.5-4.9 MeV; m e a s u r e d or(0), a°Ne d e d u c e d b r o a d r e s o n a n c e s , rotational band,cluster structure. Phase shift,optical m o d e l a n a l y s e s . HPACA 54 439. NUCLEAR REACTIONS ~60((x,c~'),E=9.52-9.8 MeV; taC(~aC,a),E=30 MeV; m e a s u r e d a(E(a),O(a~)), F ( a i ) / F . ZONe d e d u c e d l e v e l J , r r , ( x - p a r t i c l e b r a n c h i n g r a t i o s , P ( a 0 ) , F ( a i ) . NUPAB 372 194. NUCLEAR REACTIONS ~O,zsSi(%i,d),E=75 MeV; m e a s u r e d a(0). a°Ne,aaS levels d e d u c e d r e l a t i v e Sa. DWBA a n a l y s i s . PRVCA 24 2556. NUCLEAR REACTIONS ~4N(a,(x)(a,-/),E ~ 1517.5-1535 keV; m e a s u r e d o'(0,E),ct(E-~). ~60(a,-/), E=3.020,3.036 MeV; m e a s u r e d E-~,I% a°Ne d e d u c e d E2 t r a n s i t i o n strength. Differentially pumped transmission gas t a r g e t . NUIMA 192 143. NUCLEAR REACTIONS ~ZC(~zC,a),E=32.6,33.5 MeV; m e a s u r e d a(ET,0),7(0,B),DSA. ZONe l e v e l d e d u c e d g,T~/z. NUPAB 378 130. NUCLEAR MOMENTS z°,z~,z~,z4,~Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). ~o,z~,zz,a4, ~ N a d e d u c e d /~. Z~Na,~5,z~,aT,aS,~Na m e a s u r e d hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756.

A e, 0

AND

=

23

NUCLEAR REACTIONS a l , Z Z N e ( p , 7 ) , E = 7 0 - 3 5 5 k e V ; m e a s u r e d (r(ET,E),ET,I~/(E,O); d e d u c e d astrophysical reaction r a t e . ZaNa d e d u c e d resonances,FT,J,rr,resonance strengths, a3Na deduced resonance strength u p p e r l i m i t s . E n r i c h e d gas t a r g e t s , G e ( L i ) d e t e c t o r s . NUPAB 385 57. NUCLEAR REACTIONS Z a N a ( 7 , 7 ) , ( - y , n ) , ( 7 , p ) , ( 7 , 7 ' ) , E = 7 1 4 , 1 6 - 3 1 MeV; m e a s u r e d a(E) for reactions,nuclear R a m a n e f f e c t . 23Na d e d u c e d g i a n t r e s o n a n c e c o n f i g u r a t i o n . YAFIA 35 3. NUCLEAR REACTIONS l Z C ( n B , X ) , E = 1 4 - 5 4 MeV; IZC(lIB,UB),E=25,40,50 MeV; 13C(I°B,X),E=14-48 MeV; 13C(l°B,l°B),E=18,25,32,39,46 MeV; m e a s u r e d •(fragment 0,E) f o r A = 9 - 2 3 ; d e d u c e d q ( f u s i o n ) v s E. ZaNa d e d u c e d L ( c r i t i c a l ) v s e x c i t a t i o n . O p t i c a l m o d e l , M o n t e C a r l o , H a u s e r F e s h b a c h c a l c u l a t i o n s . PRVCA 25 2963.

12

KEY

NUMBERS

A a4Na

D 80Joll

J

a4Mg

82To05

R 81Ho30

81SzO7

81TrO8 82BIOl

82C101

82Da16

82De02:

82Ka17:

82Me05:

AND

=

KEYWORDS

24

R A D I O A C T I V I T Y 38K(IT) [ f r o m Z4Mg(lSO,np),E=38 MeV]; 24Na(IT) [ f r o m aaNa(d,p),E=4 MeV]; 77Se(IT) [ f r o m 7 4 G e ( ~ , n ) , E = 1 6 M e V ] ; 71Ge(EC) [ f r o m 7°Ge(d,p),E=6 M e V ] ; 73As(EC),~TAs(fl-) [from 72,76Ge(d,n),E=6,7 Me V ]; m e a s u r e d T1/2. O n - l i n e c o m p u t e r i z e d d i g i t i z e r . NUIMA 178 581. NUCLEAR MOMENTS a°,2',2z,z4,31Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). 20,2~,zz,24, alNa d e d u c e d iz. alNa,aS,as,aT,aS,aSNa m e a s u r e d hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756. NUCLEAR REACTIONS I a C ( 1 2 C , S B e ) , ' a C ( I a C , ( ~ ) , E ( c m ) = 2 2 - 2 8 MeV; l ° B ( 1 4 N , I a C ) , E ( e m ) = 6 - 1 0 MeV; l ° B ( 1 4 N , ( ~ ) , ( 1 4 N , S B e ) , E ( c m ) = 8 - 1 7 . 5 MeV; m e a s u r e d cr(0,E), a4Mg d e d u c e d m o l e c u l a r resonance exit channel dependence. FZKAA 13 17. NUCLEAR REACTIONS 1 8 C ( 1 8 0 , a ) , E = 4 8 . 8 , 5 4 . 2 , 5 8 . 6 , 5 5 , 6 5 MeV; m e a s u r e d ~(O),cr(Ea); d e d u c e d broad structures,angular momentum matching, a4Mg d e d u c e d selective yrast cluster population. FZKAA 13 29. NUCLEAR REACTIONS a 3 N a ( p , p ' v ) , ( p , a T ) , ( p , ~ ) , E = 5 0 0 - 1 7 0 0 k e V ; m e a s u r e d G(E). a4Mg d e d u c e d resonances,F. T h i n t a r g e t s . JRACB 67 135. NUCLEAR REACTIONS e 4 , a ° M g ( p , p ) , ( p , p ' ) , E = 0 . 8 GeV; m e a s u r e d ~r(0). 24,26Mg d e d u c e d deformation lengths,multipole moments. Optical model,DWBA,coupled-ehannets analyses, rotational m o d e l . PRVCA 25 422. NUCLEAR REACTIONS 10,180,a4Mg,20Si,3aS,36Ar,4°Ca,54Cr,14%lsa,154Sm,2°°Pb,232Th(polarized d,d), (polarized d,d'),E=18-23 MeV; m e a s u r e d a ( 0 ) , i T n ( O ). 10,100,a4Mg,aSSi,3ZS,aSAr,4°Ca,54Cr, 144, lsz,154Sm,Z°sPb,232Th l e v e l s d e d u c e d i s o s e a l a r q u a d r u p o l e , o c t u p o l e transition strength. ~54 152,144Sm,23aTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PR LTA 48 1082. NUCLEAR REACTIONS laC(laC,X),E=4.2-7 MeV; 13C(IZC,X),E=3.1-6.7 MeV; m e a s u r e d ~ ( f u s i o n ) v s E. ~4Mg d e d u c e d resonance. NaI,surface barrier detectors,natural,enriched targets. O p t i c a l m o d e l a n a l y s i s . NUPAB 3 8 4 257. NUCLEAR REACTIONS a 4 M g ( p , p ' T ) , E = 1 4 . 5 - 4 1 . 1 MeV; 3 2 S ( p , p ' T ) , E = 1 5 . 5 - 4 0 . 9 MeV; l a C ( p , p ' T ) , E=41.1 MeV; Z S S i ( p , p ' T ) , E = 3 5 . 3 , 4 0 . 9 MeV; m e a s u r e d ~(Ep',0p',~T=908),spin-flip probability v s E,0. Z4Mg,3aS,asSi,laC l e v e l d e d u c e d fla. D W B A , c o u p l e d - c h a n n e l s a n a l y s e s . PRVCA 35 i0 7 . NUCLEAR REACTIONS 12C(12C,a),E=29.5-30.5 MeV; m e a s u r e d a(0),a(E); deduced nonstatistical contributions. 24ME d e d u c e d r e s o n a n c e , c h a n n e l correlation effects. Hauser-Feshbach model. NUPAB 383 530. NUCLEAR REACTIONS 1 2 C ( l a C , ' a C ) , ( l a C , l a C ' ) , E ( c m ) = 2 5 . 2 MeV; measured (IaC)(laC)-, ( 1 2 C ) ( l a C ) T - c o i n . 24ME r e s o n a n c e s deduced T-decay upper limit,characteristics. PRVCA 25

1486. 82Sa19:

82St11:

82Va16 82ZwOl 24A1

D 82Ra05 R 82An08

820r01

• 89 NUCLEAR REACTIONS 1 6 O, 24 ME, 28 Sl,' 40 A t , 40 , 44 , 48 Ca, 46 , 48 , 5 0 TI,' 5 4 ,5 8 Fe . 5 8 . 00 . . 62 82~N1, Y, 90 Zr, 98 , 100 Mo, 144Sm,a°ePb,a°SBi(polarized p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(0); d e d u c e d optical model parameters. 16O,24 ME,28 Sl,- 40 A r , 40 , 44 , 48 Ca, 46 , 48 , 50 T1,• 54 , 56 Fe . 58. 00 - 89 Y, - 90 Zr, 88 , 100 Mo, 144 S i n , . . 62 64 N1,

a°sPb,a°9Bi deduced point nucleon distribution. PRVCA 26 9 4 4 . NUCLEAR REACTIONS 1 2 C ( 1 0 0 , a ) , E = 9 4 - 1 5 0 MeV; m e a s u r e d cr(Ea) v s E; d e d u c e d reaction mechanism. 24Mg d e d u c e d narrow,closely spaced levels. Kinematic analysis,inclusive reactions. P R L T A 49 640. NUCLEAR REACTIONS N a ( p , a ) , ( p , p ' ) , E = 6 . 2 7 , 6 . 3 7 , 6 . 5 2 MeV; m e a s u r e d a ( 0 ) . a4Mg r e s o n a n c e s d e d u c e d J,Tv. S t a t i s t i c a l m o d e l . IA N F A 46 940. NUCLEAR REACTIONS a4Mg,4aCa(a,pot),(ct,2ot),E=120 MeV; m e a s u r e d ap(O),ota(O),(7(Ea),a(O=O°)/ a ( 0 = l S 0 ° ) , a4Mg,4°Ca d e d u c e d g i a n t r e s o n a n c e decay characteristics. P R V C A 25 2139. R A D I O A C T I V I T Y a4,a4mAl [ f r o m 24Mg(p,n)3; m e a s u r e d ET,Iv; d e d u c e d log f t , G a m o w - T e l l e r matrix elements. Shell model calculations. NUPAB 378 29. , , NUCLEAR REACTIONS 12C,160,24,26Mg,28Si,48Ca(p,n),E=62-160 MeV; measured o'(0=O°) vs E. laNa~ 20AI,~°F,aSP,48Sc level deduced cr/B(Ml) s p i n , c u r r e n t c o n t r i b u t i o n dependence. Inelastic electron scattering data i n p u t . PRVCA 26 8. NUCLEAR REACTIONS 2~Mg(p,n),E=35 MeV; m e a s u r e d c~(En),c~(6), a4Al deduced level,J,Tr,T, s t r e t c h e d p a r t i c l e - h o l e c o n f i g u r a t i o n , m u l t i p o l e character. Tof. DWBA analysis. PRLTA 48 469.

A

aSNe

D

ZSNa

D 82A127: J

82Mu08:

82To05:

=

35

RADIOACTIVITY 2ao,ZSNe,aT,aSNa,aV,3°Mg,31,32Al [ f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 GeV~; m e a s u r e d fl-decay TI/2. PRLTA 49 455. R A D I O A C T I V I T Y 25Na(fl-),29AI(fl-),25AI(fl+) [froin 23Na,aTAl(t,p),24Mg(d,n)]; measured ET,IT; deduced log f t , I f l . 25Mg,29Si d e d u c e d - / - b r a n c h i n g . NUPAB 385 4 7 4 . NUCLEAR MOMENTS a°,21,22,24,31Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). 20,21,22,24 31Na deduced }z. 21Na,25,zs,aT,as,ZSNa m e a s u r e d byperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756.

13

KEY

A 25Mg

D 82A127: J

81Je02: 82We04:

R 83Hu03:

25AI

D 82A137: R 82Pr03:

J

82To05:

26Mg

R 82Al15:

82Be32:

83BI01:

82Hu02: 83Sp05: 26A1

R 81Ko38: 82Al19:

82An01:

82An08:

82De15:

83Ke08:

83Pa02:

83Ta03:

aSSi

R 82A115:

82Bo14:

=

25

continued

RADIOACTIVITY 25Na(fl-),29Al(fl-),aSAl(fl+) [ f r o m 23Na,aTAl(t,p),a4Mg(d,n)]; m e a s u r e d E3,,I7; d e d u c e d log ft,lfl. ZSMg,29Si d e d u c e d T - b r a n c h i n g . NUPAB 385 474. NUCLEAR MOMENTS 25Mg,aTAl; m e a s u r e d h f s , m u o n i c X - r a y s ; d e d u c e d s p e c t r o s c o p i c q u a d r u p o l e moments. HPACA 54 321. NUCLEAR MOMENTS 25Mg,aTAl; m e a s u r e d m u o n i c X - r a y s , h f s ; d e d u c e d e l e c t r i c f i e l d g r a d i e n t , S t e r n h e i m e r f a c t o r . 25Mg,aTA1 d e d u c e d s p e c t r o s c o p i c q u a d r u p o l e m o m e n t . N u c l e a r r o t a t i o n a l model,strong-coupling l i m i t . NUPAB 377 361. NUCLEAR REACTIONS z4,25,26Mg(n,v),E=thermal; m e a s u r e d EV. z5,2°,aTMg d e d u c e d l e v e l s , n e u t r o n b i n d i n g e n e r g y . NUIMA 192 609. RADIOACTIVITY 25Na(fl-),ZgAl(fl-),a5Al(fl+) C f r o m 23Na,27Al(t,p),a4Mg(d,n)]; m e a s u r e d E7,I7; d e d u c e d log ft,Ifl. 25Mg,29Si d e d u c e d T - b r a n c h i n g . NUPAB 385 474. NUCLEAR REACTIONS 2 4 M g ( p o l a r i z e d p , p ) , E = 3 . 8 9 - 4 . 1 7 MeV; m e a s u r e d a(E,0),P(E,0). 25A1 d e d u c e d r e s o n a n c e , J , T r , P , F p . E n r i c h e d t a r g e t . P h a s e s h i f t a n a l y s i s . PRVCA 26 254.

A a6Na

AND K E Y W 0 R D S

NUMBERS

=

26

NUCLEAR MOMENTS 2°,al,z~,a4,31Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). a0,31,32,34, 31Na d e d u c e d p . 21Na,25,2°,27,28,2~Na measured hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756. NUCLEAR REACTIONS 3He(24Mg,n),E=50 MeV; m e a s u r e d "y3'-coin,DSA. 26Si l e v e l s d e d u c e d Tl/2, B ( E 2 ) , n e u t r o n to p r o t o n t r a n s i t i o n m a t r i x e l e m e n t s . 180,aeMg t r a n s i t i o n s d e d u c e d i s o c a l a r transition strengths,neutron to p r o t o n transition matrix elements. Electromagnetic transition,pion s c a t t e r i n g d a t a i n p u t . PYLBB 113 132. NUCLEAR REACTIONS a 4 S , 4 a C a ( p o l a r i z e d p,p'),E=650 MeV; 3 ° S t ( p o l a r i z e d p,p'),E=650,800 MeV; measured a ( 0 ) . 26Mg,3°Si,42Ca,34S d e d u c e d neutron,proton transition matrix element r e l a t i v e s i g n . PRLTA 49 451. NUCLEAR REACTIONS 2 4 , 2 8 M g ( p , p ) , ( p , p ' ) , E = 0 . 8 GeV; m e a s u r e d a ( 0 ) . z4,eSMg d e d u c e d deformation lengths,multipole moments. Optical model,DWBA,coupled-channels analyses, rotational m o d e l . PRVCA 25 422. NUCLEAR REACTIONS 24,25,aeMg(n,7),E=thermal; m e a s u r e d EV. as,26,27Mg d e d u c e d l e v e l s , n e u t r o n b i n d i n g e n e r g y . NU1MA 192 609. NUCLEAR REACTIONS 2°ePb(aSMg,aSMg'),E=80-120 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n . 26Mg level deduced quadrupole m o m e n t , B ( E 2 ) . E n r i c h e d t a r g e t . NUPAB 378 559. NUCLEAR REACTIONS 25Mg(p,v),E=l.716 MeV; m e a s u r e d V(0). 26AI d e d u c e d r e s o n a n c e decay,FV,6, B ( X ) , J j r . IANFA 45 2157. NUCLEAR REACTIONS 25Mg(p,7),E=resonance; m e a s u r e d EV,I3'; d e d u c e d Q. 26A1 d e d u c e d levels, 7-branching u p p e r l i m i t . 13C((x,n),E=5.498 MeV; m e a s u r e d E7,I3,. 160 d e d u c e d t r a n s i t i o n energy. High precision measurements,a38Pu source,198Au standard. NUIMA 197 383. NUCLEAR REACTIONS 25Mg(p,3,),E=600-1730 k e V ; m e a s u r e d a ( E ) . aSA1 d e d u c e d r e s o n a n c e strengths,thermonuclear reaction rates. Statistical-model analysis. Enriched target. NUPAB 373 326. NUCLEAR REACTIONS 12C,160,24,ZSMg,28Si,48Ca(p,n),E=62-160 MeV; m e a s u r e d ~(O=O°) vs E. 12N,24, 26Al,~SF,28P,48Sc l e v e l d e d u c e d cr/B(M1) s p i n , c u r r e n t contribution dependence. Inelastic e l e c t r o n s c a t t e r i n g d a t a i n p u t . PRVCA 36 8. NUCLEAR REACTIONS 25Mg(p,-/),E=774,880 k e V ; m e a s u r e d E v , 1 3 ' , D o p p l e r s h i f t s . 26Al l e v e l deduced Tl/a,7-branching,transition strength,v-multipolarity,isospin character. Mirror d e c a y s d i s c u s s e d . PYLBB 113 137. NUCLEAR REACTIONS a5Mg(p,v),E=I.2 MeV; m e a s u r e d g(E,ET,0),DSA. ZSAl levels d e d u c e d 7 - r a y branching ratios,Tl/2,E2 transition strengths. Implanted,enriched 25Mg t a r g e t s . NUPAB 385 461. NUCLEAR REACTIONS la,12C(170,170),(170,a),E=30-57 MeV; 13C( I7 O, 13C), 12C( 17O, 12C ) , E = 3 0 - 5 7 MeV; 13 C( 16 O, 18 0 ) , ( 16 O, 13 C),( 16 0 , a ) , E = 2 9 . 5 - 5 3 . 6 MeV; I ° B ( 1 6 0 , 1 6 0 ) , ( 1 6 0 , I O B ) , ( 1 6 0 , a ) , E = 4 3 . 4 - 6 0 . 1 MeV; m e a s u r e d (~(E); d e d u c e d r e a c t i o n m e c h a n i s m . 26A1,29,30Si d e d u c e d h i g h - s p i n n o n r e s o n a n t structures. Hauser-Feshbach a n a l y s i s . PRVCA 25 313. NUCLEAR REACTIONS 7 Li, 13 , 1 4 C, 2 6 Mg, 3 7 CI, 4 2 C a ( p , n ) , E = 6 0 - 2 0 0 MeV; m e a s u r e d ~(0=0°); d e d u c e d isovector effective interaction strength r a t i o . ?Be,13,14N,26A1,37Ar,4aSc l e v e l s d e d u c e d Gamow-Teller transition s t r e n g t h s . PRVCA 25 1094. NUCLEAR REACTIONS 3He(a4Mg,n),E=50 MeV; m e a s u r e d 7 7 - c o i n , D S A . 26Si l e v e l s d e d u c e d TI/a, B ( E S ) , n e u t r o n to p r o t o n t r a n s i t i o n m a t r i x e l e m e n t s . 180,26Mg t r a n s i t i o n s d e d u c e d i s o c a l a r transition strengths,neutron to p r o t o n transition matrix elements. Electromagnetic transition,pion s c a t t e r i n g d a t a i n p u t . PYLBB 113 132. NUCLEAR REACTIONS a4,aeMg,2eSi(aHe,n),E=13 MeV; m e a s u r e d cr(En,0), ze,aSSi,a°S d e d u c e d levels,L,J,~r. E n r i c h e d t a r g e t s . NUPAB 378 525.

14

KEY

NUMBERS

A aTNa

D

82Mu08:

J

82To05:

27Mg

R

83Hu02:

Z7A1

J

81Je02: 82Ba30: 82Bu18: 82We04:

R 82Anll: 83Di13:

82E104 82Ry02 82Sm04 82Ta05

27Si

R 82Ta05

D

82Mu08

J

82To05

aSMg

R

81Be64

aSAI

D 82De08 82Sc14 R 82Br04

82Sc14 82U101 aSSi

D 82Se14 82Wa05 R 81Erl2 81Ga33

=

KEYWORDS

37

R A D I O A C T I V I T Y a20,aSNe,27,28Na,a9,3°Mg,31,32A1 [ f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 GeV]; m e a s u r e d f l - d e c a y Tl/2. PRLTA 49 455. NUCLEAR MOMENTS 2o,21,a2,a4,3~Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). 20,2122,24, 31Na d e d u c e d tz. a~Na,2S,26,aT,28,agNa m e a s u r e d hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756. NUCLEAR REACTIONS 24,25,26Mg(n,7),E=thermal; m e a s u r e d ET. as,26,aTMg d e d u c e d l e v e l s , n e u t r o n b i n d i n g e n e r g y . NUIMA 192 609. NUCLEAR MOMENTS 2SMg,aTA1; m e a s u r e d h f s , m u o n i c X - r a y s ; d e d u c e d s p e c t r o s c o p i c q u a d r u p o l e moments. HPACA 54 321. NUCLEAR MOMENTS aTA1; m e a s u r e d NMR; d e d u c e d h y p e r f i n e i n t e r a c t i o n s . P a r a m a g n e t i e DyA12, G d A l a s a m p l e s . PLRAA 25 6616. NUCLEAR MOMENTS 27A1; m e a s u r e d NMR vs T; deduced n u c l e a r q u a d r u p o l e tensor. Single YAIO3 c r y s t a l . PYLAA 91 465. NUCLEAR MOMENTS 25Mg,aTA1; m e a s u r e d m u o n i c X - r a y s , h f s ; d e d u c e d e l e c t r i c field g r a d i e n t , Sternheimer f a c t o r . 25Mg,aTA1 d e d u c e d s p e c t r o s c o p i c q u a d r u p o l e m o m e n t . N u c l e a r r o t a t i o n a l model,strong-coupling l i m i t . NUPAB 377 361. NUCLEAR REACTIONS 2 6 M g ( p , 7 ) , E = l . 4 - 2 . 2 MeV; m e a s u r e d ET,DSA. aTA1 l e v e l s d e d u c e d Tl/2. Ge(Li) d e t e c t o r , e n r i c h e d , i m p l a n t e d t a r g e t s . NUPAB 385 194. NUCLEAR REACTIONS ~3C(14N,X),E=86,103.8,149,161.3,180 MeV; m e a s u r e d o r ( f r a g m e n t 0,E) f o r f r a g m e n t Z=5-12; d e d u c e d a ( f u s i o n ) , c r ( d i r e c t ) , c r ( r e a c t i o n ) , aTA1 d e d u c e d m a x i m u m J limit. PRVCA 26 1490. NUCLEAR REACTIONS 2 7 A l ( n , n ' 7 ) , E = f a s t ; m e a s u r e d ET,I%DSA. aTA1 l e v e l s d e d u c e d TI/a,B(X),& JPHGB 8 997. NUCLEAR REACTIONS a7Al(e,p),E=16.8-25.6 MeV; m e a s u r e d atE,0); d e d u c e d cr(7,p) v s 0. 27A1 d e d u c e d GDR c o n f i g u r a t i o n s , E 3 decay characteristics. NUPAB 389 29. NUCLEAR REACTIONS 26Mg(p,7),E=0.29-2.2 MeV; m e a s u r e d a(E,E(7)),E~,IT(0),DSA. 27A1 l e v e l s deduced resonance strengths,7-branching,T~/~,J,~,~. E n r i c h e d t a r g e t s . NUPAB 377 15. NUCLEAR REACTIONS 12C,160,aTAl,asSi,4°Ca,46Ti,9°Zr(3He,t),(3He,aHe'),E=130,170 MeV; m e a s u r e d a ( E t ) , a ( E ( 3 H e ) ) , c r ( 0 ) . 160,a~Al,asSi,4°Ca,4~Ti,9°Zr d e d u c e d T=0,GQR. ~ZN,16F,avSi,aSP,4°Sc,4~V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253. NUCLEAR REACTIONS ~aC,~60,aTAl,~sSi,4°Ca,46Ti,9°Zr(3He,t),(aHe,aHe'),E=130,170 MeV; m e a s u r e d a ( E t ) , ~ ( E ( a H e ) ) , a ( 0 ) . 160,27Al,asSi,4°Ca,46Ti,g°Zr d e d u c e d T=0,GQR. ~aN,~°F,aTSi,eSP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 35 1253.

A 28Na

AND

=

28

RADIOACTIVITY 220,aSNe,a7,28Na,29,3°Mg,31,32A1 [ f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 GeV]; m e a s u r e d f l - d e c a y Tl/2. PRLTA 49 455. NUCLEAR MOMENTS 2°,21,a2,a4,alNa; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). a0,al,aa,24, 31Na d e d u c e d ~. 21Na,aS,as,27,28,29Na measured hyperfine constants; deduced spectroscopic quadrupole moment. PRVCA 25 2756. NUCLEAR REACTIONS 14 C( 14 C, 14 C'),( 14 C , x n ) , ( 14 C , x n a ) , E ( c m ) = 1 2 . 5 - 3 2 . 5 MeV; m e a s u r e d c~(E), production a t E ) f o r a5Mg,aaNe,Ne,lSc; d e d u c e d c h a n n e l c o r r e l a t e d s t r u c t u r e , aSMg d e d u c e d possible quasimolecular r e s o n a n c e s . FZKAA 13 37. R A D I O A C T I V I T Y 2SAI,a°F,aeCI,aaRb [ f r o m aTAl,19F,a7Cl,STRb(d,p),E=l-6.5 MeV3; m e a s u r e d Eft, flT-coin,fl-endpoint energies,Qfl. H y p e r p u r e Ge d e t e c t o r , o n - l i n e s e p a r a t i o n . NUIMA 192 261. RADIOACTIVITY aSA1 [ f r o m 2 T A l ( n , 7 ) , E = t h e r m a l ] ; m e a s u r e d E7,I7 f o l l o w i n g f l - d e c a y , aSSi deduced transition energy. Crystal spectrometer,Ge(Li) d e t e c t o r . PRVCA 25 2888. NUCLEAR REACTIONS SLi,lZC,asSi(n,p),E=60 MeV; m e a s u r e d cr(Ep),ff(0); d e d u c e d e f f e c t i v e isovector spin-flip nucleon-nucleon i n t e r a c t i o n . 6Be,laN,aaA1 l e v e l d e d u c e d G a m o w - T e l l e r transition strength. PRLTA 48 860. NUCLEAR REACTIONS 2 7 A l ( n , 7 ) , E = t h e r m a l ; m e a s u r e d E7,17. aSA1 d e d u c e d l e v e l s , J , ~ r , n e u t r o n binding energy. Cyrstal spectrometer,Ge(Li) d e t e c t o r . PRVCA 25 3888. NUCLEAR REACTIONS aaSi(n,p),E=59.6 MeV; m e a s u r e d a(O). 28A1 d e d u c e d p a r e n t a n a l o g g i a n t d i p o l e r e s o n a n c e s t r e n g t h . N a t u r a l t a r g e t . NUPAB 386 179. R A D I O A C T I V I T Y 28A1 [ f r o m 2 7 A l ( n , 7 ) , E = t h e r m a l ] ; m e a s u r e d E7,I7 f o l l o w i n g f l - d e c a y . 28Si deduced transition energy. Crystal spectrometer,Ge(Li) d e t e c t o r . PRVCA 25 2888. R A D I O A C T I V I T Y asp; m e a s u r e d E7,t7; d e d u c e d log ft. aSSi d e d u c e d l e v e l s , 7 b r a n c h i n g , I f l . NUPAB 378 397. NUCLEAR REACTIONS 27Al(p,a),E=632,885,937,1002 keV; m e a s u r e d Ea. aSSi levels d e d u c e d Tl/a. Crystal blocking technique. IANFA 45 1886. NUCLEAR REACTIONS 160(160,160),160(160,a),E(cm)=15.5-17 MeV; m e a s u r e d ~(0) v s E; d e d u c e d resonant,background S matrix e l e m e n t s . 28Si d e d u c e d r e s o n a n c e s , J j r . PRLTA 47 1878.

]5

KEY

NUMBERS

A

~eSi

R 81G105:

81Ta34: 81Vo09: 82Bo14: 82Bo35: 82C101:

82CsOl:

82De02:

82Dj03: 82Fr04: 82KaO4: 82NaO2: 8~Sal9:

83Ta05:

82Wi04: asp

D 82We05: R 82An08:

82Ta05:

e8 S

R 82Mo12:

J

ZSMg

D 82Mu08:

ZSAI

D 82A127:

ZSSi

D 82A127:

82To05:

R 80Jal8:

=

~8

KEYWORDS

continued

NUCLEAR REACTIONS aSMg(a,nT),E=14,15.5 MeV; m e a s u r e d n T - c o i n , n T ( O ) , D S A . 27AI(p,7),E=2.16, 2.312 M e V ; m e a s u r e d ET,IT,DSA. 28Si d e d u c e d levels,J,zr,rotational bands,T~/e,B(),),6,Pp,F , intrinsic quadrupole moments. S h e l l m o d e l . Z P A A D 303 239. NUCLEAR REACTIONS l Z C ( 1 6 0 , l e C ) , E ( c m ) = l S . 2 - 1 3 . 5 MeV; m e a s u r e d a ( 0 ) v s E , a ( E ( ' e C ) ) . ZOSi resonance deduced J,rr,F,a-cluster structure. PYLBB 107 35. NUCLEAR REACTIONS ZTAl(p,a),E=1365,1439,1647 keV; m e a s u r e d G(0a). ZSSi r e s o n a n c e s d e d u c e d Tl/e. C r y s t a l b l o c k i n g t e c h n i q u e . A N P Y A 38 298. NUCLEAR REACTIONS 24,eSMg,eeSi(ZHe,n),E=13 MeV; m e a s u r e d a(En,O), es,ZSSi,3°S d e d u c e d levels,L,J,rr. Enriched t a r g e t s . N U P A B 378 525. NUCLEAR REACTIONS 6°Ni(eSSi,zSSi),(aeSi,eSSi'),E= 140 MeV; m e a s u r e d a(O). ZSSi,69Ni l e v e l s deduced sequential,simultaneous excitation. Coupled-channels method. PYLBB 114 423. NUCLEAR REACTIONS 18,'SO,Z4Mg,zSSi,3eS,3SAr,4°Ca,54Cr,144,tsa,154Sm,SOSpb,Z3ZTh(polarized d,d), (polarized d,d'),E=lS-23 MeV; m e a s u r e d a ( 0 ) , i T u ( 0 ). 16,~80,a4Mg,ZSSi,3ZS,38Ar,4OCa,54Cr,144, 15e,154Sm,e°sPb,Z32Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition strength. ,54 152,144Sm,Z3eTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . P R L T A 48 1082. NUCLEAR REACTIONS e 4 M g ( a , a ) , E = 2 . 6 - 4 . 9 MeV; m e a s u r e d G(E,0). e 4 M g ( a , 7 ) , E = 3 . 7 - 5 . 1 MeV; measured a(E),a(ET,O). ZSSi d e d u c e d r e s o n a n c e s , F , F a , J , T r , 7 - b r a n c h i n g , r e s o n a n c e strength,F-/, d. E n r i c h e d targets. R-matrix a n a l y s i s . N U P A B 385 43. NUCLEAR REACTIONS Z 4 M g ( p , p ' 7 ) , E = 1 4 . 5 - 4 1 . 1 MeV; a a S ( p , p ' 7 ) , E = 1 5 . 5 - 4 0 . 9 MeV; l Z C ( p , p ' 7 ) , E=41.1 MeV; Z S S i ( p , p ' 7 ) , E = 3 5 . 3 , 4 0 . 9 MeV; m e a s u r e d a(Ep',Op',~7=90°),spin-flip p r o b a b i l i t y v s E,0. e4Mg,3aS,a~Si,~ZC l e v e l d e d u c e d fie. D W B A , c o u p l e d - c h a n n e l s a n a l y s e s . PRVCA 25 107. NUCLEAR REACTIONS eTAl,esSi(3He,d),E=130 MeV; m e a s u r e d a(O),a(Ed); d e d u c e d o p t i c a l m o d e l parameters, eeSi,zgP l e v e l d e d u c e d s p e c t r o s c o p i c strength. P R V C A 26 797. NUCLEAR REACTIONS IeC(~80,X),E(cm)=IE-EO MeV; m e a s u r e d (r(fragment 0,E,mass); deduced (r(fusion) vs fragment m a s s , E . ZSSi d e d u c e d r e s o n a n c e s . P R V C A 25 860. NUCLEAR REACTIONS S i ( p , p ' ) , e S S i ( p , p ' ) , E = l l 5 MeV; m e a s u r e d (r(O). ZSSi l e v e l s d e d u c e d isospin,transition rates,EWSR strengths. DWBA a n a l y s i s . P R V C A 25 1263. NUCLEAR REACTIONS ZTAl(ZHe,d),E=35 MeV; m e a s u r e d ~r(Ed,O). ZSSi d e d u c e d levels,L,rr,T, spectroscopic f a c t o r s . DWBA a n a l y s i s . N U P A B 376 61. NUCLEAR REACTIONS 1 6 ~ 4 M g ~ e e S i ~ 4 ~ A r ~ 4 ~ 4 4 ~ 4 8 C a ~ 4 6 ~ 4 ~ 5 ~ T i ~ 5 4 ~ 5 s F e ~ 5 ~ 6 e ~ N i ~ 8 9 Y ~ 9 ~ Z r ~ 9 ~ M ~ 144Sm,a°8Pb,e°gBi(polarized p , p ) , E = 6 5 MeV; m e a s u r e d a(O),A(O); d e d u c e d optical model parameters. 160,~4Mg,aSsi,4°A r,4°,44,48Ca,46,48,5°Ti,54,56Fe,Se,6°,sz,64 N i , e S y , 9 ° Z r , 9 ~ , l ° ° M o , 1 4 4 S m , Z°sPb,Z°SBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . P R V C A 26 9 4 4 . NUCLEAR REACTIONS laC,'~O,ZTAl,ZeSi,4OCa,46Ti,9°Zr(3He,t),(aHe,3He'),E=130,170 MeV; m e a s u r e d a(Et),a(E(3He)),a(0), t~o,a7Al,Z8Si,4°Ca,46Ti,9°Zr deduced T=0,GQR. taN,16F,oTSi,ZsP,4°Sc,4~V, 9°Nb d e d u c e d IAS o f T = I , G D R . P R V C A 25 1253. NUCLEAR REACTIONS ~ZC(lsO,160),E=45.5-49 MeV; m e a s u r e d a(0),G(E). ZSSi d e d u c e d r e s o n a n c e , F , Pp/F,J,Tr. S-matrix a n a l y s i s . PYLBB 113 141. R A D I O A C T I V I T Y eSp; m e a s u r e d E7,I7; d e d u c e d log f t . eeSi d e d u c e d l e v e l s , 7 - b r a n c h i n g , l ft. N U P A B 378 397. NUCLEAR REACTIONS 'aC,lsO,e4,Z°Mg,eSSi,48Ca(p,n),E=62-160 MeV; m e a s u r e d ~r(O=O°) v s E. ~eN,z4, ZSAI,~F,esP,*SSc l e v e l d e d u c e d a/B(M1) spin,current contribution dependence. Inelastic electron scattering d a t a i n p u t . P R V C A 26 8. NUCLEAR REACTIONS ~eC,lsO,e7Al,ZsSi,4°Ca,4STi,S°Zr(ZHe,t),(3He,aHe'),E=130,170 MeV; m e a s u r e d G(Et),a(E(ZHe)),G(0). tSO,a7Al,esSi,4°Ca,4~Ti,99Zr d e d u c e d T=0,GQR. 'ZN,16F,ZTsi,Z8P,4°Sc,46V, 9°Nb d e d u c e d IAS o f T = I , G D R . P R V C A 25 1253. NUCLEAR REACTIONS ~60,ZSSi,4OCa(~r+,Tr-),E=164 MeV; m e a s u r e d a(E(zr-)) a t O=5°; d e d u c e d m a s s dependence of a,isobar components i n w a v e f u n c t i o n . ZSS,49Ti d e d u c e d m a s s e x c e s s . PRVCA 25 3218.

A egNa

AND

=

29

NUCLEAR MOMENTS a°,21,as,z4,3~Na; m e a s u r e d i s o t o p e s h i f t s , h y p e r f i n e c o n s t a n t (A). zo,al,as,a4, 31Na d e d u c e d /z. alNa,aS,es,o7,zs,29Na m e a s u r e d hyperfine constants; deduced spectroscopic quadrupole moment. P R V C A 25 2756. R A D I O A C T I V I T Y aSO,Z5Ne,aT,SeNa,SS,3°Mg,31,32Al [ f r o m 9 B e ( 4 ° A r , X ) , E = I I . 4 GeV3; m e a s u r e d f l - d e c a y T t / z . P R L T A 4 9 455. R A D I O A C T I V I T Y SSNa(fl-),ZSAl(fl-),aSAl(fl +) [ f r o m a3Na,a7Al(t,p),a4Mg(d,n)3; measured E7,I7; d e d u c e d log f t , I f l , a5Mg,ZSSi d e d u c e d * / - b r a n c h i n g . N U P A B 385 4 7 4 . R A D I O A C T I V I T Y S5Na(fl-),SSAl(fl-),Z5Al(fl +) [ f r o m ZaNa,eTAl(t,p),S4Mg(d,n)]; measured E7,I7; d e d u c e d log f t , I f l . 25Mg,zSSi d e d u c e d " y - b r a n c h i n g . N U P A B 385 4 7 4 . NUCLEAR REACTIONS Z e S i ( d , p ) , ( d , n ) , E = l l MeV; m e a s u r e d a(0p,0n,En),a(0n,0p,Ep),(r(0p,0n). ZSsi,eSP d e d u c e d r e s o n a n c e s , J , r r , F . DWBA a n a l y s i s , s t r i p p i n g to unbound s t a t e s . APOBB 11 641.

16

KEY

NUMBERS

A agsi

R

82Pa02:

~9p

R

80Ja18:

82A128: 82Dj03: 82Ma04

D 82Mu08

3Osi

R 82A122 82Ba49

82Be32

820d01

82Pa02

82Sa15 82Yo02 3op

R 80Li21 81Sh26 82A122 82De29

82Ta04

3o S

R 82A122 82Bo14

8EYo02

J

82To05

29

continued

=

30

RADIOACTIVITY aZo,aSNe,27,SSNa,ag,3°Mg,al,32A1 F f r o m 9 E e ( 4 ° A r , X ) , E = l l . 4 GeV]; m e a s u r e d f l - d e c a y T1/2. PRLTA 49 455. NUCLEAR REACTIONS 3He(SSSi,n),E=60 MeV; m e a s u r e d DSA. a% levels d e d u c e d Ti/~. 3°Si,3°p,3°S d e d u c e d E2 t r a n s i t i o n strength v s T ( z ) , m a s s . PRLTA 49 438. NUCLEAR REACTIONS 12C(180,X),(180,180'),(180,160),(180,170),(180,14C),(ls0,15N),(180,13C),(180, a),(~SO,2a),(180,5n),(ls0,5np),(lSO,5n2p),(~80,n2a),E=50-81 MeV; m e a s u r e d E~,I~/; d e d u c e d a(E),channel correlation e f f e c t s . 3°Si d e d u c e d s t r u c t u r e in fusion evaporation,binary c h a n n e l . PRVCA 26 1774. NUCLEAR REACTIONS 34S,4aCa(polarized p,p'),E=650 MeV; 3 ° S i ( p o l a r i z e d p,p'),E=650,800 MeV; measured a t 0 ) . ZSMg,a°Si,4aCa,34S d e d u c e d neutron,proton transition matrix element r e l a t i v e s i g n . PRLTA 49 451. NUCLEAR REACTIONS a ° S i ( % x n ) , E ~ 1 0 - 2 8 MeV b r e m s s t r a h l u n g ; m e a s u r e d n e u t r o n yield; d e d u c e d a t E ) . 3°Si d e d u c e d GDR f r a g m e n t a t i o n . NUPAB 388 445. NUCLEAR REACTIONS 1a,12C(170,170),(170,a),E=30-57 MeV; i3C(170,13C)}zC(170,leC),E=30-57 MeV; 13C(lsO,iS0),(JSO,13C),(ieo,a),E=29.5-52.6 MeV; l°B(Iso,leo),(lSO,t°B),(iSO,a),E=42.4-60.1 MeV; m e a s u r e d atE); d e d u c e d r e a c t i o n m e c h a n i s m . 26A1,29,3°Si d e d u c e d h i g h - s p i n n o n r e s o n a n t structures. Hauser-Feshbach a n a l y s i s . PRVCA 25 313. NUCLEAR REACTIONS 3°Si(a,a'),E=120 MeV; m e a s u r e d or(0). 3°Si level d e d u c e d n e u t r o n , p r o t o n matrix element r e l a t i v e s i g n . DWBA a n a l y s i s . PYLBB 114 419. NUCLEAR REACTIONS 2SSi(3He,np),E=9.5 MeV; m e a s u r e d a(E(n),E(p),0). 3% d e d u c e d IAS,L,J,Tr. 3°Si,3°S d e d u c e d C o u l o m b d i s p l a c e m e n t e n e r g i e s . NUPAB 383 298. NUCLEAR REACTIONS a S S i ( d , p ) , E = l - 2 . 5 MeV; m e a s u r e d (r(0,Ep,E). 3Op d e d u c e d i n t e r m e d i a t e r e s o n a n c e s , J , T r . YTHLD 2 316. NUCLEAR REACTIONS 27Al(aHe,p),E < 14.5 MeV; m e a s u r e d s t e p ) . 3Op d e d u c e d c o h e r e n c e e n e r g y . Multi-step compound emission,autocorrelation a n a l y s i s . I J P Y A 55 434. NUCLEAR REACTIONS 3He(ZSSi,n),E=60 MeV; m e a s u r e d DSA. 3% levels d e d u c e d T1/2. 3°Si,3°p,3°S d e d u c e d E2 t r a n s i t i o n strength v s T ( z ) , m a s s . PRLTA 49 438. NUCLEAR REACTIONS aSS,eeSi(a,d),E=50 MeV; 3 a S ( d , a ) , E = 4 0 MeV; m e a s u r e d cr(0). 3°P,34C1 deduced levels,L,S,J,~r. Natural targets. Microscopic,macroscopic DWBA c a l c u l a t i o n s . NUPAB 386 200. NUCLEAR REACTIONS aZS,3S,3SAr(polarized d,a),E=16 MeV; m e a s u r e d a(0),iTH(0),Tso(0),Tzs(0); deduced j-transfer d e p e n d e n c e . 3°p,34,3SC1 l e v e l s d e d u c e d L , j - t r a n s f e r . Enriched targets. DWBA a n a l y s i s . NUPAB 377 1. NUCLEAR REACTIONS 3He(ZSSi,n),E=60 MeV; m e a s u r e d DSA. 3% levels d e d u c e d T1/2. 3°Si,3°p,3°S d e d u c e d E2 t r a n s i t i o n strength v s T ( z ) , m a s s . PRLTA 49 438. NUCLEAR REACTIONS 24,26Mg,aSSi(3He,n),E=13 MeV; m e a s u r e d a(En,0). 2s,aeSi,3°S d e d u c e d levels,L,J,~r. E n r i c h e d t a r g e t s . NUPAB 378 525. NUCLEAR REACTIONS 28Si(3He,np),E=9.5 MeV; m e a s u r e d a(E(n),E(p),0). 3% d e d u c e d IAS,L,J,~r. 39Si,3°S d e d u c e d C o u l o m b d i s p l a c e m e n t e n e r g i e s . NUPAB 383 298.

A

alNa

=

KEYWORDS

NUCLEAR REACTIONS ~3,tZC('vO,l~0),(~70,a),E=30-57 MeV; 13C(170,13C),Iac(170,I2C),E=30-57 MeV; 13C(lsO,*60),(~SO,13C),(160,a),E=29.5-52.6 MeV; * ° E ( ~ 6 0 , ~ e o ) , ( ~ 6 0 , ~ O B ) , ( ~ O , a ) , E = 4 ~ . 4 - 6 0 . 1 MeV; m e a s u r e d a(E); d e d u c e d r e a c t i o n m e c h a n i s m . ZSAl,Zg,3°Si d e d u c e d h i g h - s p i n n o n r e s o n a n t structures. Hauser-Feshbach a n a l y s i s . PRVCA 25 313. NUCLEAR REACTIONS Z S S i ( d , p ) , ( d , n ) , E = l l MeV; m e a s u r e d cr(Op,On,En),c;(On,Op,Ep),c~(Op,On). agSi,zgP d e d u c e d r e s o n a n c e s , J , ~ , F . DWBA a n a l y s i s , s t r i p p i n g to u n b o u n d s t a t e s . APOBB 11 641. NUCLEAR REACTIONS 2VAl,egsi(aHe,n),E=15 MeV; m e a s u r e d ff(0),a(En). ~9P,3~S levels d e d u c e d L, enhancement f a c t o r s . DWBA a n a l y s i s , s h e l l m o d e l . PRVCA 26 789. NUCLEAR REACTIONS 27Al,asSi(3He,d),E=130 MeV; m e a s u r e d
A

3°Mg

AND

-

31

NUCLEAR MOMENTS a°,a1,ea,a4,31Na; m e a s u r e d isotope s h i f t s , h y p e r f i n e c o n s t a n t (A). a0,al,zs,a4, 31Na d e d u c e d /x. ZINa,aS,SS,27,as,29Na m e a s u r e d h y p e r f i n e c o n s t a n t s ; d e d u c e d s p e c t r o s c o p i c q u a d r u p o l e m o m e n t . PRVCA 25 2756.

17

KEY

NUMBERS

A 3~A1

D 82Mu08:

31p

R 82Ba45

82Ch09 82Ho06 31s

D 82AyO1 R 82A128

31CI

D 82Ay01

D 82Mu08

32Si

R 82Fo02

3ap

R 82Ma25

3a S

J

82Ei01

R 81A126

81Po16: 81Ta23: 82C101:

82De02:

82E106: 82Go13: 82Ve09:

D 81Dua0: R 82Ju02:

33C1

D 81Du20:

J

82El01:

continued

=

32

=

33

RADIOACTIVITY 33C1; m e a s u r e d E-/,I-/; d e d u c e d log f t . 33S l e v e l d e d u c e d f l - b r a n c h i n g . N i l s s o n m o d e l . JOPQA 42 1603. NUCLEAR REACTIONS 3 e S ( n , n ) , ( n , X ) , E - 0 . 1 8 - 2 MeV; m e a s u r e d a ( t o t a l ) , a ( 0 ) v s E. 33S d e d u c e d resonances,Tr,Fn,resonance parameters. N a t u r a l t a r g e t . NUPAB 386 287. RADIOACTIVITY 33C1; m e a s u r e d E-/,IT; d e d u c e d log f t . 33S l e v e l d e d u c e d f l - b r a n c h i n g . N i l s s o n m o d e l . JOPQA 42 1603.

A 34 S

31

RADIOACTIVITY ZaO,aSNe,eT,aSNa,a9,a°Mg,al,32A1 [ f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 GeV3; m e a s u r e d f l - d e c a y T~/2. PRLTA 49 455. NUCLEAR REACTIONS 3 ° S i ( t , p ) , E = 1 5 MeV; m e a s u r e d a ( E p , 0 ) . 32Si d e d u c e d levels,J,Tr, configuration. M i c r o s c o p i c DWBA a n a l y s i s . PRVCA 25 5. NUCLEAR REACTIONS l a C , 1 8 0 , a 4 S ( p o l a r i z e d d,(x),E=52 MeV; m e a s u r e d a(0),iT11(0). 3aP,16N d e d u c e d levels,J,Tr. E n r i c h e d t a r g e t s . NUPAB 382 173. NUCLEAR MOMENTS 34,3aS,35,37Cl,36,4°Ar; m e a s u r e d i s o t o p e s h i f t s ; d e d u c e d s t r o n g s p e c i f i c mass effect,electron momentum correlation. Collinear laser spectroscopy,Ar,S,C1 ion b e a m s . ZPAAD 305 39. NUCLEAR REACTIONS laC(asSi,3(x),(IeC,SBe),E=68-80 MeV; m e a s u r e d a a - c o i n ; d e d u c e d r e a c t i o n dependent structure. 36Ar d e d u c e d structures near yrast l i n e . 3aS d e d u c e d strong population of h i g h l y i n g l e v e l s . FZKAA 13 43. NUCLEAR REACTIONS 160(160,a),E ~ 2 0 - 4 5 MeV; m e a s u r e d a(0,E). 3aS d e d u c e d i n t e r m e d i a t e structure. Correlation,deviation function a n a l y s i s . FZKAA 13 35. NUCLEAR REACTIONS J60,aSSi(6Li,d),E=75 MeV; m e a s u r e d a(0). a°Ne,3ZS l e v e l s d e d u c e d r e l a t i v e S~. DWBA a n a l y s i s . PRVCA 24 2556. NUCLEAR REACTIONS 16,180,a4Mg,a8Si,3aS,a6Ar,4°Ca,54Cr,144,15a,154Sm,a°sPb,a3aTh(polarized d,d), (polarized d , d ' ) , E = 1 8 - 2 3 MeV; m e a s u r e d q ( 0 ) , i T l l ( 0 ) . 16,180,a4Mg,aSSi,32S,36Ar,4°Ca,a4Cr,144, 15a,154Sm,288pb,a3aTh l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition s t r e n g t h . 154 ~sa,144Sm,a3aTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082. NUCLEAR REACTIONS a 4 M g ( p , p ' 7 ) , E = 1 4 . 5 - 4 1 . 1 MeV; 3 a S ( p , p ' - / ) , E = 1 5 . 5 - 4 0 . 9 MeV; laC(p,p'-/), E-41.1 MeV; a S S i ( p , p ' - / ) , E = 3 5 . 3 , 4 0 . 9 MeV; m e a s u r e d ~(Ep',0p',~-/=90°),spin-flip probability v s E,0. a4Mg,3aS,asSi,l~C l e v e l d e d u c e d fla. D W B A , c o u p l e d - c h a n n e l s a n a l y s e s . PRVCA 25 107. NUCLEAR REACTIONS 3aS(n,n'v),E-fast; m e a s u r e d DSA. 3aS level d e d u c e d Tl/2. NUIMA 201 377. NUCLEAR REACTIONS 3ZS(p,p'),E=7.5 MeV; m e a s u r e d p - / - c o i n , p - / ( 0 ) , E - / , I T . 3aS t r a n s i t i o n s d e d u c e d 6. JPHGB 8 1391. NUCLEAR REACTIONS a o S p b ( 3 u S , 3 a S ' ) , E = 1 2 2 - 1 6 0 MeV; m e a s u r e d Coulomb excitation p r o b a b i l i t i e s . 3aS l e v e l d e d u c e d q u a d r u p o l e m o m e n t , B ( E a ) . E n r i c h e d t a r g e t . NUPAB 389 185.

A 33 S

=

KEYW0RDS

RADIOACTIVITY aaO,a5Ne,aT,aeNa,ag,3°Mg,31,3aA1 [ - f r o m 9 B e ( 4 ° A r , X ) , E = l l . 4 G e V ] ; m e a s u r e d p-decay T1/a. PRLTA 49 455. NUCLEAR REACTIONS 3 a S ( p o l a r i z e d t , t ) , ( p o l a r i z e d t , t ' ) , ( p o l a r i z e d t , a ) , E = 1 7 MeV; m e a s u r e d a(O),A(O). 31p l e v e l s d e d u c e d s p e c t r o s c o p i c f a c t o r s . O p t i c a l model,DWBA,CCBA a n a l y s e s . NUPAB 388 542. NUCLEAR REACTIONS 3°Si(p,(~),E=4.9-6.08 MeV; m e a s u r e d a(E,E((x),O), alp d e d u c e d levels,J,Tr, orbital momentum m i x i n g r a t i o s , F , l e v e l d e n s i t y . E n r i c h e d t a r g e t . PRVCA 25 1751. NUCLEAR REACTIONS aSSi(a,pT),E=7.95,8 MeV; m e a s u r e d pv(O,H) i n m a g n e t i z e d Fe. 31p l e v e l s d e d u c e d g. E n r i c h e d t a r g e t , I M P A C . NUPAB 379 22. RADIOACTIVITY 31C1 f f r o m 3aS(p,an),E=33 MeV]; m e a s u r e d f l - d e l a y e d Ep,Ip,E(x,I~; d e d u c e d TI/a, log f t . 3iS d e d u c e d l e v e l , p o s s i b l e J,zr. H e l i u m j e t s y s t e m , Z n S t a r g e t s . PYLBB 110 437. NUCLEAR REACTIONS a7Al,agSi(3He,n),E=15 MeV; m e a s u r e d a(O),a(En), agP,31S l e v e l s d e d u c e d L, enhancement f a c t o r s . DWBA a n a l y s i s , s h e l l m o d e l . PRVCA 26 789. RADIOACTIVITY 31C1 [ - f r o m 3aS(p,an),E=33 MeV]; m e a s u r e d f l - d e l a y e d Ep,lp,Ea,l~; d e d u c e d T1/a, log f t . 31S d e d u c e d l e v e l , p o s s i b l e J,~r. H e l i u m j e t s y s t e m , Z n S t a r g e t s . PYLBB 110 437.

A 3aAl

AND

=

34

NUCLEAR MOMENTS 34,32S,35,37C1,36,4°Ar; measured isotope shifts; deduced strong specific mass effect,electron momentum correlation. Collinear laser spectroscopy,Ar,S,C1 ion b e a m s . ZPAAD 305 39.

18

KEY

NUMBERS

A 34 S

R

34C1

D 82Gr07

82Be32

R 82De29

82Ta04

82Va02

J

82El01

D 82Hi05

36 S

D 82Hi05

36C1

R 82Kr12 82Ta04

36Ar

J

82El01

R 81A126

81Ca16

81Pa27 83C101

82Ga09

82Pa17 82Sc13

82Xa01

34

continued

=

35

NUCLEAR MOMENTS 34,32S,35,37C],36,4°Ar; m e a s u r e d isotope mass effect,electron momentum correlation. Collinear b e a m s . Z P A A D 305 39.

A

36p

=

KEYWORDS

NUCLEAR REACTIONS 3 4 S , 4 2 C a ( p o l a r i z e d p , p ' ) , E = 6 5 0 MeV; 3 ° S i ( p o l a r i z e d p , p ' ) , E = 6 5 0 , 8 0 0 MeV; measured a(O). 26Mg,3°Si,42Ca,34S d e d u c e d neutron,proton transition matrix element relative s i g n . P R L T A 4 9 451. R A D I O A C T I V I T Y 81,82m,83,84,s4mRb,83,85mSr; m e a s u r e d T1/2,ET,IT. 87mSr,34mc1; m e a s u r e d T~/a. Spoliation reaction p r o d u c t s , R b C 1 t a r g e t s . I J A R A 33 456. NUCLEAR REACTIONS 32S,~8Si(a,d),E=50 MeV; a e S ( d , a ) , E = 4 0 MeV; m e a s u r e d a(O). 3°p,34C1 deduced levels,L,S,Jjr. Natural targets. Microscopic,macroscopic DWBA c a l c u l a t i o n s . N U P A B 386 200. NUCLEAR REACTIONS 3 e S , a s , 3 a A r ( p o l a r i z e d d , a ) , E = 1 6 MeV; m e a s u r e d a(O),iTll(0),T~0(0),Tea(0); deduced j-transfer dependence. 3°p,34,36C1 l e v e l s d e d u c e d L , j - t r a n s f e r . Enriched targets. DWBA a n a l y s i s . N U P A B 377 l. NUCLEAR REACTIONS 3 ~ P ( a , n T ) , E = l l . 7 , 1 6 . 3 MeV; m e a s u r e d a(E%E),Doppler pattern,T1/~. a 4 M g ( 1 2 C , n p T ) , E = 3 2 - 3 5 MeV; m e a s u r e d a ( E T , 0 ) , c r ( E T , E ) , 7 7 - e o i n , E T , 7 7 ( 0 ) , a4CI d e d u c e d l e v e l s , T~/a,7-branching,J,rr,& Enriched target,hyperpure Ge,large-angle Compton suppression spectrometer. N U P A B 373 81.

A 35C1

AND

=

shifts; deduced strong specific laser spectroscopy,Ar,S,C1 ion

36

R A D I O A C T I V I T Y 38p [ f r o m 37Cl(n,2p)J; measured E T , I T , 7 7 - c o i n , T 1 / z ; d e d u c e d log f t . 36S d e d u c e d l e v e l s , J j r . Ge(Li) d e t e c t o r s . P R V C A 25 3104. R A D I O A C T I V I T Y 36p [ f r o m 37Cl(n,2p)]; measured E T , I T , 7 7 - c o i n , T 1 / 2 ; d e d u c e d log f t . aSS deduced l e v e l s , J , r r . Ge(Li) d e t e c t o r s . P R V C A 25 3104. NUCLEAR REACTIONS 3 5 C l ( n , 7 ) , E = t h e r m a l ; measured ET,I~. 3~C1 d e d u c e d levels,neutron binding energy. Crystal,pair spectrometers. N U P A B 386 245. NUCLEAR REACTIONS 3aS,36,3SAr(polarized d , a ) , E = 1 6 MeV; m e a s u r e d cr(0),iTn(0),T20(0),Tze(O); deduced j-transfer dependence. 3°P,34,36C1 l e v e l s d e d u c e d L , j - t r a n s f e r . Enriched targets. DWBA a n a l y s i s . N U P A B 377 1. NUCLEAR MOMENTS 34,32S,35,37C1,36,4°Ar; m e a s u r e d isotope shifts; deduced strong specific mass effect,electron momentum correlation. Collinear laser spectroseopy,Ar,S,C1 ion b e a m s . Z P A A D 305 39. NUCLEAR REACTIONS 12C(28Si,2a),(12C,SBe),E=68-80 MeV; m e a s u r e d a a - c o i n ; d e d u c e d r e a c t i o n dependent structure, aSAr d e d u c e d structures near yrast l i n e . 3aS d e d u c e d strong population o f h i g h l y i n g l e v e l s . F Z K A A 13 43. NUCLEAR REACTIONS 2 4 M g ( l a C , a ) , E ( c m ) = l l . 9 - 1 6 . 1 MeV; m e a s u r e d or(E); d e d u c e d spin selectivity. 36Ar d e d u c e d no definitive intermediate resonances. Statistical analysis. F Z K A A 13 37. NUCLEAR REACTIONS 1ZC(zeSi,a),E=84-92 MeV; m e a s u r e d cr(E(x,E). 3SAr l e v e l s d e d u c e d s e l e c t i v e population. F Z K A A 13 41. NUCLEAR REACTIONS 16,180,a4Mg,aSSi,aaS,36Ar,4°Ca,54Cr,144,15~,154Sm,Z°apb,a3aTh(polarized d,d), (polarized d,d'),E=18-23 MeV; m e a s u r e d c r ( ~ ) , i T u ( e ). Is,180,24Mg,Zssi,32S,36Ar,4°Ca,54Cr,144, 15a,154Sm,2°spb,a32Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition strength. 154 ~5a,144Sm,23aTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . P R L T A 48 1082. NUCLEAR REACTIONS 24Mg(lZC,X),I2C(a4Mg,X),E(cm)=16.4-29.8 MeV; 1 2 C ( a s S i , X ) , E ( c m ) = 1 5 . 1 - 2 4 . 6 MeV; 2 4 M g ( 2 4 M g , X ) , E ( c m ) = 3 1 - 4 1 . 6 MeV; a S M g ( e 4 M g , X ) , E ( c m ) = 2 0 . 3 - 3 2 . 9 MeV; aeSi(24Mg,X), E(cm)=24.2-38.1 MeV; 2 8 S i ( 2 s S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; a g s i ( a e S i , X ) , E ( c m ) = 2 7 . 4 - 4 2 . 1 MeV; 3 ° S i ( a S S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d a(fusion) vs E,0,a(fragment 0,E). 36Ar,4°Ca,48, 5°Cr,52Fe,56,57,SSNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877. NUCLEAR REACTIONS 12,13C(aeSi,a),E=75-102 MeV; m e a s u r e d cr(Ea),cr(0=0 °) v s E. 3SAr d e d u c e d l e v e l s . P R V C A 26 1295. NUCLEAR REACTIONS a ° N e ( 1 6 0 , l e C ) , E ( c m ) = 2 2 . 8 - 3 8 . 6 MeV; m e a s u r e d a ( E ) , a ( 0 ) , e°Ne(~60,e°Ne), E(cm)=22.8-38.6 MeV; m e a s u r e d cr(E); d e d u c e d deviation function v s E. 36At d e d u c e d resonances,J. PYLBB 112 323. NUCLEAR REACTIONS a°Ne(160,X),E(cm)=15-29 MeV; m e a s u r e d p r o d u c t i o n cr(E) f o r 3°,31P,34C1,33, 34S,a4Mg,aSSi,a°Ne. 36At d e d u c e d c r i t i c a l (L) f o r f u s i o n , r e s o n a n c e s , e f f e c t i v e band crossing moment of inertia. Activation techniques. P R V C A 25 2 4 5 7 .

19

KEY

NUMBERS

A aTCI

J

37At

R 82Ta03:

82El01:

AND

=

D 82De08:

37

NUCLEAR MOMENTS a4,aas,a5,a~Cl,aS,4OAr; m e a s u r e d isotope shifts; deduced strong specific mass effect,electron momentum correlation. Collinear laser spectroseopy,Ar,S,C1 ion b e a m s . Z P A A D 305 39. NUCLEAR REACTIONS 7Li,is,~4C,aOMg,a?C1,4eCa(p,n),E=60-200 MeV; m e a s u r e d q(0=0°); deduced isovector effective interaction strength r a t i o . ?Be,la,~4N,ZSAl,aTAr,~aSc l e v e l s d e d u c e d Gamow-Teller transition strengths. P R V C A 25 1094.

A 38C1

KEYWORDS

38

RADIOACTIVITY

aSAl,ZSF,aaCl,SSRb V f r o m aTAl,iOF,a~c1,87Rb(d,p),E=l-6.5 MeV]; m e a s u r e d Eft, energies,Qfl. Hyperpure Ge d e t e c t o r , o n - l i n e s e p a r a t i o n . NUIMA 192 261. R A D I O A C T I V I T Y aSK(IT) [ f r o m e4Mg(~°O,np),E=38 MeV]; e4Na(IT) [ f r o m eaNa(d,p),E=4 MeVJ; ~TSe(IT) [ f r o m ~ 4 G e ( a , n ) , E = 1 6 M e V ] ; 71Ge(EC) [ f r o m 7 ° G e ( d , p ) , E = 6 M e V ] ; 7aAs(EC),77As(fl-) [from 7a,TSGe(d,n),E=6,7 MeV]; m e a s u r e d T1/a. 0 n - l i n e computerized d i g i t i z e r . NUIMA 178 581. R A D I O A C T I V I T Y asK [ f r o m aoK(7,n),E=22 MeV b r e m s s t r a h l u n g ] ; m e a s u r e d fl+ e n d - p o i n t e n e r g y . NCLTA 32 267. NUCLEAR MOMENTS 3~,as,41,4a,44,45,~,47K [ f r o m Ir(p,X),E=2O GeV]; measured hfs,isotope shifts. 38,39,41,4g,43,44,45,46,47K d e d u c e d /~,rms charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169.

flT-coin,fl-endpoint as K

D 80Joll:

81Ch34: J

82To02:

A aa K

J

82To02:

agCa

R 82Wa17:

J

82Ei01:

R 820tOl: 82Sa19:

40 K

R 81He20:

40Ca

D 82Ho09: J

82Ay02:

R 82B109 82Bl10

82Bu05 82C101

82Co12

39

NUCLEAR MOMENTS as,as,41,43,44,45,4°,47K [ f r o m Ir(p,X),E=2O GeV]; measured hfs,isotope shifts. 3s,39,41,42,43,44,45,46,47K d e d u c e d /~,rms charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169. NUCLEAR REACTIONS 4°,4BCa(p,np),E=149.5 MeV; m e a s u r e d a ( 0 p , 0 n , E p ) , p n - c o i n . 3a,47Ca l e v e l s d e d u c e d CaS. DWIA a n a l y s i s . P R V C A 26 961.

A 40At

=

=

40

NUCLEAR MOMENTS 34,32S,35,37C1,36,4°Ar, m e a s u r e d isotope shifts; deduced strong specific mass effect,electron momentum correlation. Collinear laser spectroscopy,Ar,S,Cl ion b e a m s . Z P A A D 305 39. NUCLEAR REACTIONS 4°Ar(e,e),E=116,249 MeV; m e a s u r e d (T(0). 4°Ar d e d u c e d r m s c h a r g e r a d i u s . Fourier-Bessel a n a l y s i s . N U P A B 379 396. NUCLEAR REACTIONS 1~24Mg~8Si~4~Ar~4~44~48Ca~46~4~5~Ti~54~56Fe~58~6~6~64Ni~9Y~9~Zr~8~1~M~ 1 4 4 S m , a ° s p b , Z ° O B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d (7(0),A(0); d e d u c e d optical model parameters. 1°0,24 Mg,zSSi,4 SA r,4°,44,4SCa,4°,as,SOTi,S4,SSFe,58,so,°2,64Ni,sSY,9°Zr,SS,lOOMo,144Sm, essPb,eSSBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . P R V C A 26 9 4 4 . NUCLEAR REACTIONS 27Al(lSF,xnyp),E=47-108 MeV; m e a s u r e d E % 7 7 - c o i n , 7 ( 0 ) . 4°K,42Ca d e d u c e d high-spin states. Anti-Compton Spectrometer. N U P A B 372 253. R A D I O A C T I V I T Y 4°Sc [ f r o m 4°Ca(p,n)~; m e a s u r e d f l - d e l a y e d E(p),Ea,I(p),I(x,T1/e; d e d u c e d log ft,fl-strength function. 4°Ca d e d u c e d l e v e l s , F c ~ / F p , J , ~ , T . N U P A B 380 410. NUCLEAR MOMENTS 43Ca; m e a s u r e d h f s ; d e d u c e d electric q u a d r u p o l e m o m e n t , d i p o l e , q u a d r ' u p o l e constants. Atomic beam magnetic resonance,laser i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 4 0 4243, 44,4s,4SCa; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High' resolution laser spectroscopy. Z P A A D 306 1. NUCLEAR REACTIONS lZc,4SCa(Tr+,Tr+'),(~-,Tr-'),E=80 MeV; m e a s u r e d cr(0),(r(Tr'); d e d u c e d o p t i c a l potential parameters. 4°Ca d e d u c e d , l e v e l , L , G Q R e x c i t a t i o n . DWBA a n a l y s i s . PRVCA 25 2554. NUCLEAR REACTIONS 4 S C a ( p , p ) , ( p , p ' ) , ( p o l a r i z e d p,p),(polarized p , p ' ) , E = 0 . 8 GeV; m e a s u r e d (r(Ep'),a(O),A(0). 4SCa d e d u c e d ground state density distribution,correlation length, deformation parameters fla,fla,fl5. G l a u b e r m u l t i p l e scattering t h e o r y . P R V C A 25 2563. NUCLEAR REACTIONS 4 ° C a ( e , e ' ) , E = 3 1 - 6 5 MeV; m e a s u r e d a(0),(~(E(e')),form factors. 4SCa transition d e d u c e d B(MI),F. P R V C A 25 2805. NUCLEAR REACTIONS ~s,iaO,24Mg,28si,a2s,aSAr,4°Ca,54Cr,144,15~,154Sm,e°sPb,232Th(p o l a r i z e d d,d), (polarized d,d'),E=18-23 MeV; m e a s u r e d q ( 0 ) , i T l ~ ( 0 ) , ls,lSO,24Mg,2SSi,aZS,SSAr,4OCa,54Cr,144, ls2,1S4Sm,2°sPb,aa~-Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition strength. 154 15a,144Sm,ZaaTh d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . P R L T A 4 8 1082. NUCLEAR REACTIONS 4°Ca(SLi,SLi),E=36,30 MeV; 4°Ca(~Li,SLi'),E=30 MeV; m e a s u r e d a(0); deduced optical model parameters. 4°Ca l e v e l s d e d u c e d d e f o r m a t i o n lengths. DWBA,double folding,cluster f o l d i n g m o d e l s . P R V C A 26 486.

20

KEY

NUMBERS

A 49Ca

R

82Ec01

82Ga02

82Ga09

82Ho13 82Mo05

82Pr05 82Re03

82Re14

82Sa19

82Ta05

82Zw01 4OSc

D

82Ho09

R

82Ba50 82Ta05

49Ti

R 82Mo12:

J

82To02:

R 82Re14:

41Sc

R 82Wa12:

J

82To02:

continued

=

41

38,39,41,43,44,45,46,47K C f r o m I r ( p , X ) , E = 2 0 GeV]; m e a s u r e d h f s , i s o t o p e 38,39,41,42,43,44,45,46,47K d e d u c e d / z , r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y , t h e r m a l b e a m . PYLBB 108 169.

atomic NUCLEAR REACTIONS 4°Ca(lSO,lS0),(ls0,180'),(lSO,170),(180,19F),E=62.14 MeV; m e a s u r e d a(0), a(E(lV0)),cr(E(19F)), lSO,4°Ca t r a n s i t i o n deduced deformation l e n g t h s . 41Ca l e v e l s d e d u c e d spectroscopic factors. Optical model,DWBA,coupled-channels c a l c u l a t i o n s . PRVCA 26 1010. NUCLEAR REACTIONS 4 ° C a ( p , p ' ) , ( p o l a r i z e d p , p ' ) , E = 5 . 9 - 6 . 5 MeV; m e a s u r e d a(Ep',E),a(0), a n a l y z i n g p o w e r , s p i n f l i p v s 0. 41Sc d e d u c e d r e s o n a n c e s , J , r r , F , P p , F p ' , c o n f i g u r a t i o n . PRVCA 26 107.

A 42 K

40

NUCLEAR MOMENTS

shifts. 41Ca

=

KEYWORDS

NUCLEAR REACTIONS 2SSi,4°Ca(TLi,TLi),(TLi,TLi'),E=45 MeV; m e a s u r e d a ( 0 ) ; d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 4°Ca d e d u c e d d e f o r m a t i o n l e n g t h . D o u b l e f o l d i n g m o d e l , c o u p l e d - c h a n n e l s c a l c u l a t i o n s . PRVCA 25 2391. NUCLEAR REACTIONS 9°Zr,12OSn,144Sm,2°spb(p,p'),E=800 MeV; m e a s u r e d a(0). 9°Zr,la°Sn,144Sm, a°epb,4°Ca,SSNi d e d u c e d d e f o r m a t i o n lengths,neutron,proton matrix element ratios. Optical m o d e l , D W B A a n a l y s e s . PRVCA 25 408. NUCLEAR REACTIONS e4Mg(leC,X),laC(24Mg,X),E(cm)=16.4-29.8 MeV; laC(asSi,X),E(cm)=15.1-34.6 MeV; 24Mg(a4Mg,X),E(cm)=21-41.6 MeV; 26Mg(24Mg,X),E(cm)=20.3-32.9 MeV; 2SSi(a4Mg,X), E(cm)=24.2-38.l MeV; 2 8 S i ( 2 8 S i , X ) , E ( e m ) = 2 7 . 9 - 4 1 . 4 MeV; 2 9 S i ( a S S i , X ) , E ( e m ) = 3 7 . 4 - 4 2 . 1 MeV; 3 ° S i ( a S S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d a ( f u s i o n ) v s E , 0 , G ( f r a g m e n t 0,E). 36Ar,4°Ca, 48, 5°Cr,haFe,56,57,SSNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . M a c r o s c o p i c m o d e l , c o u p l e d - c h a n n e l s calculations. PRVCA 25 1877. NUCLEAR REACTIONS 4°Ca,2SSi,24Mg(polarized p,p'),E=65 MeV; m e a s u r e d a(0),A(O). 4°Ca l e v e l s d e d u c e d i s o s p i n d e p e n d e n c e . DWBA a n a l y s i s . PRVCA 26 1440. NUCLEAR REACTIONS 4°Ca(~/,~'),E=8.5,11.3,11.7 MeV b r e m s s t r a h l u n g ; measured E% 4°Ca deduced Ievels,J,w,F,F%B(E2),EWSR,B(M1). R e s o n a n c e f l u o r e s c e n c e technique. PRVCA 25 1824. NUCLEAR REACTIONS 3 6 A r ( a , 7 ) , E = 5 . 4 9 5 - 5 . 5 0 5 MeV; m e a s u r e d E-/,IT,-/ y i e l d s . 4°Ca d e d u c e d v-transitions,B(M1),F~F~//F,F~//F,P% PYLBB 115 291. NUCLEAR REACTIONS 4°,4a,44Ca(lSO,lsO),(iSo,~S0'),E=60 MeV; 48Ca(160,160),(160,160'),E=56 MeV; m e a s u r e d a(0),a(E(160)). 4°Ca l e v e l s d e d u c e d d e f o r m a t i o n l e n g t h s . 42,44,4SCa l e v e l s d e d u c e d deformation l e n g t h s , B ( X ) . D W B A , c o u p l e d - c h a n n e l s a n a l y s i s . PRVCA 25 1915. NUCLEAR REACTIONS 4°Ca(leo,lS0),(lSO,isO'),(iSo,170),(lSo,19F),E=63.14 MeV; m e a s u r e d cr(0), ~(E(~vO)),cr(E(19F)). iSO,4°Ca t r a n s i t i o n deduced deformation l e n g t h s . 4iCa l e v e l s d e d u c e d spectroscopic factors. Optical model,DWBA,coupled-channels c a l c u l a t i o n s . PRVCA 26 1010. NUCLEAR REACTIONS 16O'a4Mg'2~Si~4~Ar~4o'44~4~Ca'46~48~5~Ti'54'56Fe'5~69~s2~64Ni~9Y~99Zr'9~']9~M~ i 4 4 S m , a ° S P b , 2 0 9 B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d &(O),A(O); d e d u c e d optical model parameters. 160,a4Mg,~8Si,49A r,49,44,49Ca,46,48,59Ti,54,56 Fe,58,6°,62,64 Ni,89y,9°Zr,98,19°Mo,144Sm, 298pb,209Bi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944. NUCLEAR REACTIONS 12C,~60,a7A1,28Si,49Ca,46Ti,9°Zr(3He,t),(3He,3He'),E=130,170 MeV; m e a s u r e d c r ( E t ) , a ( E ( 3 H e ) ) , a ( O ) . 160,27Al,~sSi,4OCa,46Ti,99Zr d e d u c e d T=0,GQR. IaN,16F,aTsi,aSP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253. NUCLEAR REACTIONS Z4Mg,4°Ca(a,pa),(a,2a),E=120 MeV; m e a s u r e d ap(O),ac~(O),cr(Ea),a(O=O°)/ a ( 0 = 1 8 0 9 ) . 24Mg,49Ca d e d u c e d g i a n t r e s o n a n c e d e c a y c h a r a c t e r i s t i c s . PRVCA 25 2i39. RADIOACTIVITY 49Sc [ f r o m 4°Ca(p,n)3; m e a s u r e d f l - d e l a y e d E(p),Ea,I(p)ja,Twa; d e d u c e d log ft,fl-strength function. 4°Ca d e d u c e d l e v e l s , F a / F p , J , T r , T . NUPAB 380 410. NUCLEAR REACTIONS 49Ca(Tr+3r°),(Tr-,rr°),E=164 MeV; m e a s u r e d a(0,E(r;°)); d e d u c e d a(Tr+)/a(~-). 4°Sc d e d u c e d IAS. D W I A , G o l d h a b e r - T e l l e r transition d e n s i t y . PRLTA 49 1376. NUCLEAR REACTIONS 12C,t60,aTA1,28Si,4OCa,46Ti,99Zr(3He,t),(aHe,aHe'),E=130,170 MeV; m e a s u r e d a ( E t ) , ~ ( E ( 3 H e ) ) , ~ ( 0 ) . 160,a7Al,assi,4°Ca,46Ti,99Zr d e d u c e d T=0,GQR. 12N,16F,a7Si,aSp,49Sc,4°V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253. NUCLEAR REACTIONS 160,aSSi,4OCa(~r+,Tr-),E=164 MeV; m e a s u r e d a(E(Tr-)) at 0=59; d e d u c e d m a s s d e p e n d e n c e of or,isobar c o m p o n e n t s i n w a v e f u n c t i o n . 2SS,4°Ti d e d u c e d m a s s e x c e s s . PRVCA 25 3218.

A 41K

AND

=

42

NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K C f r o m I r ( p , X ) , E = 2 0 s h i f t s , as . 39. 41. 42 . 43 . .44. 45. 46 47 K d e d u c e d / ~ , r m s c h a r g e r a d i i . a t o m i c b e a m . PYLBB 108 169.

21

CeV]; Laser

measured hfs,isotope spectroscopy,thermal

KEY

N U M B E R S AND

A 42Ca

J

82Ay02:

R

81He20: 82Be32:

82Re03:

42Sc

R

81Go18: 82Ta03:

J 82Du06 82To0E

43Ca

J 82Ay02

43S0

R 81Bo37

82Ab03 43Ti

R

82Vi05

J 82Du06 82To02

44Ca

D 81Yu03 J

82Ay02

R

81Ha50 82Re03

82Sa19

44S0

D

44Ti

R 82Di05:

81Yu03

continued

=

43

NUCLEAR MOMENTS 43,44K; m e a s u r e d hfs. ABMR,laser optical pumping. JOPQA 4 3 509. NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K [ f r o m I r ( p , X ) , E = 2 0 GeV3; m e a s u r e d hfs,isotope shifts. 38,39,41,42,43,44,45,46,47K d e d u c e d /-t,rms charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169. NUCLEAR MOMENTS 43Ca; m e a s u r e d hfs ; d e d u c e d e l e c t r i c q u a d r u p o l e m o m e n t , d i p o l e , q u a d r u p o l e constants. Atomic beam magnetic resonance,laser i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 424243 44,46,49Ca; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High resolution laser spectroscopy. ZP A A D 306 1. NUCLEAR REACTIONS 4 6 , 4 9 T i ( p o l a r i z e d p , a ) , E = 7 9 . 2 MeV; m e a s u r e d (r(0),A(0). 43,45Sc d e d u c e d levels,j-transferjr. DWBA,multi-step analysis,microscopic form factors. Enriched 46,48Ti t a r g e t s . NUPAB 372 51. NUCLEAR REACTIONS 4 6 , 4 8 , 5 6 T i ( p , a ) , E = 4 0 . 3 5 MeV; m e a s u r e d or(0). 43,45,47Sc d e d u c e d l e v e l s , j-transferdr. DWBA a n a l y s i s , m i c r o s c o p i c f o r m f a c t o r s . NUPAB 382 185. NUCLEAR REACTIONS 1 4 C ( p , w - ) , E = 1 8 3 MeV; 1 8 0 ( p , ~ - ) , E = 1 9 1 MeV; 42,48Ca,89Y,gOZr(p,Tr-),E=206 MeV; m e a s u r e d a(0,E(Tr)),cr(0). 150,19Ne,4a,ggTi,agNb,glMo d e d u c e d h i g h - s p i n state excitation mechanism. PRLTA 49 1314.

A 44 K

42

NUCLEAR MOMENTS 43Ca; m e a s u r e d hfs ; d e d u c e d e l e c t r i c q u a d r u p o l e m o r n e n t , d i p o l e , q u a d r u p o l e constants. Atomic beam magnetic resonance,laser i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 4 6 4 e, 4 3 44,46,4aCa; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High resolution laser spectroscopy. ZP A A D 306 1. NUCLEAR REACTIONS 27Al(19F,xnyp),E=47-108 MeV; m e a s u r e d E T , 7 7 - c o i n , 7 ( 0 ) . 49K,42Ca d e d u c e d high-spin states. Anti-Compton Spectrometer. NUPAB 372 253. NUCLEAR REACTIONS 3 4 S , 4 2 C a ( p o l a r i z e d p , p ' ) , E = 6 5 0 MeV; 3 ° S i ( p o l a r i z e d p , p ' ) , E = 6 5 0 , 8 0 0 MeV; measured a(0). 26Mg,3°Si,42Ca,34S deduced neutron,proton transition matrix element relative s i g n . PRLT A 49 451. NUCLEAR REACTIONS 46,42,44Ca(160,160),(160,160'),E=60 MeV; 49Ca('60,160),(160,160'),E=56 MeV; measured a(0),o'(E(160)). 46Ca l e v e l s d e d u c e d d e f o r m a t i o n l e n g t h s . 42,44,48Ca l e v e l s d e d u c e d deformation lengths,B()Q. DWBA,coupled-channels a n a l y s i s . PRVCA 25 1915. NUCLEAR REACTIONS 4 2 C a ( p , n ) , E = 1 6 0 MeV; m e a s u r e d a ( 0 , E n ) . 4ZSc d e d u c e d G a m o w - T e l l e r transition strength distribution. S h e l l m o d e l . PYLBB 107 406. NUCLEAR REACTIONS 7Li,la,14C,26Mg,aTC1,42Ca(p,n),E=60-200MeV; m e a s u r e d a(0=06); d e d u c e d isovector effective interaction strength r a t i o . 7Be,~3,14N,26A1,3~Ar,42Sc l e v e l s d e d u c e d Gamow-Teller transition strengths. PRVCA 25 1094.

A 43 K

=

KEYWORDS

=

44

NUCLEAR MOMENTS 43,44K; m e a s u r e d hfs. ABMR,laser optical pumping. JOPQA 4 3 509. NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K [ f r o m Ir(p,X),E=20 GeV]; measured hfs,isotope shifts. 38,39,41,42,48,44,45,46,47K d e d u c e d ~t,rrns charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169. R A D I O A C T I V I T Y 44,44mSc; m e a s u r e d E7,I7; deduced I ( f l + E C ) , l o g f t . 44Ca l e v e l d e d u c e d T-branching. YTHLD 3 316. NUCLEAR MOMENTS 43Ca; m e a s u r e d hfs ; d e d u c e d e l e c t r i c q u a d r u p o l e m o r n e n t , d i p o l e , q u a d r u p o l e constants. Atomic beam magnetic resonance,laser i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 40 4243 44,46,48Ca; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High resolution laser spectroscopy. ZPAAD 306 1. NUCLEAR REACTIONS 4 4 C a ( 7 , n ) , E = l l - 2 6 MeV b r e m s s t r a h l u n g ; measured a ( t o t a l ) v s E. 44Ca d e d u c e d GDR i s o s p i n , d e f o r m a t i o n splittings. A U J P A 34 505. NUCLEAR REACTIONS 4°,42,44Ca('60,160),(1~0,160'),E=60 MeV; 4aCa(160,160),(160,160'),E=56 MeV; measured (7(0),or(E(160)). 4°Ca l e v e l s d e d u c e d d e f o r m a t i o n l e n g t h s . 48,44,48Ca l e v e l s d e d u c e d deformation lengths,B(A). DWBA,coupled-channels a n a l y s i s . PRVCA 25 1915. NUCLEAR REACTIONS i6O~24Mg'~Si~4~Ar~4~'44~4~Ca~46~4~'5~Ti'54~56Fe~5~6o~62~4Ni'~9Y~9~Zr'9~'i~M~ 1 4 4 S m , 2 ° B P b , Z ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model 16Kl parameters. ~, 24~J ...g, 28~i ~., 40At, .._, 46 , 44 , 48("~ ~_, 46 , 49 , 56 T -1,' 54 , 56~ r e , 56 , 66 , 62 , 64Ni , 8 9 y , 9 6 Z r , 98 , i66M0 , 1 4 4 S m , 268pb,269Bi d e d u c e d p o i n t n u c l e o n distribution. PRVCA 26 9 4 4 . R A D I O A C T I V I T Y 44,44mSc; m e a s u r e d E7,I7; deduced l ( f l + E C ) , l o g f t . 44Ca l e v e l d e d u c e d 7-branching. YTHLD 3 316. NUCLEAR REACTIONS 4°Ca((~,7),E=4.46-4.62 MeV; m e a s u r e d , E T , I T , Q . 44Ti d e d u c e d m a s s e x c e s s . NUPAB 378 273.

22

KEY

NUMBERS

A 45K

J

45Se

R 81Bo37:

82To02:

82Ab03 82RyOl

82Sh12 45Ti

D 82Ho11:

45V

D 82Holl

J

82To02

46Ca

J

82Ay02

46Sc

R 82Ti02

46Ti

R 81Ch32

82Hali 82Ra01

82Sa19

82Ta05

46 V

R 82Ta05

J

47Ca

R 82Wa17:

47Sc

R 82Ab03:

47Cr

R 82Ha36:

82To02:

45

=

46

NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K [ f r o m Ir(p,X),E=20 GeV]; m e a s u r e d h f s , i s o t o p e s h i f t s . 38,39,41,4a,43,44,45,46,47K d e d u c e d /z,rms charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169. NUCLEAR MOMENTS 43Ca; m e a s u r e d hfs; deduced electric q u a d r u p o l e m o m e n t , d i p o l e , q u a d r u p o l e c o n s t a n t s . A t o m i c b e a m m a g n e t i c r e s o n a n c e , l a s e r i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 404243 44,4s,4SCa; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 306 1. NUCLEAR REACTIONS 4 5 S c ( n , ~ / ) , E = t h e r m a l ; m e a s u r e d E7,I7; d e d u c e d Q - v a l u e . 46Sc d e d u c e d l e v e l s J , r r , - y - b r a n c h i n g . NUPAB 376 421. NUCLEAR REACTIONS 27A1,28,a°Si(19F,X),E=34-75 MeV; m e a s u r e d a ( f u s i o n , E ) ; d e d u c e d m o d e l parameters. 46Ti d e d u c e d L ( c r i t i c a l ) v s e x c i t a t i o n . Glas-Mosel,statistical yrast models. PRVCA 24 2507. NUCLEAR REACTIONS 45Sc(3He,d),E=16 MeV; m e a s u r e d a ( E d , 0 ) . 46Ti d e d u c e d levels,L,Tr,CaS. N a t u r a l t a r g e t . NUPAB 378 11. NUCLEAR REACTIONS 4°Ar(gBe,3n),E=20 MeV; m e a s u r e d ?~/-coin,DSA; 43Ca(a,n),E=12-17 MeV; measured c r ( E ) , ~ / ~ - c o i n . 4STi d e d u c e d l e v e l s , T l / 2 , E 2 t r a n s i t i o n strength,7-branehing,Jdr, band structure. E n r i c h e d t a r g e t s , s o l i d A r t a r g e t , G e ( L i ) d e t e c t o r s . JPHGB 8 101. NUCLEAR REACTIONS 1sO•24Mg'a8Si•4•Ar'4•'44'4•Ca•46'48•••Ti•54••6Fe•5••6••6•'s4Ni•s•Y•9•Zr'9a'i••M•• 1 4 4 S m , 2 ° s P b , a ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(0); d e d u c e d optical model parameters. 160,24Mg,aSSi,4°A r,4 °,44,48Ca,46,48,5°Ti,54,S6Fe,58,6°,62,64 Ni,89y,a°Zr,98 lOOM0,144 Sin, a°aPb,a°gBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944. NUCLEAR REACTIONS laC,160,ZTAl,aSSi,4°Ca,46Ti,9°zr(aHe,t),(3He,aHe'),E=130,170 MeV; m e a s u r e d a ( E t ) , c r ( E ( a H e ) ) , a ( 0 ) . 160,aVAl,aeSi,4°Ca,4STi,9°Zr d e d u c e d T=0,GQR. laN,16F,avSi,aSP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253. NUCLEAR REACTIONS laC,xsO,27Al,asSi,4°Ca,4STi,9°Zr(3He,t),(aHe,3He'),E=130,170 MeV; m e a s u r e d c r ( E t ) , a ( E ( a H e ) ) , ~ ( 0 ) , l~O,aVAl,asSi,4OCa,46Ti,gOzr d e d u c e d T=0,GQR. tZN,laF,27Si,aaP,4°Sc,4SV, a°Nb d e d u c e d IAS o f T=I,GDR. PRVCA 25 1253.

A 47 K

=

KEYWORDS

NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K [ f r o m I r ( p , X ) , E = 2 0 GeV]; m e a s u r e d hfs,isotope s h i f t s . 38,39,41,42,43,44,45,46,47K d e d u c e d be,rms charge radii. Laser spectroscopy,thermal a t o m i c b e a m . PYLBB 108 169. NUCLEAR REACTIONS 46,48Ti(polarized p,a),E=79.2 MeV; m e a s u r e d a(0),A(0). 43,45Sc d e d u c e d levels,j-transfer,zr. DWBA,multi-step analysis,microscopic f o r m f a c t o r s . E n r i c h e d 46,48Ti t a r g e t s . NUPAB 372 51. NUCLEAR REACTIONS 46,4a,SOTi(p,a),E=40.35 MeV; m e a s u r e d or(0). 43,4s,47Sc d e d u c e d l e v e l s , j-transfer,w. DWBA a n a l y s i s , m i c r o s c o p i c f o r m f a c t o r s . NUPAB 382 185. NUCLEAR REACTIONS 4 S S c ( % p ) , E = 1 5 . 6 - 2 5 MeV b r e m s s t r a h l u n g ; m e a s u r e d a b s o l u t e a(E,0); deduced direct-semidirect,preequilibrium contributions. 45Sc d e d u c e d GDR i s o s p i n s p l i t t i n g . PRVCA 26 4 4 8 . NUCLEAR REACTIONS 44Ca(p,p'7),E=2.315-2.9903 MeV; m e a s u r e d a(0p'),-y(0). 4SSc r e s o n a n c e s deduced reduced widths,channel amplitudes. ZPAAD 305 307. R A D I O A C T I V I T Y 4SV [ f r o m 4°Ca(VLi,2n),E=14 MeV]; m e a s u r e d ET,I%fl-decay T~/2; d e d u c e d log f t . 45Ti l e v e l s d e d u c e d Ifl. PYLBB 116 4. RADIOACTIVITY 45V [ f r o m 4°Ca(7Li,2n),E=14 MeV]; m e a s u r e d ET,l%fl-deeay TI/z; d e d u c e d log f t . 45Ti l e v e l s d e d u c e d Ifl. PYLBB 116 4.

A 46 K

AND

=

47

NUCLEAR MOMENTS 38,39,41,43,44,45,46,47K [ f r o m I r ( p , X ) , E = 2 0 GeV]; m e a s u r e d hfs,isotope s h i f t s . 3s . 39. 41. 42 . 43 . .44. 45. 46 47 K d e d u c e d ~ z , r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y , t h e r m a l a t o m i c b e a m . PYLBB 108 169. NUCLEAR REACTIONS 4o,48Ca(p,np),E=149.5 MeV; m e a s u r e d a ( 0 p , 0 n , E p ) , p n - c o i n , ag,47Ca l e v e l s d e d u c e d C2S. DWIA a n a l y s i s . PRVCA 26 961. NUCLEAR REACTIONS 46,48,S°Ti(p,a),E=40.35 MeV; m e a s u r e d or(O). 43,4s,47Sc d e d u c e d l e v e l s , j-transfer,w. DWBA a n a l y s i s , m i c r o s c o p i c f o r m f a c t o r s . NUPAB 382 185. NUCLEAR REACTIONS 4STi(aHe,2n),E=32 MeV; 4°Ca(laC,na),E=38 MeV; m e a s u r e d ~ ? - c o i n , ~ ? ( t ) . 4?Cr d e d u c e d l e v e l s , J , T r , C o u l o m b d i s p l a c e m e n t e n e r g y . PRVCA 26 456.

23

NUMBERS

KEY

A 48Ca

J

82Ay03:

R 8~EuOI:

82Fu0~: 82Re03:

82Re07 :

82S219:

R 82An08 :

electron

R 82Sa19:

48

16(] q " 40 h 89~r ~, ~4~ ...g, 2 8~l, . . r , 40 , 44 ,48 C' _ a , 46 , 48 ,50rp" - I , 54 , 56~ r e , 58, 60, 62, 64~," i'~I, * , 90~ ~r, 98 , I 00, ~~ o , 144~ ~m,

2°aPb,2°SBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 9 4 4 . NUCLEAR REACTIONS i2C,~O,a4,2~Mg,aaSi,4SCa(p,n),E=6R-160 MeV; m e a s u r e d 26Al,16F,aap,4aSc

48Ti

=

KEYWORDS

NUCLEAR MOMENTS 43Ca; m e a s u r e d hfs; d e d u c e d e l e c t r i c q u a d r u p o l e m o m e n t , d i p o l e , q u a d r u p o l e constants. Atomic beam magnetic resonance,laser i n d u c e d r e s o n a n c e f l u o r e s c e n c e . 40,42 43, 44,46,48Ca; m e a s u r e d isotope shifts; deduced field,specific mass shifts. High resolution laser spectroscopy. ZP A A D 306 1. NUCLEAR REACTIONS 4 8 C a , 5 ° T i , S 2 C r , 5 4 F e ( e , e ' ) , E = 3 0 - 5 8 MeV; m e a s u r e d cr(E(e')),a(0). 5°Ti,52Cr, 54Fe d e d u c e d B(M1) s t r e n g t h distribution. 48Ca d e d u c e d t o t a l B(MI). S h e l l m o d e l . PYLBB 116 113. NUCLEAR REACTIONS 4 a C a ( p , p ' ) , E = 6 5 MeV; 4 8 C a ( a , a ' ) , E = 7 0 MeV; m e a s u r e d a ( 8 ) . 4SCa l e v e l deduced Jjr. Enriched t a r g e t , D W B A a n a l y s i s . PRVCA 25 678. NUCLEAR REACTIONS 4°,42,44Ca(~60,160),(160,160'),E=60 MeV; 48Ca(160,*60),(160,160'),E=56 MeV; measured a ( 0 ) , a ( E ( * 6 0 ) ) . 4°Ca l e v e l s d e d u c e d d e f o r m a t i o n l e n g t h s . 42,44,48Ca I e v e l s d e d u c e d deformation lengths,B(X). DWBA,coupled-channels a n a l y s i s . P R V C A ~5 1915. NUCLEAR REACTIONS 4 S C a ( p o l a r i z e d p , p ' ) , E = 1 5 9 . 8 MeV; m e a s u r e d a (Ep' ),~ r ( O ) , A ( 0 ) . 4SCa transition deduced virtual isobar-hole pair excitation effects. DWIA,shell model wave functions. PYLBB 114 15. - 40 - so NUCLEAR REACTIONS ~ 6 O, ~ 4 Mg, 2 2 Sl, A r , 4 0,~ 4 4, 2 Ca, 4 ~ 4 e,5 0 , T1,. s ~ 5 ~, Fe, ~ s ,s 0 6, z ~, N1, Y, ~ 0 Zr, 9 2 ~ ,0 ~ Mo, l~4Sm,2°aPb,2asBi(polarized p , p ) , E = 6 5 MeV; m e a s u r e d ¢(0),A(O); d e d u c e d optical model parameters.

48Sc

AND

level

scattering

deduced

data

a/B(MI)

input.

spin,current

contribution

a(O=O°)

v s E. t2N,24,

dependence.

Inelastic

PRVCA ~6 8.

NUCLEAR REACTIONS Is O, 24 Mg, ~aS*, • ~9 A r , 40 , 44 , 4a Ca, 4~ , 4a , 50 T1, . 54 , 5~Fe . 5s. 60~2 . u9 Y, 90 Zr, 9s , ~00Mo, . . ~4 N*, p , p ) , E = 6 5 MeV; m e a s u r e d o~(@),A(0); d e d u c e d optical model 16 ~, N 24~[ U 46 , 48 ~50~p. [ 144~~ m , parameters. ...g, 28~i ~., 40A~ .._, 40 , 44 , 48 ~a, -1, 54 , 561~ _e, 58 , 60 , 62 , 64N~.1,89 -v, 90~ ~ r , 98 , lOO}v ...o, 2°spb,a°SBi deduced point nucleon distribution. P R V C A 26 9 4 4 . NUCLEAR REACTIONS 2 4 M g ( l e c , x ) , 1 2 C ( Z 4 M g , X ) , E ( c m ) = 1 6 . 4 - 2 9 . 8 MeV; * 2 C ( 2 8 S i , X ) , E ( c m ) = 1 5 . l - 2 4 . 6 MeV; 2 4 M g ( e 4 M g , X ) , E ( c m ) = ~ l - 4 1 . 6 MeV; 2 S M g ( e 4 M g , X ) , E ( c m ) = 2 0 . 3 - 3 2 . 9 MeV; 28Si(24Mg,X), E(cm)=24.~-38.1 MeV; Z S s i ( Z a S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; ~ S S i ( ~ S S i , X ) , E ( c m ) = 2 7 . 4 - 4 ~ . l MeV; a ° S i ( 2 8 S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d a(fusion) vs E,0,a(fragment 0,E). a~Ar,4°Ca,4a, 5°Cr,52Fe,Sa,57,SSNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877.

i44Sm,2°ePb,a°SBi(polarized

48Cr

R 82Ga09 :

A 49 K

D 82Ca04:

49Ca

D 82Ca04:

49Sc

R

49Ti

R 82P104:

82Fi14:

82Vi05

49 V

R 810h08

R 81Wa31

82Eu01:

82Sa19:

49

R A D I O A C T I V I T Y 49K [ f r o m U(p,X),E=600 MeV]; m e a s u r e d f l - d e l a y e d E n , I n , n 7 - c o i n , E T , I T , T 1 / 2 , fl-activity; deduced fl-strength function,Ifl,log ft,neutron branching ratio,(Qfl-B(n)) difference. 49Ca d e d u c e d l e v e l s , p o s s i b l e J,Tr,configurations. PYLBB 109 419. R A D I O A C T I V I T Y 4*K [ f r o m U(p,X),E=600 MeV]; m e a s u r e d f l - d e t a y e d E n , I n , n T - c o i n , E 7 , I T , T , / 2 , fl-activity; deduced fl-strength function,Ifl,log ft,neutron branching ratio,(Qfl-B(n)) difference. 4aCa d e d u c e d l e v e l s , p o s s i b l e Jjr,configurations. PYLBB 109 419. NUCLEAR REACTIONS 48Ca,92Mo(a,t),E=:26-30 MeV; 42Ca,92Mo(3He,d),E=16 MeV; m e a s u r e d a b s o l u t e a ( 0 ) . 49Sc,93Tc l e v e l d e d u c e d n o r m a l i z a t i o n s . Enriched t a r g e t s . NUPAB 389 18. NUCLEAR REACTIONS 4 9 T i , 5 1 V , 5 ° C o , 8 7 S r , 9 3 N b , 2 ° S B i ( e , e ) , E = 1 7 5 - 3 2 5 , 5 0 0 MeV; m e a s u r e d a(0,E). 49Ti,5'V,aTSr,SaNb d e d u c e d v a l e n c e n u c l e o n rms,charge r a d i i . PWBA,DWBA a n a l y s e s , m e s o n exchange e f f e c t s . PRVCA 25 2318. NUCLEAR REACTIONS ' 4 C ( p , T r - ) , E = 1 8 3 MeV; laO(p,~r-),E=191 MeV; 42,4SCa,89Y,9°Zr(p,~r-),E=206 MeV; m e a s u r e d a ( 0 , E ( T r ) ) , q ( 0 ) , iao,'9Ne,a3,49Ti,9°Nb,SlMo d e d u c e d h i g h - s p i n state excitation mechanism. PRLTA 4 9 1314. NUCLEAR REACTIONS 4 6 T i ( a , p ) , E = 8 MeV; m e a s u r e d 77(0),pT-coin,recoil,DSA. 49V l e v e l s d e d u c e d 8,T1/2,B(),). S t r o n g - c o u p l i n g model calculation. J P H G B 7 1691.

A a0Ti

=

=

50

NUCLEAR REACTIONS 1 5 a G d ( n , a ) , b e V ( n , p ) , E = t h e r m a l ; m e a s u r e d a ( E a ) , a ( E p ) ; d e d u c e d Q. 153Gd d e d u c e d m a s s . SOV,b°Ti,'53Gd,15%m d e d u c e d m a s s d i f f e r e n c e . 235Th d e d u c e d m a s s . A n a l y z e d (n, a ) d a t a , 2 3 S u m a s s i n p u t . NUIMA 190 167. NUCLEAR REACTIONS 4 a C a , 5 ° T i , b a c r , a 4 F e ( e , e ' ) , E = 3 0 - 5 8 MeV; m e a s u r e d a ( E ( e ' ) ) , a ( O ) . 5°Ti,5eCr, 54Fe d e d u c e d B(M1) s t r e n g t h distribution. 4SCa d e d u c e d t o t a l B(M1). S h e l l m o d e l . PYLBB 116 113. NUCLEAR REACTIONS 16O~24Mg~Si'4oAr~4o~44~4~Ca'46'~'5~Ti~54~56Fe~5~6o~62'64Ni~Y~9oZr~1~oM~ 1 4 4 S m , 2 O a p b , 2 ° a B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model parameters, l s 0 , 2 4 M g , 2 8 S i , 4 ° A r,4a,44,48Ca,46,48,5°Ti,S4,bSFe,58,6°,62,64 N i ,89y,9° Zr,O S , l° ° M o , 1 4 4 S m , 2°8pb,2°OBi d e d u c e d point nucleon distribution. P R V C A 26 9 4 4 .

24

KEY

NUMBERS

A 5o V

J

82BI03

R 81Wa31

5OCF

R 82Ga09

J

81Pa28 82B103

R 78An29 82Dj04

82P104:

51Mn

R 78An28: 82Br03

R 81Isl0

82EuO1

5eFe

R 82Ga09:

R 82By01:

53Mn

R 78An28: 82K106:

continued

=

51

=

52

NUCLEAR REACTIONS 52Cr(3,,nT),(3,,pa,),E=10-32 MeV b r e m s s t r a h l u n g ; measured Ey,Ia,,ff(0), y i e l d s ; d e d u c e d a ( r e a c t i o n ) . 5aCt d e d u c e d g i a n t r e s o n a n c e c o n f i g u r a t i o n m i x i n g . YAFIA 33 570. NUCLEAR REACTIONS 4aCa,5°Ti,52Cr,S4Fe(e,e'),E=30-58 MeV; m e a s u r e d G(E(e')),cr(0). 5°Ti,S2Cr, 54Fe d e d u c e d B(M1) s t r e n g t h distribution. 4eCa d e d u c e d t o t a l B(M1). S h e l l m o d e l . PYLBB 116 113. NUCLEAR REACTIONS 24Mg(tmC,X),~2C(24Mg,X),E(cm)=16.4-29.8 MeV; ~2C(28Si,X),E(cm)=15.1-24.6 MeV; e 4 M g ( a 4 M g , X ) , E ( c m ) = 2 1 - 4 1 . 6 MeV; a 6 M g ( 2 4 M g , X ) , E ( c m ) = 2 0 . 3 - 3 2 . 9 MeV; ZaSi(24Mg,X), E(cm)=24.2-38.1 MeV; 2 8 S i ( 2 8 S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; a 9 S i ( ~ a S i , X ) , E ( c m ) = 2 7 . 4 - 4 2 . 1 MeV; a°Si(2Ssi,X),E(cm)=27.3-42.8 MeV; m e a s u r e d a(fusion) v s E,O,~(fragment O,E). 36Ar,4°Ca,48, ~°Cr,SaFe,56,57,5aNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877.

A 53Cr

50

NUCLEAR MOMENTS 51V; m e a s u r e d NMR; deduced electric quadrupole c o u p l i n g c o n s t a n t s . ZENAA 37 139. NUCLEAR MOMENTS 5°,SlV; m e a s u r e d NMR; d e d u c e d e l e c t r i c q u a d r u p o l e m o m e n t ratio. SmVO 4 crystal,low temperature. Spin Hamiltonian a n a l y s i s . J P C P A 15 L349. NUCLEAR REACTIONS 5 ¿ V ( p , p ) , ( p , p ' ) , E = 6 . 0 5 MeV; m e a s u r e d or(0). 5 1 V ( p , p ) , E = 5 . 3 9 - 6 . 0 5 MeV; measured ~(E). SlV l e v e l s d e d u c e d J , T r ~ c o n f i g u r a t i o n s . PIFLD 8 31. NUCLEAR REACTIONS 51v,SS,6°,6~Ni,68Zn,9°,92,94,96Zr,92,94,96,98,1°°Mo,12°,124Sn,140Ce(p,p,),E=200 MeV; m e a s u r e d o ( 0 ) . 51v,S8,6°,62Ni,68Zn,9°,92,94,96Zr,92,94,96,98,100Mo,120,124Sn,140Ce d e d u c e d resonances,F,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 4 9 T i , 5 ' V , 5 9 C o , S T S r , 9 3 N b , ~ ° g B i ( e , e ) , E = 1 7 5 - 3 2 5 , 5 0 0 MeV; m e a s u r e d a(O,E). 49Ti,s~V,STSr,gaNb d e d u c e d v a l e n c e n u c l e o n t i n s , c h a r g e r a d i i . PWEA,DWBA a n a l y s e s , m e s o n exchange e f f e c t s . P R V C A 25 2318. NUCLEAR REACTIONS s°,sa,53,54Cr,54,56,sT,5SFe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d or(E). 5t, 5a,54,55Mn,55,57,ss,59Co d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 5 O C r ( p , 7 ) , E = 3 . 2 - 3 . 3 MeV; m e a s u r e d ~(Ea,,E). 51Mn d e d u c e d r e s o n a n c e strengths,Fa,,gg/2 IAR c o m p o n e n t s . NCLTA 33 25. A

52Cr

=

KEYWORDS

NUCLEAR MOMENTS s°,51V; m e a s u r e d NMR; d e d u c e d e l e c t r i c q u a d r u p o l e m o m e n t ratio. SmVO¢ crystal,low temperature. Spin Hamiltonian a n a l y s i s . J P C P A 15 L349. NUCLEAR REACTIONS 1 5 a G d ( n , a ) , 5 ° V ( n , p ) , E = t h e r m a l ; m e a s u r e d cr(Ecx),o'(Ep); d e d u c e d Q. 15aGd d e d u c e d m a s s . 5°V,S°Ti,153Gd,ZS°Sm d e d u c e d m a s s d i f f e r e n c e , aaSTh d e d u c e d m a s s . A n a l y z e d (n, ~) d a t a , Z a S u m a s s i n p u t . NUIMA 190 167. NUCLEAR REACTIONS Z4Mg(laC,X),taC(a4Mg,X),E(cm)=16.4-29.8 MeV; t e C ( e s S i , X ) , E ( c m ) = 1 5 . 1 - 2 4 . 6 MeV; 2 4 M g ( 2 4 M g , X ) , E ( e m ) = 2 1 - 4 1 . 6 MeV; a 6 M g ( a 4 M g , X ) , E ( c m ) = 2 0 . 3 - 3 2 . 9 MeV; eSSi(a4Mg,X), E(em)=24.2-38,1 MeV; 2 8 S i ( a e S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; 2 9 S i ( z S S i , X ) , E ( c m ) = 2 7 . 4 - 4 2 . 1 MeV; 3 ° S i ( e a S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d if(fusion) vs E,0,G(fragment 0,E). 36Ar,¢°Ca,48, 5°Cr,52Fe,56,s7,sSNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877.

A 5t V

AND

=

53

NUCLEAR REACTIONS 5 ° T i , C r ( c ~ , n ) , E = l l MeV; m e a s u r e d Ev,13`,linear polarization v s 0,3,(0). 5act levels deduced rr,3,-branehing,d. Two crystal Compton polarimeter,sum,difference s p e c t r a . NUIMA 193 489. NUCLEAR REACTIONS 5°,sz,sa,S4Cr,54,ss,sT,SSFe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d ¢I(E). st sa,54,55Mn,SS,SV,ss,Sgco d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 5 2 C r ( p , 3 , ) , ( p , p ' 3 , ) , E = 4 . 1 4 - 4 . 2 MeV; m e a s u r e d E3,,13,,3,(0),¢7(0). 5 a C r ( p , p ) , E=4.59-4.72 MeV; m e a s u r e d cr(0) v s E. 5aMn d e d u c e d r e s o n a n e e s , F p , P , L , J , p o s s i b l e IAR. lSN(n, n ) , E = 1 4 - 1 8 MeV; c a l c u l a t e d a(E). Continuum shell model,correlation analysis. JPHGB 8 955.

25

KEY

NUMBERS

A 54Cr

R 82C101:

54Mn

R 78An28: 81Ga38:

24Fe

R 82EuOl:

82GuO2:

82Sa19:

R 78An28: 81Ka46:

55Fe

R 82Ke07:

52Co

D 82GrlO: R 78An28: 82Ma04:

D 80Sh28 R 82G106 82Gu02

82Sa19

26Co

D 80Sh28 82Gr08 82Gr10 82Ma24 R 82Na05:

54

=

55

NUCLEAR REACTIONS 5°,22,23,54Cr,24,ss,57,SSFe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d (x(E). 5, 23,54,55Mn,22,57,28,59Co d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 2 5 M n ( n , n ' 7 ) , E = l - 8 MeV; m e a s u r e d E~,,I% 25Mn d e d u c e d l e v e l s , J j r , T l / a . 1ANFA 45 1889. NUCLEAR REACTIONS 48Ti('2C,na),(12C,2np),E=39 MeV; m e a s u r e d ~ / - s p e c t r a , r e c o i l . 55Fe l e v e l s d e d u c e d T,/2,B(X ). 27Co l e v e l s d e d u c e d E2,M1 t r a n s i t i o n strength. Natural target,Ge(Li) d e t e c t o r s . PRVCA 26 716. RADIOACTIVITY 22Co,57Ni,S°,S'Cu,S2,S3Zn; m e a s u r e d E'r,I3,,T1/2. 55,27,58Co; m e a s u r e d E3',I3'. I J A R A 33 533. NUCLEAR REACTIONS s°,52,53,54Cr,54,2s,27,5SFe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d a(E). 5, 53,24,25Mn,52,27,58,59Co d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 28Si,24Fe,SSNi(3He,3He),(3He,d),E=90. MeV; 9OZr(aHe,3He),(3He,d),E=89.3 MeV; '24Sn(3He,3He),(3He,d),E=89.8 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l p o t e n t i a l s , aSP,22Co, 29Cu,91Nb,12sSb l e v e l s d e d u c e d spectroscopic f a c t o r s . DWBA a n a l y s e s . E n r i c h e d , n a t u r a l t a r g e t s . NUPAB 373 377.

A 5SFe

=

KEYW0RDS

NUCLEAR R E A C T I O N S 16,180,24Mg,2Ssi,32s,aSAr,40Ca,S4Cr,144,15a,'54Sm,20spb,232Th(polarized d,d), (polarized d,d'),E=18-23 MeV; m e a s u r e d cr(0),iT,i(0). 's,lSo,24Mg,ZSsi,a2s,S6Ar,4OCa,S4Cr,'44, '22,124Sm,2SSpb,23aTh levels deduced isoscalar quadrupole,oetupole transition strength. ,24 isz,144Sm,a32Th d e d u c e d neutron,proton deformation differences. Q 3 D spectrograph. Collective model. P R L T A 48 1082. NUCLEAR R E A C T I O N S 2°,2a,s3,54Cr,54,ss,sv,SSFe(p,p),(p,p'),E=5.20-6.05MeV; m e a s u r e d or(E). 21 2a,s4,52Mn,55,57,ss,29Co d e d u c e d IAR. Enriched targets. PIFLD 8 25. NUCLEAR R E A C T I O N S 23Cr(p,'7),(p,n),(p,p'),E=0.88-2.4 MeV; m e a s u r e d ¢x(E). 24Mn deduced IAS. Ge(Li),BF 3 n e u t r o n detectors. Statistical,global optical m o d e l analyses. A U J P A 34 25. NUCLEAR R E A C T I O N S 48Ca,S°Ti,52Cr,24Fe(e,e'),E=30-58 MeV; m e a s u r e d a(E(e')),a(0). 5°Ti,SaCr, 54Fe d e d u c e d B(MI) strength distribution. 4SCa d e d u c e d total B(MI). Shell model. P Y L B B 116 113. NUCLEAR REACTIONS 54,SSFe,2S,°°Ni,'2°Sn,a°spb(polarized n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 24, 2aFe,SS,SSNi,'a°Sn,Z°spb l e v e l d e d u c e d s p i n - o r b i t to C o u l o m b d e f o r m a t i o n parameter ratio. Coupled-channels a n a l y s i s . PRVCA 25 2854. NUCLEAR REACTIONS •••••4Mg•2•Si•4•Ar•4••44•4•Ca•4••48•5•Ti•54•••Fe••••s•••••64Ni••9Y•9•Zr•••••••M•• 1 4 4 S m , a ° a p b , ~ ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d (~(0),A(0); d e d u c e d optical model parameters. •6••24Mg•28Si•4•Ar•4••44•48Ca•4••4••5•Ti••4•••Fe•5•••••62 64Ni••9Y•9•Zr•••••••M••144Sm• Z°spb,2SgBi d e d u e e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944.

A 22Ms

AND

=

56

RADIOACTIVITY 5SCo; m e a s u r e d ET,IT,'y~(0 ). 5SFe d e d u c e d l e v e l s , J D r , 6 . PIPSB 46 181. NUCLEAR REACTIONS 5 S F e ( n , n ' 3 , ) , ( n , 2 n - / ) , E = 1 4 . 6 MeV; m e a s u r e d E3,,I~/; d e d u c e d a. 5SFe transitions deduced -/-multiplicity. IANFA 46 903. NUCLEAR REACTIONS s4,SSFe,5S,S°Ni,12°Sn,a°apb(polarized n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 54 5SFe,SS,6°Ni,12°Sn,2°aPb l e v e l d e d u c e d s p i n - o r b i t to C o u l o m b d e f o r m a t i o n parameter ratio. Coupled-channels a n a l y s i s . PRVCA 25 2854. NUCLEAR REACTIONS 2 •4 lMg S •4 A i•4 •r4 •4 4 •C •a 4 •4 •5 •T •5 •i4 5 •F •6 e •6 •2 4 •N Y •i9 •Z •9 •M r• • i44Sm,2°spb,2°SBi(polarized p,p),E=65 MeV; measured cr(0),A(0); deduced optical model p a r a m e t e r s . 160,24Mg,2asi,4°A r,4°,4 %4aca,4a,4 s,5°Ti,S4,SaFe,Se,s°,sa,s4 Ni,ssy,S°Zr,SB,i°°Mo,144 Sin, a°spb,2°SBi deduced point nucleon d i s t r i b u t i o n . PRVCA 26 944. RADIOACTIVITY SSCo; measured E-/,I~c/~/(0). 56Fe deduced levels,J,Tr,6. PIPSB 46 181. RADIOACTIVITY SSCo; measured Ifl+(0),asymmetry parameter; deduced Fermi,Gamow-Teller mixing ratio. Polarized source. PRLTA 49 109. RADIOACTIVITY 55Co,57Ni,s°,aIcu,62,S3Zn; measured E-/;I~/,T,/2. 55,57,58Co; measured E-y,I'y. IJARA 33 533. RADIOACTIVITY 2SCo; measured 7 CP following fl-decay; deduced Fermi to Gamow-Teller a m p l i t u d e ratio. PRVCA 26 287. NUCLEAR REACTIONS 5SNi(polarized d,a),E=80 MeV; measured vector analyzing power vs 0. 5SCo levels deduced J. Zero-range DWBA analysis. PYLBB 109 175.

26

KEY

NUMBERS

A 56Ni

R 82Ga09

R

57Co

D 82GrlO

81Wil5

R 78An28 82Ar04

82Ke07

57Ni

D 82Gr10 R 82Ga09

R 82NiOl

5SCo

D 82Gr10 R 78An28:

5SNi

R 81Ac02

83B116 82Dj02

82Dj04

82Ga02:

83Ga09:

82Ga16: 83Gu02:

56

continued

=

57

NUCLEAR REACTIONS S S F e ( n , v ) , E = 2 1 - 4 2 keV; m e a s u r e d c a p t u r e y i e l d v s E. 5~Fe r e s o n a n c e s deduced Fv,absolute v-transition strength. NSENA 77 58. R A D I O A C T I V I T Y 55Co,57Ni,6°,61Cufiafi3Zn; m e a s u r e d EV,Iv,T1/2. 56,57,S8Co; m e a s u r e d E7,I% I J A R A 33 533. NUCLEAR REACTIONS 50,52,sa,54Cr,54,56,57,56Fe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d or(E). 51 53,54,S5Mn,55,57,58,59Co d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 5 6 F e ( p , p ) , E = 3 . 1 - 4 . 2 MeV; m e a s u r e d a(E,0). 57Co d e d u c e d IAR,J,rr,Fp,F, Coulomb energy differences,S,proton strength function of s-wave resonances. Enriched t a r g e t . N U P A B 378 259. NUCLEAR REACTIONS 48Ti(lac,nc0,(~aC,2np),E=39 MeV; m e a s u r e d V - s p e c t r a , r e c o i l . 55Fe l e v e l s deduced T1/2,B(X ). 5~Co l e v e l s d e d u c e d E2,M1 t r a n s i t i o n strength. Natural target,Ge(Li) d e t e c t o r s . P R V C A 26 716. R A D I O A C T I V I T Y 55Co,5~Ni,S°,S~Cu,6a,~3Zn; m e a s u r e d EV,Iv,T1/~. 56,57,5SCo; m e a s u r e d EV,Iv. I J A R A 33 533. NUCLEAR REACTIONS 24Mg(12C,X),1ZC(a4Mg,X),E(cm)=16.4-29.8 MeV; 1 2 C ( a s S i , X ) , E ( c m ) = 1 5 . 1 - 2 4 . 6 MeV; a4Mg(a4Mg,X),E(cm)=21-41.6 MeV; ~aMg(a4Mg,X),E(cm)=20.3-33.9 MeV; 2SSi(a4Mg,X), E(cm)=24.2-38.1 MeV; a S S i ( z S S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; Z S s i ( a S S i , X ) , E ( e m ) = 2 7 . 4 - 4 2 . 1 MeV; 3 ° S i ( e S S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d a(fusion) v s E , 0 , ~ r ( f r a g m e n t 0,E). 36Ar,4°Ca,48, 5°Cr,5ZFe,56,57,58Ni d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877.

A 58Fe

=

KEYWORDS

NUCLEAR REACTIONS e4Mg(~aC,X),lZC(24Mg,X),E(em)=16.4-29.8 MeV; l a C ( a a S i , X ) , E ( c m ) = 1 5 . 1 - 2 4 . 6 MeV; 2 4 M g ( a 4 M g , X ) , E ( e m ) = 2 1 - 4 1 . 6 MeV; Z6Mg(Z4Mg,X),E(cm)=20.3-32.9 MeV; ZSSi(a4Mg,X), E(cm)=24.2-38.1 MeV; ZSsi(aSSi,X),E(cm)=~7.9-41.4 MeV; a S s i ( Z e S i , X ) , E ( c m ) = 2 7 . 4 - 4 3 . 1 MeV; 3 ° S i ( z S S i , X ) , E ( c m ) = 2 7 . 3 - 4 2 . 8 MeV; m e a s u r e d o r ( f u s i o n ) v s E , 0 , ~ r ( f r a g m e n t 0,E). 36Ar,49Ca, 48, 5°Cr,5aFe,56,57,58Ni d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 35 1877.

A 57Fe

AND

=

58

NUCLEAR REACTIONS 59Co(d,aHe),E=33.3 MeV; m e a s u r e d cr(E(3He),v). 58Fe l e v e l s d e d u c e d L,S. N U P A B 377 148. R A D I O A C T I V I T Y 55Co,57Ni,6°,61Cu,Sa,63Zn; m e a s u r e d EV,Iv,T1/2. 56,s7,58Co; m e a s u r e d EV,Iv. I J A R A 33 533. NUCLEAR REACTIONS 50,ha,53,54Cr,54,hS,57,58Fe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d a(E). 51, 53,54,55Mn,55,57,SS,haCo d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS 58Ni,2°8pb(V,v),E < 10 MeV; m e a s u r e d a(O). 58Ni d e d u c e d levels,J,rr,Py,E1, M1 t r a n s i t i o n strength. 2°sPb levels deduced PV. E n r i c h e d targets,nuclear resonance fluorescence technique. NUPAB 372 1. NUCLEAR REACTIONS 58Ni(p,p'),E=2Y MeV; m e a s u r e d G(0). 5SNi l e v e l s d e d u c e d J,Tr. C o l l e c t i v e , microscopic DWBA a n a l y s i s . N U P A B 386 61. NUCLEAR REACTIONS 58Ni(SHe,3He'),E=I30 MeV; m e a s u r e d (7(0); d e d u c e d optical model parameters. 58Ni d e d u c e d d e f o r m a t i o n lengths,parameters,giant resonance excitation,EWSR. DWBA a n a l y s i s . PHSTB 26 46. NUCLEAR REACTIONS 51v,hS,6°,SaNi,6SZn,9°,9a,94,96Zr,92,94,96,ss,1°°Mo,la°,124Sn,140Ce(p,p,),E=200 MeV; m e a s u r e d ~ ( 0 ) . 51V,hS,so,6zNi,68Zn,O°,sz,94,96Zr,Sa,94,96,ss,1°OMo 120,124Sn,140Ce d e d u c e d resonances,F,T,M1 character. NUPAB 388 I. NUCLEAR REACTIONS 9 ° Z r , l a ° S n , 1 4 4 S m , a ° 8 p b ( p , p ' ) , E = 8 0 0 MeV; m e a s u r e d ~(0). 9°Zr,12°Sn,144Sm, 208pb,4°Ca,58Ni d e d u c e d d e f o r m a t i o n lengths,neutron,proton matrix element ratios. Optical m o d e l , D W B A a n a l y s e s . P R V C A 25 408. NUCLEAR REACTIONS 24Mg(~aC,X),IaC(Z4Mg,X),E(cm)=16.4-29.8 MeV; ~ 2 C ( a s S i , X ) , E ( c m ) = I 5 . 1 - 2 4 . 6 MeV; a 4 M g ( 2 4 M g , X ) , E ( c m ) = 2 1 - 4 1 . 6 MeV; a S M g ( a 4 M g , X ) , E ( c m ) = 2 0 . 3 - 3 2 . 9 MeV; 2SSi(a4Mg,X), E(em)=a4.2-38.1 MeV; a a S i ( ~ S S i , X ) , E ( c m ) = 2 7 . 9 - 4 1 . 4 MeV; 2 9 S i ( a S S i , X ) , E ( c m ) = 2 7 . 4 - 4 2 . 1 MeV; a°Si(zSSi,X),E(cm)=27.3-42.8 MeV; m e a s u r e d G ( f u s i o n ) v s E , 0 , c r ( f r a g m e n t O,E). aSAr,4°Ca, 48, 50Cr,S2Fe,56,57,hSNi d e d u c e d f u s i o n b a r r i e r p a r a m e t e r s . Macroscopic model,coupled-channels calculations. P R V C A 25 1877. NUCLEAR REACTIONS 5 S N i ( a , a ' ) , E = 1 2 9 MeV; m e a s u r e d cr(0),cr(Ec~'). 58Ni d e d u c e d giant resonances,L,possible monopole. DWBA a n a l y s i s . P R V C A 35 3 ~ 0 4 . NUCLEAR REACTIONS 5 4 , 5 6 F e , 5 S f i ° N i , l a ° S n , a ° s p b ( p o l a r i z e d n , n ' ) , E = l O MeV; m e a s u r e d A(0). 54 56Fe,58,6°Ni,129Sn,a°spb l e v e l d e d u c e d s p i n - o r b i t to C o u l o m b d e f o r m a t i o n parameter ratio. Coupled-channels a n a l y s i s . P R V C A 25 2 8 5 4 .

27

KEY

NUMBERS

AND

A = 58Ni

R 82Sa19:

4 0

•

A R 78An28:

50Cu

R 82Ma04:

82Sz01:

R 82Bo09

82Bo25 82Dj04

82Gu02

82Sa19:

6OCu

D 82Gr10: R 82Ts04:

D 82Gr10:

OIZn

R 82SmOl:

R 82Dj04:

82Sa19:

62Zn

D 82Gr10:

=

60

=

61

R A D I O A C T I V I T Y 55Co,57Ni,60,°iCu,62,°aZn; m e a s u r e d ET,17,TI/2. 5°,57,50Co; m e a s u r e d E7,I7. I J A R A 33 533. NUCLEAR REACTIONS S ° N i ( a , n T ) , E = l O . 7 5 - 1 6 MeV; m e a s u r e d 77-,nT-coin,77(0),linear po!arization,(;(ET). °lZn deduced levels,J,~r,d,7-branching ratios. Enriched target,Ge(Li) detector,planar polarimeter. S h e l l m o d e l . J P H G B 8 281.

A OaNi

59

NUCLEAR REACTIONS ° ° N i ( 7 , n ) , ( 7 , p ) , E = 1 4 - 2 4 MeV b r e m s s t r a h l u n g ; m e a s u r e d (r(0),(r(total) v s E. S°Ni d e d u c e d GDR i s o s p i n s p l i t t i n g . Photon scattering d a t a i n p u t . P R LT A 4 8 986. NUCLEAR REACTIONS ° ° N i ( 2 e S i , 2 8 S i ) , ( 2 8 S i , 2 ° S i ' ) , E = 140 MeV; m e a s u r e d (7(0). 2SSi,S°Ni l e v e l s deduced sequential,simultaneous excitation. Coupled-channels method. PYLBB 114 423. NUCLEAR REACTIONS 61V,SS,60,62Ni,68Zn,90,9~,94,9°Zr,92,94,96,°8,160Mo,12o,124Sn140Ce(p,p,),E=200 MeV; m e a s u r e d (7(0). 51V,SS,60,°2Ni,°SZn,°O,92,94,96Zr,°2,94,9°,98,166Mo,i20,134Sn,140Ce d e d u c e d resonances,P,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 54,50F e ,58,° ° N i ,126S n,208pb(pol a ri z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 54, 56Fe,58,6°Ni,12°Sn,20epb l e v e l d e d u c e d s p i n - o r b i t to Coulomb deformation parameter ratio. Coupled-channels a n a l y s i s . P R V C A 35 2 8 5 4 . NUCLEAR REACTIONS 10~24Mg~28Si~4~Ar~4~44~40Ca~4~4~50Ti~54~5~Fe~5~6~02~0~Ni~Y~96Zr~100M~ 1 4 4 S m , 2 0 8 p b , 2 0 9 B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model parameters. 100,24 M g , a e S i , 4 ° A r , 4 ° , 4 4 , 4 ° C a , 4 °,48,50Ti,54,5°Fe,58,°6,62,o4 N i , 8 9 y , 9 0 Z r 98,100Mo,144Sm, 2°sPb,2°°Bi deduced point nucleon distribution. PRVCA 26 9 4 4 . R A D I O A C T I V I T Y 55Co,57Ni,60,°lCu,S2,SaZn; m e a s u r e d ET,IT,T1/2. 5°,57,56C0; m e a s u r e d E7,17. I J A R A 33 533. NUCLEAR REACTIONS S e N i ( a , p n ) , E = 2 4 - 4 0 MeV: m e a s u r e d E T , I T ( 0 ) , 7 7 - c o i n , D S A . 60Cu d e d u c e d high-spin levels,J,rr,T,/2,E1,E2 transition strength,7-branching. PRVCA 26 4 2 4 .

A

61Cu

=

•

NUCLEAR REACTIONS s°,52,53,54Cr,54,50,57,58Fe(p,p),(p,p'),E=5.20-6.05 MeV; m e a s u r e d a ( E ) . 51 53,54,S5Mn,55,57,ss,59Co d e d u c e d IAR. E n r i c h e d t a r g e t s . PIFLD 8 25. NUCLEAR REACTIONS e S S i , S a F e , 5 0 N i ( 3 H e , 3 H e ) , ( 3 H e , d ) , E = 9 0 MeV; 9 0 Z r ( 3 H e , a H e ) , ( 3 H e , d ) , E = 8 9 . 3 MeV; 124Sn(3He,aHe),(3He,d),E=89.8 MeV; m e a s u r e d a ( 0 ) ; d e d u c e d o p t i c a l p o t e n t i a l s . 20P,55Co, 50Cu,°lNb,lZsSb levels deduced spectroscopic factors. DWBA a n a l y s e s . Enriched,natural t a r g e t s . NUPAB 373 377. NUCLEAR REACTIONS SeNi(p,T),E=2839,3488,3550 keV; m e a s u r e d 7(0). 59Cu d e d u c e d r e s o n a n c e J, ~r,go/2 IAR f r a g m e n t a t i o n , 8 , F T , F y / F . C J P H A 60 959.

A

SONi

continued

NUCLEAR REACTIONS 16O, 24 Mg, 28$1,• 40 A r , 40 , 44 , 48 Ca, 46 , 48 , 50 T1,. 54 , 56 Fe . 58. 60 . 89 Y, 90Zr, 08 , i00 Mo, . . 62 64 N1, 1 4 4 S m , 2 0 9 p b , 2 0 0 B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(O); d e d u c e d optical model 16O, 24 Mg, 28 S1, A r , 40 , 44 , 48 Ca, 46 , 48 , 50 Tl, 54 , 56 Fe . 58. 60 parameters. . . 02 64 N1, 80 Y, 90 Zr, 98 , 100Mo, 144 S m , 2°sPb,200Bi d e d u c e d p o i n t n u c l e o n distribution. PRVCA 26 9 4 4 . •

50Co

58

KEYWORDS

=

62

NUCLEAR REACTIONS 51V,SS,6°,SaNi,SSZn,9°,sz,94,9°Zr,92,94,ss,98,1°°Mo,'2°,la4Sn,i4°Ce(p,p'),E=200 MeV; m e a s u r e d a(O). 51V,SS,6°,SaNi,68Zn,9°,92,94,gSZr,92,94,ss,98,'°°Mo,i2°,124Sn,14°Ce d e d u c e d resonances,F,T,M1 character. NUPAB 3 8 8 1. NUCLEAR REACTIONS i ~ 2 4 M g ' 2 ~ S i ' ~ A r ' 4 ~ 4 4 ' 4 ~ a ~ 4 s ~ 4 ~ 5 o T i ~ 5 4 ' ~ F e ~ 5 ~ 6 ~ 6 z ' 6 4 N i ' ~ 9 Y ' ~ o Z r ~ ' ~ o o M ~ 1 4 4 S m , e ° s P b , a ° S B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(O); d e d u c e d optical model parameters. 160,24 M g , 2 8 S i , 4 ° A r , 4 0 , 4 4 , 4 0 C a , 4 6 , 4 0 , 5 ° T i , 5 4 , 5 S F e , 5 0 , 6 0 , 6 2 , 6 4 N i , s S y , ° ° Z r , ° S , l ° ° M o , 1 4 4 S m , a°sPb,2°SBi d e d u c e d p o i n t n u c l e o n distribution. P R V C A 26 9 4 4 . R A D I O A C T I V I T Y SSCo,STNi,S°,°lCu,Sa,S3Zn; m e a s u r e d E ' / , I T , T I / 2 . 50,57,58Co; I J A R A 33 533.

28

measured

EV,17.

KEY

NUMBERS

AND

A

S3Cu

R

82Se06

63Zn

D

82Gr10

R 82Pa01

R

8ESal9:

64Zn

R 8ZBelS:

R

82Se06:

SSGa

R

81Ra23: 83RaII:

R 81Zh07

83C102

82Na06

,~SGe

R 8~So04

R 82Be37

6aZn

R 82Dj04

6aGe

R

82Ba42 82Pa03

R 82Ga08

65

=

66

=

68

NUCLEAR REACTIONS 7°Zn(~dC,160),E=72 MeV; m e a s u r e d cr(0). BSNi d e d u c e d levels,J,w, quasimagie configuration. DWBA a n a l y s i s . PYLBB 113 279. NUCLEAR REACTIONS 51V,Se,6°,62Ni,SSZn,9°,o2,9%96Zr,O2,94,96,gs,1°°Mo,~Z°,124Sn,14°Ce(p,p'),E=200 MeV; m e a s u r e d or(0). 51V,58,s°,62Ni,68Zn,9°,92,94,96Zr,92,94,96,9s,l°°Mo,lZ°,l~4Sn,14°Ce deduced resonanees,F,T,M1 character. N U P A B 388 1. NUCLEAR REACTIONS 5aNi(lUC,2p),E=40 MeV; m e a s u r e d ET,Iv,77(0,H). 68Ge l e v e l s d e d u c e d g. Recoil into gas technique. JPHGB 8 1397. NUCLEAR REACTIONS 64Zn(TLi,xnp),E=15-18 MeV; m e a s u r e d E7,Iv(0),DSA. usfigGe d e d u c e d levels, J,~r,6,Tl/z,v-branching, Enriched t a r g e t , G e ( L i ) d e t e c t o r . P R V C A 25 350.

A

69Zn

=

NUCLEAR REACTIONS e3Cu(c~,pv),E=16.7 MeV; m e a s u r e d E~/,Iv,DSA,pv-coin. 6eZn l e v e l s d e d u c e d T t / a . I A N F A 45 1879. NUCLEAR REACTIONS 55Mn(14N,n2p),E=47 MeV; 56Fe(160,2p),E=46 MeV; m e a s u r e d ET,I~/,reeoil. 86Zn,7°Ge d e d u c e d T1/2,B(M1),B(E2). N a t u r a l targets,Ge(Li) detectors,plunger. NUPAB 386 367. NUCLEAR REACTIONS 68Zn,9°,93,94Zr,94,96,go,l°°Mo,124Te,138Ba,142Ce,146Nd,15°Sm,a3~Th(p,t),E=52 MeV; m e a s u r e d a(Et,O). 66Zn,9°,9~Zr,92,94,96Mo,14OCe,144Nd,14SSm,~3°Th d e d u c e d d e e p t w o - h o l e states, Enriched t a r g e t s , N U P A B 376 513. NUCLEAR REACTIONS 5SNi(mB,np),E=31 MeV; m e a s u r e d E T , I v , 7 ( 0 ) , o r i e n t e d n u c l e i . 66Ge d e d u c e d levels,J,~r,7-branching,rotational bands. Two-quasipartiele plus rotor model,interacting boson approximation calculations. P R V C A Z5 1575.

A

~8Ni

64

NUCLEAR REACTIONS 6 3 , 6 5 C u ( e , e ) , E = 4 0 - 9 0 MeV; m e a s u r e d o r , m a g n e t i c f o r m f a c t o r s . 63,65Cu deduced magnetic oetupole moment. Shell model,core polarization,meson exchange effects. Z P A A D 307 2 4 7 . NUCLEAR REACTIONS 64Zn(p,p),E=2.88-5.02 MeV; m e a s u r e d or(O). 85Ga d e d u c e d r e s o n a n c e s , J , ~ , IAR,Coulomb energy difference,s-wave strength function. R-matrix a n a l y s i s . HPACA 54 326. NUCLEAR REACTIONS S d Z n ( p , p ' 7 ) , E = 3 . 2 4 - 3 . 2 6 MeV; m e a s u r e d E%I7,7(0). SSGa d e d u c e d IAR,J,Tr, (PpFv/F),-y-branching,B(k),configuration. C J P H A 60 815.

A

66Zn

=

NUCLEAR REACTIONS IBO,24Mg,28Si,4°Ar,4°,44,dSCa,46,48,5°Ti,54,56Fe,58,6°,62,64Ni,agY,9°Zr,gS, l°°Mo, 144Sm,Z°sPb,~egBi(polarized p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(0); d e d u c e d optical model parameters. ~4Mg~BSi~4~Ar~4~44~4~Ca~46~48~5~Ti~54'56Fe~58~6~6a~64Ni~9Y~9~Z~98~M~ 144Sin , aeepb,a°gBi deduced point nucleon distribution. P R V C A 36 9 4 4 . NUCLEAR REACTIONS ~ ° N i ( ~ 6 0 , t ~ C ) , E = 6 0 MeV; ~ ° N i ( l e O , ~ O ) , ~ Z n ( ~ C , t ~ C ) , E = 4 5 , 5 4 , 6 0 MeV; measured a(E(laC)),cr(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . SCZn l e v e l s d e d u c e d r e l a t i v e S. E x a c t f i n i t e - r a n g e DWBA a n a l y s i s , a l p h a cluster transfer. Z P A A D 305 235.

A

65Cu

63

NUCLEAR REACTIONS ~3,SSCu(e,e),E=40-90 MeV; m e a s u r e d a,magnetic f o r m f a c t o r s . 63,65Cu deduced magnetic oetupole moment. Shell model,core polarization,meson exchange effects. Z P A A D 307 2 4 7 . R A D I O A C T I V I T Y 55Co,STNi,se,SlCu,Sa,63Zn; m e a s u r e d EV,17,T~/a. 5%s~,5~C0; m e a s u r e d E7,I7. I J A R A 33 533. NUCLEAR REACTIONS ~3Cu(p,n),E=5-7.8 MeV; ~ n e a s u r e d Ev,lo,(0),VT-coin. e~Zn d e d u c e d levels,J, ~r,Tl/~,6,B(k),7-branching r a t i o s . Ge(Li) d e t e c t o r , e n r i c h e d t a r g e t . P R V C A 25 155.

A

64Ni

=

KEYWORDS

=

69

NUCLEAR REACTIONS 68Zn(n,n),E=10-380 keY; 6SZn(n,7),E=2.5-130 keY: m e a s u r e d or(total), ~(capture) vs E. Sgzn deduced resonances,J,Tr,Fn,FT,s-,p-,d-wave level spacings,strength f u n c t i o n s , n - , 7 - c h a n n e l correlation coefficient. PRVCA 35 1808.

39

KEY

NUMBERS

A 69Ga

R 82Ba25

69Ge

D 81Sel5

R 8gPa03 ~gAs

R 781v03

R 79Ne09 82Be13

83C103:

82Va08: 7OSe

R 82An09:

D 80Joll:

7*Se

D 82Ha33:

7~Br

D 82Ha33:

R 83Be13:

82Va08: 82We03:

72Se

R 82An09:

7ZBr

R 82Ga06: 82Ga22:

continued

=

70

=

71

R A D I O A C T I V I T Y 3SK(IT) [ f r o m Z4Mg(160,np),E=38 MeV3; Z4Na(IT) [ f r o m a3Na(d,p),E=4 MeV3; 77Se(IT) [ f r o m 7 4 G e ( a , n ) , E = 1 6 MeV3; 71Ge(EC) [ f r o m 7UGe(d,p),E=6 MeV3; 73As(EC),VTAs(fl-) [from 72,76Ge(d,n),E=6,7 MeV3; m e a s u r e d Tl/2. O n - l i n e c o m p u t e r i z e d d i g i t i z e r . NUIMA 178 581. R A D I O A C T I V I T Y 71Br [ f r o m 4°Ca(35C1,2n3p),mass separation3; measured Tl/2,ET,IT,77-coin. ViSe d e d u c e d levels,Tl/z,transition,possible J,~r,7-multipolarity. Oe(Li),Ge detectors. N U P A B 383 109. R A D I O A C T I V I T Y 71Br [ f r o m 4°Ca(35C1,2n3p),mass separation3; measured Tl/z,ET,IT,77-coin. 71Se d e d u c e d levels,T1/2,transition,possible J,~r,7-multipolarity. Ge(Li),Ge detectors. N U P A B 383 109.

A 72Ge

69

NUCLEAR REACTIONS 6 8 Z n ( ( x , 3 n ) , E = 2 3 MeV; m e a s u r e d I(ce). 7°Ge l e v e l s d e d u c e d J,Tr,ICC. Mini-orange spectrometers. NUIMA 164 5 3 9 . NUCLEAR REACTIONS 7z,74,76Ge(p,t),E=13 MeV; m e a s u r e d a(O). 7°,72,74Ge l e v e l s d e d u c e d normalization factor. Sub-Coulomb energies,zero-range coupled-channels calculation. PYLBB llO 199. NUCLEAR REACTIONS 55Mn(14N,n2p),E=47 MeV; SSFe(160,2p),E=45 MeV; m e a s u r e d E%IT,recoil. n~Zn,V°Ge d e d u c e d T1/a,B(M1),B(E3 ). N a t u r a l targets,Ge(Li) detectors,plunger. NUPAB 386 367. NUCLEAR REACTIONS 74,76,vs,a°,S2Se(d,SLi),E=45 MeV, m e a s u r e d (7(E(SLi),0). 70,Ta,74,76,78Ge l e v e l s d e d u c e d Sc(,L,J,~r. M a g n e t i c s p e c t r o g r a p h , enriched t a r g e t s . NUPAB 379 239. NUCLEAR REACTIONS Fe,59Co,6°Ni,63,65Cu,89Y,O°,91,9aZr,93Nb,95Mo(160,xnyp),E=56,64 MeV. Fe,59Co, 6°Ni,63,65Cu,SgY,g°,9~,gZZr,9~Nb,95Mo(~ZC,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t),centroid shifts. 7°,72,74,76Se,74,76,78Kr,l°°,l°2,1°4pd,l°4,106,l°8Cd d e d u c e d yrast cascade delay times. ~°sCd d e d u c e d i s o m e r s , T ~ / ~ . PYLBB 113 209.

A 7~Ge

=

KEYWORDS

NUCLEAR REACTIONS 64Ni(VLi,3n),E=14-18 MeV; m e a s u r e d 77-coin,IT,ET,7(0),DSA. SgGa d e d u c e d levels,J,~r,8,7-branehing,band structure. Enriched target,Ge(Li) detectors. P R V C A 25 2947. R A D I O A C T I V I T Y 69Ge [ f r o m 5SFe(160,n3p),E=56 MeV]; ll3Sn [ f r o m l°°Mo(~e0,3n),E=56 MeV]; measured 7(0,H,T); d e d u c e d quadrupole interaction constants f o r Ge i n T I , S n i n S n . Recoil implantation. ZPBBD 4 5 29. NUCLEAR REACTIONS e¢Zn(TLi,xnp),E=15-18 MeV; m e a s u r e d E%IT(0),DSA. 6e,6gGe d e d u c e d levels, J,~,6,Tt/z,7-branching. Enriched t a r g e t , G e ( L i ) d e t e c t o r . P R V C A 25 350. NUCLEAR REACTIONS 5SNi(14N,n2pT),E=47.5 MeV; m e a s u r e d ET,IT,recoil d i s t a n c e s . 69As l e v e l s deduced J,~r,Ti/~,7-multipolarity. Enriched t a r g e t , G e ( L i ) d e t e c t o r . PIFLD 8 54.

A 7OGe

AND

=

72

NUCLEAR REACTIONS 7u,Ta,VSGe(p,t),E=13 MeV; m e a s u r e d ~ ( 0 ) . 7°,72,74Ge l e v e l s d e d u c e d normalization factor. Sub-Coulomb energies,zero-range coupled-channels calculation. PYLBB 110 199. NUCLEAR REACTIONS 74,7%7s,8°,SaSe(d,SLi),E=45 MeV, m e a s u r e d a(E(SLi),0). 7°,72,74,76,78Ge levels deduced Sa,L,JJr. Magnetic spectrograph, enriched t a r g e t s . NUPAB 379 239. NUCLEAR REACTIONS 7 2 G e ( p , p ' e ) , E = 3 - 4 . 3 4 MeV; m e a s u r e d p'e-coin,I(ce)(t),a(E). 7ZGe l e v e l d e d u c e d Tt/a. 73As d e d u c e d IAR. P u l s e d b e a m , l a r g e s o l i d a n g l e e l e c t r o n d e t e c t o r . NUIMA 192 273. NUCLEAR REACTIONS Fe,SOCo,~aNi,63fiaCu,SgY,9°,9~,~2Zr,93Nb,gSMo(~60,xnyp),E=56,64 MeV. Fe,59Co, 6°Ni,63,SaCu,SOY,Oa,ol,OZZr,93Nb,95Mo(~2C,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t),centroid shifts. 7°,7~,74,76Se,7¢,76,78Kr,l°°,l°2,1°4pd,l°a,l°6,1°sCd d e d u c e d yrast cascade delay times. l°sCd d e d u c e d i s o m e r s , T 1 / 2 . PYLBB 113 209. NUCLEAR REACTIONS 5SNi(160,np),E=40-55 MeV; m e a s u r e d E7,17,IT(t),I7(0),77(t). 72Br d e d u c e d levels,Jjr. Enriched t a r g e t , G e ( L i ) d e t e c t o r . P R V C A 25 1396. NUCLEAR REACTIONS 58Ni(160,np),E=50 MeV; m e a s u r e d DSA,recoil,ET. 72Br l e v e l s d e d u c e d T1/2, 7-branching,B(E2). P R V C A 26 1748.

30

KEY

AND

NUMBERS

A

73Ge

R 81Ch41

73As

D 8OJoll

81Ma37 R 82We03

R 82Be13

82Ta16 82Va08 74Se

R 82An09

74Kr

R 82An09:

R 83Is07:

75As

D 82Ha37: R 8OJoll:

75Se

D 82Ha37: R 81En07: 82Fa08:

D 82Be20:

R 82Va08: 76Se

R 81Ma39:

82An09:

76BF

R 82Do11:

74

=

75

NUCLEAR REACTIONS 74Ge(d,p3/),E=6 MeV; m e a s u r e d E % I T , T l / a , p T - c o i n . 7SGe d e d u c e d level,JjT, ICC,B(M1),B(E2). E n r i c h e d t a r g e t , G e ( L i ) d e t e c t o r . N U P A B 380 438. R A D I O A C T I V I T Y 1311,75Se; m e a s u r e d E%IT,-/~-coin. 131Xe,7SAs l e v e l s d e d u c e d ~ - b r a n c h i n g . S u m coincidence spectometer. NUIMA 198 305. NUCLEAR REACTIONS 74Ge(d,n),E=7 MeV; m e a s u r e d 7 7 - c o i n . VSAs level d e d u c e d TI/2. O n - l i n e computerized d i g i t i z e r . NUIMA 178 581. R A D I O A C T I V I T Y 131I,TSSe; m e a s u r e d E % I % 7 7 - c o i n . 131Xe,TSAs l e v e l s d e d u c e d 7 - b r a n c h i n g . S u m coincidence spectometer. NUIMA 198 305. NUCLEAR REACTIONS 7 4 , 7 6 , 7 7 , 7 8 , 8 ° S e ( n , 7 ) , E - t h e r m a l , r e s o n a n c e ; measured E7,I% 75,77,78,81Se deduced neutron separation e n e r g i e s , Q . 75,77,78,79,8iSe d e d u c e d l e v e l s , J J r . NUPAB 372 125. NUCLEAR REACTIONS aaMo,gOzr,8%r,74Se(n,2n),(%n),E=14.5 MeV; m e a s u r e d a ( i s o m e r ) / a ( g r o u n d s t a t e ) . 9aMo,atZr,87Sr,TSSe d e d u c e d level density spin dependence parameter. Compound nucleus decay calculations. Y A F I A 35 257.

A 76Ge

=

NUCLEAR REACTIONS 7a,74,76Ge(p,t),E=13 MeV; m e a s u r e d or(O). 7°,Ta,7¢Ge l e v e l s d e d u c e d normalization factor. Sub-Coulomb energies,zero-range coupled-channels calculation. PYLBB 110 199. NUCLEAR REACTIONS 7 4 G e ( p , p ' ) , E = 2 2 MeV; m e a s u r e d a ( E , 0 ) . 74Ge d e d u c e d levels,L,J,~. Enriched target,magnetic spectrometer. DWBA,CCBA c a l c u l a t i o n s . NUPAB 385 430. NUCLEAR REACTIONS 74,76,TS,8°,aaSe(dfiLi),E=45 MeV, m e a s u r e d ~ ( E ( e L i ) , 0 ) . v°,Ta,74,76,TSGe l e v e l s d e d u c e d Sa,L,J,Tr. M a g n e t i c s p e c t r o g r a p h , enriched t a r g e t s . NUPAB 379 239. NUCLEAR REACTIONS Fe,59Co,8°Ni,63f15Cu,BgY,9°,gi,9aZr,93Nb,O5Mo(~60,xnyp),E=56,64 MeV. Fe,5OCo, 6eNi,ea,65Cu,SgY,O°,gi,gaZr,gUNb,O5Mo(taC,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t),centroid shifts. 7°,7~,74,TSSe,74,Te,78Kr,l°6,1°2,1°4pd,l°4,1°6,1°sCd d e d u c e d yrast cascade delay times. ~°6Cd d e d u c e d i s o m e r s , T ~ / 2 . PYLBB 113 209. NUCLEAR REACTIONS Fe,SgCo,6ONi,63,SSCu,Say,g°,9~,aaZr,aaNb,aSMo(~60,xnyp),E=56,64 MeV. Fe,SaCo, 6°Ni,63,65Cu,89y,9°,9~,gazr,gaNb,aSMo(~aC,xnyp),E=48 MeV; m e a s u r e d E-/,IT,~(t),centroid shifts. 7°,72,74,76Se,74,76,78Kr,l°°,l°a,l°4pd,164,1°6,1°8Cd d e d u c e d yrast cascade delay times. l°6Cd d e d u c e d i s o m e r s , T t / ~ . PYLBB 113 209.

A

75Ge

73

NUCLEAR REACTIONS 74Ge(n,2n),E=14.4 MeV; m e a s u r e d p r o d u c t i o n cr f o r 73raGe. 7aGe d e d u c e d a(isomer)/a(ground state). Activation technique. R R A L A 4 9 199. R A D I O A C T I V I T Y aSK(IT) [ f r o m a4Mg(leO,np),E=38 MeV3; a4Na(IT) [ f r o m e3Na(d,p),E=4 MeV]; 77Se(IT) [ f r o m 7 4 G e ( a , n ) , E = 1 6 MeVS; 7tGe(EC) [ f r o m 7 ° G e ( d , p ) , E = 6 MeV]; 73As(EC),77As(fl-) [from 7z,7~Ge(d,n),E=6,7 MeV]; m e a s u r e d T~/z. 0 n - l i n e computerized d i g i t i z e r . NUIMA 178 581. R A D I O A C T I V I T Y 73As; m e a s u r e d a c t i v i t y ; d e d u c e d c h e m i c a l s t a t e e f f e c t s . IANFA 45 1852. NUCLEAR REACTIONS 7 Z G e ( p , p ' e ) , E = 3 - 4 . 3 4 MeV; m e a s u r e d p'e-coin,I(ce)(t),a(E). 7aGe l e v e l d e d u c e d T~/a. 73As d e d u c e d IAR. P u l s e d b e a m , l a r g e s o l i d a n g l e e l e c t r o n d e t e c t o r . NUIMA 192 273.

A

74Ge

=

KEYWORDS

=

76

R A D I O A C T I V I T Y Nd,Mo,Ge; m e a s u r e d E7,I7; d e d u c e d n o e v i d e n c e f o r n e u t r i n o l e s s process, r i g h t h a n d e d c u r r e n t f r a c t i o n l i m i t s , t4s,15°Nd,aa,l°°Mo d e d u c e d l i m i t o n d o u b l e f l - d e c a y T1/ 3. 76Ge d e d u c e d l i m i t o n n e u t r i n o l e s s d o u b l e f l - d e c a y T j / a . NCLTA 33 273. NUCLEAR REACTIONS 74,76,TS,8°,aZSe(d,SLi),E=45 MeV, m e a s u r e d cr(E(6Li),O), v°,Ta,74,76,TaGe levels deduced Sa,L,J,~. Magnetic spectrograph, enriched t a r g e t s . N U P A B 379 239. NUCLEAR REACTIONS 74,76Ge(a,3n),E=27 MeV; m e a s u r e d 73,(t),7(0),linear polarization. 76Se deduced level,J,wp/-multipolarity. Compton polarimeter,high p u r i t y Ge d i o d e s . NUIMA 188 63. NUCLEAR REACTIONS Fe,5aCo,6°Ni,63,6fiCu,89y,9°,91,a2Zr,93Nb,a~Mo(160,xnyp),E=56,64 MeV. Fe,59Co, 6°Ni,ea,eScu,a9y,9°,gt,gaZr,93Nb,aSMo(~aC,xnyp),E=48 MeV; m e a s u r e d E~/,l~/,3~(t),centroid shifts. 7°,T2,74,76Se,74,76,TaKr,l°°,l°2,1°4pd,l°4,1°6,1°8Cd d e d u c e d yrast cascade delay times. to6Cd d e d u c e d i s o m e r s , T 1 / 2 . PYLBB 113 209. NUCLEAR REACTIONS 7 4 S e ( a , n p ) , E = 2 7 MeV; 7 6 s e ( a H e , 3 n p ) , E = 3 2 MeV; 7 a S e ( d , 2 n ) , E - 1 3 . 5 MeV; W S e ( p , n ) , E - 6 . 7 MeV; m e a s u r e d ET,IT,~/7-coin,cr(ET),~/(0),linear polarization. 76Br d e d u c e d Ievets,J,Tr,isomer Tl/a,7-branching,rotational bands,configurations,B(M1)/B(E2). Cranked s h e l l m o d e l a n a l y s i s . Z P A A D 305 365.

31

KEY

NUMBERS

AND

A 7SBr

R 82Wo06:

~SKr

D 82Mo10:

R 82AnO9 :

82Ke01:

82Ma18:

82Pi01: 7SRb

D 8EMol0:

D 80Jo11:

77Se

D 80Joll:

R 81EnO7: 77KF

D

82Mo10:

77Rb

D

82Mo10:

77Sr

R 82Li08:

R 82Va08:

78As

D 82Si07:

7SSe

D 82Si07: R 81En07:

78Br

R 82Be03:

78Kr

R 82An06: 82An09:

continued

=

77

RADIOACTIVITY aSK(IT) [ f r o m a4Mg(lSO,np),E=38 MeV]; SaNs(IT) [ f r o m 2aNa(d,p),E=4 MeV]; 77Se(IT) [ f r o m 74Ge(a,n),E=16 MeV]; 71Ge(EC) [ f r o m 7°Ge(d,p),E=6 MeV]; 73As(EC),77As(fl-) [ f r o m 7z,78Ge(d,n),E=6,7 MeVa; m e a s u r e d T,/2. O n - l i n e c o m p u t e r i z e d d i g i t i z e r . NUIMA 178 581. RADIOACTIVITY aSK(IT) [ f r o m 24Mg(lSO,np),E=38 MeV]; 24Na(IT) [ f r o m 2aNa(d,p),E=4 MeV]; 77Se(IT) [ f r o m 74Ge(a,n),E=16 MeVa; 71Ge(EC) [ f r o m 7°Ge(d,p),E=6 MeV]; 73As(EC),77As(fl-) [ f r o m 72,TaGe(d,n),E=6,7 MeV]; m e a s u r e d TI/2. 0 n - l i n e c o m p u t e r i z e d d i g i t i z e r . NUIMA 178 581. NUCLEAR REACTIONS 74,Ts,77,~s,a0Se(n,7),E=thermal,resonanee; m e a s u r e d E7,I7. 75,77,78,81Se d e d u c e d n e u t r o n s e p a r a t i o n e n e r g i e s , Q . 75,77,78,79,81S e d e d u c e d levels,J,rr. NUPAB 372 125. RADIOACTIVITY 77,76Rb [ f r o m S°Ni(a°Ne,xnp)],77Kr [ f r o m 77Rb decay]; m e a s u r e d fl7-,T~-coin, f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q(EC). 7SRb l e v e l d e d u c e d J,vr. 7SKr l e v e l d e d u c e d J,Tr, 7 - b r a n c h i n g . PYLBB 113 16. RADIOACTIVITY 77,~6Rb [ f r o m S°Ni(a°Ne,xnp)],77Kr [ f r o m 77Rb decay]; m e a s u r e d flT-,72-coin, f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q(EC). 7SRb l e v e l d e d u c e d J,rr. 78Kr l e v e l d e d u c e d J,Tr, 7 - b r a n c h i n g . PYLBB 113 16. NUCLEAR REACTIONS 5SNi(24Mg,xnyp),E=100 MeV; 4°Ca(4°Ca,xnyp),E=ll7 MeV; 5aNi(2SSi,xnyp), (29Si,xnyp),4°ca(aaK,xnyp)77Sr/TaSr/TaSr/a°Sr/,E not given; measured ET,IT,Tnn-, 7 n ( p a r t i e l e ) - c o i n , r e c o i l , - y ( O ) . 77Sr deduced l e v e l s , p o s s i b l e J , T r , 7 - b r a n c h i n g ' 7s,vs,S0Sr d e d u c e d l e v e l s , T 1 / z , p o s s i b l e j , T r , ~ , 7 - b r a n c h i n g , q u a d r u p o l e m o m e n t . PRLTA 49 308.

A

78Ge

76

NUCLEAR REACTIONS 7s,so,S2Se(p,n),E=19,20,22,25 MeV; m e a s u r e d ~(En),cr(0). 7s,ao,aeBr d e d u c e d a n a l o g e x c i t a t i o n m e c h a n i s m . C o u p l e d - c h a n n e l s c a l c u l a t i o n . PRVCA 26 889. RADIOACTIVITY ~7,76Rb [ f r o m S°Ni(2ONe,xnp)]77Kr [ f r o m 77Rb decay]; m e a s u r e d flT-,77-coin, f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q(EC). 7SRb l e v e l d e d u c e d J,Tr. 76Kr l e v e l d e d u c e d J,Tr, 7 - b r a n c h i n g . PYLBB 113 16. NUCLEAR REACTIONS Fe,~SCo,SONi,Sa,SSCu89y,SO,91,SZZr,S3Nb,SSMo(lSO,xnyp),E=56 64 MeV. pe,59Co, S°Ni'Sa'65Cu,SSY,aO,sl,SaZr,SaNb,95Mo(laC,xnyp),E=48 MeV; m e a s u r e d E7,I7,7(t),centroid s h i f t s . 76,Ta,74,TSSe,74,76,TaKr,160,l°2,1°4pd,104,106,1oSCd d e d u c e d y r a s t c a s c a d e d e l a y t i m e s . ~°6Cd d e d u c e d i s o m e r s T , / 2 . PYLBB 113 209. NUCLEAR REACTIONS SaCu(ISF,2na),E=58 MeV; m e a s u r e d recoil. 27AlS4SSZnT0727476Ge(a2Kr S2Kr'),(S4Kr,a4Kr'),E=ll5,118 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , a ( E ) , D S A ; d e d u c e d s t o p p i n g p o w e r f o r Kr i n A1,Zn,Ge,Ge i n Ge,Zn in Zn. 7s,s2,a4Kr level d e d u c e d B(E2),TI/2. NUPAB 376 246. NUCLEAR REACTIONS 7s,a°,az,a4Kr(p,t),E=51.9 MeV; m e a s u r e d a(0). 7s,Ta,so,S2Kr d e d u c e d octupole state splittings,enhancement f a c t o r s DWBA a n a l y s i s , i n t e r a c t i n g b o s o n m o d e l . PYLBB 113 El. NUCLEAR REACTIONS 6SZn(leC,2n),E=39 MeV; m e a s u r e d E T , I 7 , 7 ( 0 ) , r e c o i l , D S A , 7 7 - c o i n . 76Kr d e d u c e d l e v e l s , J , T r , B ( E E ) , ~ , 7 - b r a n c h i n g , r o t a t i o n a l b a n d s . PRVCA 25 1941. RADIOACTIVITY 77,76Rb [ f r o m S°Ni(a°Ne,xnp)],77Kr [ f r o m 77Rb decay]; m e a s u r e d f17-,77-coin, f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q(EC). 7SRb l e v e l d e d u c e d J,rr. 7aKr l e v e l d e d u c e d J,rr, 7 - b r a n c h i n g . PYLBB 113 16.

A

77As

=

KEYWORDS

=

78

NUCLEAR REACTIONS 74,7s,vs,s°,SZSe(d,SLi),E=45 MeV, m e a s u r e d a(E(SLi),0). 70,72,74 76 78Ge l e v e l s d e d u c e d Sa,L,J,~r. M a g n e t i c s p e c t r o g r a p h , e n r i c h e d t a r g e t s . NUPAB 379 239. RADIOACTIVITY 7SAs [ f r o m 78Se(n,p)]; m e a s u r e d E T , I T , 7 7 - c o i n . 78Se d e d u c e d levels,B(E2) r a t i o s . E n r i c h e d 7SSe target,Ge,Ge(Li) d e t e c t o r s . PRVCA 25 2003. RADIOACTIVITY 7SAs [ f r o m 7SSe(n,p)3; m e a s u r e d ET,17,77-coin. 78Se d e d u c e d levels,B(E2) r a t i o s . E n r i c h e d 7SSe target,Ge,Ge(Li) d e t e c t o r s . PRVCA 25 2003. NUCLEAR REACTIONS 74 .76 . . . 77 78 80 S e ( n , 7 ) , E = t h e r m a l , r e s o n a n e e ; m e a s u r e d E7,I7. 75,777s,alSe d e d u c e d n e u t r o n s e p a r a t i o n e n e r g i e s , Q . 75,77,78,79,81Se d e d u c e d levels,J,Tr. NUPAB 372 125. NUCLEAR REACTIONS 77Se(a,EnpT),E=40-50 MeV; m e a s u r e d a(E,ET),ET,I%I7(0,t),77-eoin" 78Br d e d u c e d l e v e l s , J , T , / a . E n r i c h e d t a r g e t s . NUPAB 376 131. NUCLEAR REACTIONS 7SSe(a,2n),E=27 MeV; 6SZn(12C,2n),E=36 MeV; m e a s u r e d ET,IT,DSA,7~-eoin. 7SKr d e d u c e d l e v e l s , T l / u , J , ~ r , r o t a t i o n a 1 b a n d s , 7 _ b r a n c h i n g " IANFA 46 30. NUCLEAR REACTIONS Fe,SSCo,SONi,Sa,SSCu,aay,sO,a*,O2Zr,SaNb,a~Mo(160,xnyp),E=56,64 MeV. Pe,SaCo, S°Ni,Sa,SSCu,aSY,9O,sl,SaZr,93Nb,SSMo(12C,xnyp),E=48 MeV; m e a s u r e d E7,IT,7(t),centroid shifts. 70,72,74,76Se,74,76,78Kr,*OO,102,104pd,1041061oSCd deduced yrast cascade delay times. ~°sCd d e d u c e d i s o m e r s , T 1 / 2 . PYLBB 113 209.

32

KEY

NUMBERS

A 7SKr

R 82Ma18

7OSr

R 82Li08

R 81En07

79Kr

R 82Be48

88Bu01 88Pa20 79Rb

D 8~De36

R 82Ba33

82Pa20:

88Th03: 79Sr

D 8~De36:

R 82Li08:

=

78

KEYWORDS

continued

NUCLEAR REACTIONS 78,8°,ez,a4Kr(p,t),E=51.9 MeV; m e a s u r e d or(0). 7S,Te,S°,SZKr d e d u c e d oetupole state splittings,enhaneement f a c t o r s . DWBA a n a l y s i s , i n t e r a c t i n g b o s u n m o d e l . PYLBB 113 21. NUCLEAR REACTIONS 58Ni(adMg,xnyp),E=100 MeV; 4°Ca(4°Ca,xnyp),E=I17 MeV; 5SNi(~SSi,xnyp), (ZOSi,xnyp),d°Ca(~VK,xnyp)~TSr/78Sr/~OSr/S°Sr/,E n o t g i v e n ; m e a s u r e d ET,I~/,Tnn - , 7 n ( p a r t i c l e ) - c o i n , r e c o i l , ~ / ( 0 ) . VTSr d e d u c e d l e v e l s , p o s s i b l e J J r , T - b r a n c h i n g . vs,7~,S°Sr d e d u c e d l e v e l s , T w a , p o s s i b l e J , r r , 8 , T - b r a n c h i n g , q u a d r u p o l e m o m e n t . PRLTA 49 308.

A 79Se

AND

=

79

NUCLEAR REACTIONS 74,76,77,Te,8°Se(n,7),E=thermal,resonance; m e a s u r e d E~/,17. 75,77,Ts,SlSe d e d u c e d n e u t r o n s e p a r a t i o n e n e r g i e s , q . ~5,~7,Ts,Ts,elSe d e d u c e d levels,J,Tr. NUPAB 372 125. NUCLEAR REACTIONS 78Se(a,3n),E=30-55 MeV; m e a s u r e d a(E%E),7(0),ET,lT,'yT-coin. ~SKr deduced levels,J,rotational band,6,branching ratios,(g(k)-g(R)/Oo) 2. Q u a s i p a r t i c l e p l u s r o t o r m o d e l . E n r i c h e d t a r g e t s . PRVCA 26 1417. NUCLEAR REACTIONS 7SKr(polarized d , p ) , ( p o l a r i z e d d,d),E=ll MeV; m e a s u r e d cr(e),A(0). 7~Kr d e d u c e d l e v e l s , J J r , S . E n r i c h e d t a r g e t . DWBA,optical m o d e l a n a l y s e s . NUPAB 377 i05. NUCLEAR REACTIONS 63Cu(tgF,3np),(tgF,ndp),E-46-62 MeV; 7°Ge(12C,3np),E=33-48 MeV; m e a s u r e d E ( T ) , l ( E ( T ) ) , 7 ( 0 ) , r e c o i l , D o p p l e r s h i f t , D S A . 79Rb,79Kr d e d u c e d l e v e l s , J , T r , T l / a . E n r i c h e d t a r g e t s . A s y m m e t r i c r o t o r p l u s p a r t i c l e , i n t e r a c t i n g bosun f e r m i o n m o d e l s . NUPAB 389 434. RADIOACTIVITY 7gSr(fl÷) [ f r o m SdFe(3ZS,n3pa),5°Cr(3ZS,n2p),E=123 MeV]; m e a s u r e d 7 T - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , t o g f t . 79Rb d e d u c e d l e v e l s , J j r , l C C , T ~ / z , 7-multipolarity,T-branching. S0y(fl+) [ f r o m 54Fe(3ZS,np),E=123 MeV]; m e a s u r e d Twd,T'y-, fl~/-coin; d e d u c e d log f t , Q ( E C ) , m a s s exeess,Q(fl). S°Sr d e d u c e d levels,J,Tr,Ti/z,ICC. SlZr(fl +) [ f r o m 54Fe(adS,na),E=123 MeV]; 81y(fl+) [ f r o m 8tZr decay]; m e a s u r e d T l / 2 , f l - e n d p o i n t energies, flT-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . SlSr d e d u c e d levels,J,Tr,T1/z, 7 - b r a n c h i n g . SdZr(fl+),SdY(fl+) [ f r o m SZZr d e c a y ] ; m e a s u r e d T1/z,fl~/-coin,E~/; d e d u c e d m a s s excess. SZZr d e d u c e d Q(EC). SaSr d e d u c e d levels,J,rr,Tw2 u p p e r l i m i t , ~ / - b r a n c h i n g . S3Zr(fl+) [ f r o m 54Fe(3aS,ndp)],S3Y(fl+) [ f r o m SdFe(3ZS,3p)],S3mY(fl+) [ f r o m S3Zr decay]; m e a s u r e d T1/z,ET, 7 ( X - r a y ) , f l ~ / - , ( m a s s ) ~ / - c o i n ; d e d u c e d Q ( E C ) , m a s s e x c e s s . Say d e d u c e d levels,J,Tr,ICC, T - m u l t i p o l a r i t y , T t / 2 u p p e r l i m i t . S3Sr d e d u c e d l e v e l s . 8aZr d e d u c e d isomer,T1/a. SdZr(fl+) [ f r o m 54Fe(adS,dp)]; m e a s u r e d Tl/z,-y(X-ray)-eoin. 85Zr(fl+) [ f r o m 58Ni(32S,n4p)]; m e a s u r e d TI/ 2 , f i T - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. NUCLEAR REACTIONS 83Cu(180,X),E=40-85 MeV; 45Sc(34S,X)VTKr/TSKF/~SKr/7~Br/75Br/74Br/TaBr/TaSe/ 76Br/7°As/71As/72As/SOGe,E=85-130 MeV; m e a s u r e d E%IT; d e d u c e d p r o d u c t i o n cr v s E f o r r e s i d u a l s . 79Rb d e d u c e d f u s i o n b a r r i e r . A c t i v a t i o n t e c h n i q u e , e n r i c h e d t a r g e t . S t a t i s t i c a l m o d e l . NUPAB 384 ~11. NUCLEAR REACTIONS 63Cu(lSF,Enp),(19F,ndp),E=46-62 MeV; 7°Ge(l~C,dnp),E=33-48 MeV; m e a s u r e d E ( 7 ) , I ( E ( 7 ) ) , 7 ( 0 ) , r e c o i l , D o p p l e r s h i f t , D S A . 79Rb,79Kr d e d u c e d l e v e l s , J J r , T ~ / , . E n r i c h e d t a r g e t s . A s y m m e t r i c r o t o r p l u s p a r t i c l e , i n t e r a c t i n g bosun f e r m i o n m o d e l s . NUPAB 389 4~4. NUCLEAR REACTIONS 54,SSFe(Z~Si,xnypT),E=80-99 MeV; m e a s u r e d ET,IT,TT-coin,a(E%E),ff(E%O). 79Rb,e°,elSr d e d u c e d levels,J,rr. E n r i c h e d t a r g e t s . PRVCA 25 1325. RADIOACTIVITY 79Sr(fl+) [ f r o m 5~Fe(a~S,nEpa),5°Cr(3~S,ndp),E=lE3 MeVd; m e a s u r e d ~/'/-, (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,Tl/2, 7-multipolarity,7-branehing. 8Oy(fl+) [ f r o m 54Fe(~ZS,np),E=123 MeV]; m e a s u r e d T i / z , 7 7 - , f i T - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl), e°Sr d e d u c e d levels,J,rr,Twz,lCC, eiZr(fl +) [ f r o m S4Fe(3eS,na),E=183 MeV]; S~Y(fl+) [ f r o m S~Zr decay]; m e a s u r e d T , / z , f l - e n d p o i n t energies, flT-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d levels,J,Tr,T~/~, T - b r a n c h i n g . 8ZZr(fl+),SaY(fl+) [ f r o m SZZr d e c a y ] ; m e a s u r e d Tl/2,flT-coin,ET; d e d u c e d m a s s excess. ~UZr d e d u c e d Q(EC). ~USr d e d u c e d levels,J,~r,Ti/~ u p p e r l i m i t , T - b r a n c h i n g . 8aZr(fl +) [ f r o m 54Fe(3aS,nEp)],SUY(fl +) [ f r o m 54Fe(3eS,3p)],83my(fl+) [ f r o m S3Zr decay]; m e a s u r e d TI/z,ET, T(X-ray),fl-/-,(mass)3,-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . S~y d e d u c e d l e v e l s , J , n , I C C , T - m u l t i p o l a r i t y , T ~ / 2 u p p e r l i m i t . SaSr d e d u c e d l e v e l s , eSZr d e d u c e d isomer,T~/z. ~4Zr(fl +) [ f r o m 54Fe(3aS,Ep)]; m e a s u r e d T l / z , T ( X - r a y ) - c o i n . eSZr(fl +) [ f r o m 5SNi(3eS,n4p)]; m e a s u r e d Tl/ 2 , f i T - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. NUCLEAR REACTIONS 58Ni(~aMg,xnyp),E=i00 MeV; 4°Ca(4°Ca,xnyp),E=ll7 MeV; 5SNi(~aSi,xnyp), (egSi,xnyp),d°Ca(39K,xnyp)77Sr/78Sr/TOSr/~°Sr/,E n o t g i v e n ; m e a s u r e d E T , I T , T n n - , Tn(partiele)-coin,recoil,T(0). 77Sr d e d u c e d l e v e l s , p o s s i b l e J d r , T - b r a n c h i n g . 7e,79,8°Sr d e d u c e d l e v e l s , T w z , p o s s i b l e J , ~ T , 6 , 7 - b r a n c h i n g , q u a d r u p o l e m o m e n t . PRLTA 49 308.

33

KEY

NUMBERS

A 8OBr

R 810h09:

82Wo06: 8OKr

R 82Ma18:

SOSr

D 82De36:

R 82Li08

82Th03 SOy

D 82De36

R 8aMo04

else

R 81En07

SlKr

R 83Ko06

elRb

D 83Gr07 R 82Pa06

=

KEYW0RDS

80

NUCLEAR REACTIONS 79,81Br(n,-/),(n,X),E=0.05-10 keV; m e a s u r e d t r a n s m i s s i o n , E - / , I % 8°,e2Br d e d u c e d < F~/ > , a v e r a g e l e v e l s p a c i n g , r e s o n a n c e s , r e s o n a n c e p a r a m e t e r s , s - w a v e strength f u n c t i o n s . A r e a a n a l y s i s , M o n t e Carlo c a l c u l a t i o n . JNSTA 18 745. NUCLEAR REACTIONS 76,8o,SaSe(p,n),E=19,20,22,25 MeV; m e a s u r e d a ( E n ) , f f ( 0 ) . 76,s°,82Br d e d u c e d a n a l o g e x c i t a t i o n m e c h a n i s m . C o u p l e d - c h a n n e l s c a l c u l a t i o n . PRVCA 26 889. NUCLEAR REACTIONS 78,8°,ea,84Kr(p,t),E=51.9 MeV; m e a s u r e d if(0). 76,78,8°,SaKr d e d u c e d octupole state splittings,enhancement f a c t o r s . DWBA a n a l y s i s , i n t e r a c t i n g b o s o n m o d e l . PYLBB 113 21. RADIOACTIVITY ~gSr(fl +) [ f r o m S4Fe(aaS,n2pa),SSCr(a2S,n2p),E=123 MeV]; m e a s u r e d ~ - / - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . ~SRb d e d u c e d l e v e l s , J , ~ , I C C , T l / 2 , -/-multipolarity,7-branching. 8°Y(B*) ] - f r o m 54Fe(aaS,np),E=J23 MeV]; m e a s u r e d T1/z,7-/-, f i T - c o i n ; d e d u c e d log ft,Q(EC),mass excess,Q(fl). S°Sr d e d u c e d levels,J,Tr,Tl/2,ICC. 81Zr(fl+) [ f r o m 54Fe(aaS,na),E=123 MeV]; Sly(fl+) [ f r o m S~gr decay]; m e a s u r e d T1/a,fl-endpoint energies, f l T - , ~ / ( X - r a y ) - c o i n ; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d l e v e l s , J j r , T l / z , - / - b r a n c h i n g . SZZr(fl+),82Y(fl+) [ f r o m S2Zr decay3; m e a s u r e d Tl/z,fl-/-coin,E-/; d e d u c e d m a s s e x c e s s . S2Zr deduced Q(EC). 8aSr d e d u c e d levels,J,w;T1/2 u p p e r l i m i t , 7 - b r a n c h i n g . S3Zr(fl+) [ f r o m 54Fe(aaS,n2p)l,83Y(fl +) [ f r o m 54Fe(a2S,3p)],SSmy(fl+) [ f r o m 8aZr decay]; m e a s u r e d TI/a,ET, ~(X-ray),fl-/-,(mass)2-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s , gay d e d u c e d levels,J,Tr,ICC, 7 - m u l t i p o l a r i t y , T l / z u p p e r l i m i t . 8aSr d e d u c e d l e v e l s . SaZr d e d u c e d i s o m e r , T ] / 2 , a4Zr(fl+) [ f r o m 54Fe(a2S,3p)]; m e a s u r e d T1/z,-/(X-ray)-coin. S5Zr(fl +) [ f r o m S8Ni(3aS,n4p)]; m e a s u r e d T~/ 2 , f i T - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. NUCLEAR REACTIONS 5aNi(a4Mg,xnyp),E=100 MeV; 4°Ca(4°Ca,xnyp),E=ll7 MeV; 5SNi(aaSi,xnyp), (agSi,xnyp),4OCa(agK,xnyp)V~Sr/VSSr/VSSr/S°Sr/,E not given; measured E-/,l%Tnn-, 7 n ( p a r t i c l e ) - e o i n , r e c o i l , - / ( O ) . ~TSr deduced l e v e l s , p o s s i b l e J , ~ r , 7 - b r a n c h l n g . 78,7s,S°Sr d e d u c e d l e v e l s , T 1 / a , p o s s i b l e J , r r , 6 , 7 - b r a n c h i n g , q u a d r u p o l e m o m e n t . PRLTA 49 308. NUCLEAR REACTIONS 54,56Fe(ZSSi,xnyp-/),E=80-99 MeV; m e a s u r e d E%I%7"~-coin,a(E%E),a(E%0). 79Rb,S°,SlSr d e d u c e d levels,J,rr. E n r i c h e d t a r g e t s . PRVCA 25 1325. RADIOACTIVITY VSSr(fl +) [ f r o m 54Fe(aaS,n2pa),SOCr(aaS,n2p),E=123 MeV]; m e a s u r e d 7 ~ - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 7~Rb deduced levels,J,Tr,ICC,T~/z, 7-multipolarity,'~-branching. S0y(fl+) [ f r o m 54Fe(aaS,np),E=123 MeV]; m e a s u r e d T~/a,-/7-, f l - / - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,Tr,T~/e,ICC, a~Zr(fl +) [ f r o m 5~Fe(aaS,na),E=123 MeV]; my(fl+) [ f r o m SlZr decay]; m e a s u r e d T~/a,fl-endpoint energies, f l T - , ~ ( X - r a y ) - c o i n ; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d levels,J,rr,T1/a, - / - b r a n c h i n g . SZZr(fl+),SaY(fl ÷) [ f r o m SaZr d e c a y ] ; m e a s u r e d T~/a,fl-/-coin,ET; d e d u c e d m a s s excess. SaZr d e d u c e d Q(EC). SZSr d e d u c e d levels,J,Tr,T~/z u p p e r l i m i t , 7 - b r a n c h i n g . S3Zr(fl+) [ f r o m 54Fe(3aS,nap)],~3Y(fl +) [ f r o m 5~Fe(aZS,3p)],samY(fl÷) [ f r o m 83Zr decay]; m e a s u r e d T1/a,E-/, 7(X-ray),fl-/-,(mass)7-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . Say d e d u c e d levels,J,rr,ICC, ~ / - m u l t i p o l a r i t y , T ~ / a u p p e r l i m i t . SaSr d e d u c e d l e v e l s . 83Zr d e d u c e d isomer,T~/e. S4Zr(fl +) [ f r o m 54Fe(aZS,2p)J; m e a s u r e d T~/a,-/(X-ray)-coin. a5Zr(fl +) [ f r o m 5SNi(aaS,n4p)]; m e a s u r e d T~/ 2,fl-/-coin; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305.

A aJAs

AND

=

81

NUCLEAR REACTIONS 8aSe(t,a),E=18 MeV; m e a s u r e d •(Ea),cr(O). SlAs d e d u c e d levels,L,J,rr,S. E n r i c h e d t a r g e t . DWBA a n a l y s i s . PRVCA 25 1276. NUCLEAR REACTIONS 74,76,77,Ts,8°Se(n,'/),E=thermal,resonance; m e a s u r e d E'y,IT. 75,77,TS,SlSe d e d u c e d n e u t r o n s e p a r a t i o n e n e r g i e s , Q . 75,77,78,79,81Se d e d u c e d levels,J,rr. NUPAB 372 125. NUCLEAR REACTIONS mBr,51V,ST,ShRb(SHe,t),E=24.7 MeV; m e a s u r e d a(Et),Q. SlKr d e d u c e d mass. PRVCA 25 1076. RADIOACTIVITY 81,Sam,Sa,S4,84mRb,83,a5msr; m e a s u r e d T1/a,E-/,I% 87msr,34mCl; m e a s u r e d T1/2. S p o l i a t i o n r e a c t i o n p r o d u c t s , R b C 1 t a r g e t s . IJARA 33 456. NUCLEAR REACTIONS 65Cu(laF,2np),E=hO,55,58 MeV; m e a s u r e d ET,recoil d i s t a n c e , D S A . SJRb l e v e l s d e d u c e d T1/a,B(X). E n r i c h e d t a r g e t . A s y m m e t r i c r o t o r p l u s p a r t i c l e m o d e l . NUPAB 376 367,

34

KEY

NUMBERS

A 8~Sr

D 82De36:

R 82Th03 S~y

D 82De36

81Zr

D 82De36

R 810h09

82Wo06 aaKr

R 82Br05

82Ke01

82Mal8

~ZRb

D 82Gr07

=

81

KEYWORDS

continued

RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(32S,n2p~),SOCr(32S,n2p),E=123 MeV]; m e a s u r e d VV-, (X-ray)v-coin; d e d u c e d m a s s e x e e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d l e v e l s , d , ~ , I C C , T l / 2 , 7_multipolarity,v_branehing" 8Oy(fl+) C f r o m ~4Fe(S2S,np),E=123 MeVS; m e a s u r e d Tl/2,VV-, B V - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s exeess,Q(B). S°Sr d e d u c e d levels,J,~,Tl/2,ICC. 81Zr(B+) E f r o m 54Fe(a2S,n~),E=123 MeVS; 81Y(B+) [ f r o m SlZr decay3; m e a s u r e d T1/2,B-endpoint energies, f l V - , v ( X - r a y ) - c o i n ; d e d u c e d Q(EC),QB,log f t , m a s s e x c e s s . 81St d e d u c e d levels,J,rr,Tt/~, v - b r a n c h i n g . SeZr(B+),SeY(B+)" [ f r o m S2Zr decayS; m e a s u r e d TWe,BV-coin,Ev; d e d u c e d m a s s e x c e s s . S2Zr d e d u c e d Q(EC). S~Sr d e d u c e d levels,J,rr,Tl/2 u p p e r l i m i t , v - b r a n c h i n g . SaZr(B +) [ f r o m 54Fe(aaS,n2p)3,83Y(B+) [ f r o m 54Fe(SeS,3p)],SamY(fi+) [ f r o m 83Zr decayS; m e a s u r e d T~/e,E % 7(X-ray),Bv-,(mass)v-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d l e v e l s , J , r r , I C C , v-multipolarity,Tl/2 u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . SSZr d e d u c e d isomer,T1/z. 84Zr(B +) [ f r o m 54Fe(32S,2p)]; m e a s u r e d T t / a , v ( X - r a y ) - c o i n . 85Zr(B+) [ f r o m 5SNi(sZS,n4p)]; m e a s u r e d TI/ 2 , B v - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. NUCLEAR REACTIONS 54,5SFe(aSSi,xnypv),E=80-99 MeV; m e a s u r e d Ev,Iv,vv-coin,cr(E%E),~(E%0). 79Rb,e°,S~Sr d e d u c e d l e v e l s , J d r . E n r i c h e d t a r g e t s . PRVCA 25 1325. RADIOACTIVITY 79Sr(B +) [ f r o m 54Fe(3eS,n2pc~),S°Cr(aeS,n2p),E=123 MeV]; m e a s u r e d 7 7 - , (X-ray)v-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,~r,ICC,Tl/2, 7-multipolarity,7-branehing. 80y(fl+) [ f r o m 54Fe(a2S,np),E=123 MeV]; m e a s u r e d TI/2,VV-, f i v - e o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). S°Sr d e d u c e d levels,J,rr,T1/z,lCC. SIZr(B+) [ f r o m 54Fe(a2s,na),E=123 MeV]; mY(B*) [ f r o m mZr decayS; m e a s u r e d T~/~,B-endpoint energies, Bv-,7(X-ray)-coin; d e d u c e d Q(EC),QB,log f t , m a s s e x c e s s . SlSr d e d u c e d levels,J,vr,Tl/2, v - b r a n c h i n g . 82Zr(B+),S2Y(B +) [ f r o m S2Zr decayS; m e a s u r e d Tl/e,BV-coin,Ev; d e d u c e d m a s s e x c e s s . SeZr d e d u c e d Q(EC). 8~Sr d e d u c e d levels,J,zr,T~/2 u p p e r l i m i t , v - b r a n c h i n g . SaZr(B +) [ f r o m 5*Fe(aaS,nap)],83Y(B+) [ f r o m 54Fe(aaS,3p)],Samy(B+) [ f r o m 8aZr decay]; m e a s u r e d T~/a,E7, 7(X-ray),BV-,(mass)v-coin; d e d u c e d Q(EC),mass e x c e s s . Say d e d u c e d l e v e l s , J , ~ , I C C , 7 - m u l t i p o l a r i t y , T 1 / ~ u p p e r l i m i t . 8aSr d e d u c e d l e v e l s . 8aZr d e d u c e d isomer,T~/a. 8*Zr(B +) [ f r o m 54Fe(SaS,Sp)]; m e a s u r e d T ~ / a , v ( X - r a y ) - c o i n . 85Zr(B+) [ f r o m 58Ni(aaS,n4p)]; m e a s u r e d T~/ 3 , B v - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. RADIOACTIVITY VaSt(B+) [ f r o m 54Fe(aeS,n2pa),5°Cr(a~S,n2p),E=123 MeV]; m e a s u r e d 7 7 - , (X-ray)V-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,rr,ICC,T~/a, v-multipolarity,v-branching. S°Y(B+) C f r o m S4Fe(aaS,np),E=la3 MeV]; m e a s u r e d TWa,77-, B V - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,zr,T~/a,lCC. ~Zr(B +) [ f r o m 54Fe(3aS,na),E=123 MeV]; SlY(B+) [ f r o m mZr decay3; m e a s u r e d T~/2,fl-endpoint energies, flV-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . S~Sr d e d u c e d levels,J,~r,T~/a, 7 - b r a n c h i n g . aaZr(fl+),aaY(fl÷) [ f r o m aaZr decayS; m e a s u r e d T~/~,flV-coin,Ev; d e d u c e d m a s s e x c e s s . SaZr d e d u c e d Q(EC). 8aSr d e d u c e d levels,J,~r,T~/a u p p e r l i m i t , v - b r a n c h i n g . 8aZr(B+) [ f r o m 5~Fe(3aS,nSp)3,83y(fl+) [ f r o m 5*Fe(aas,3p)],Samy(fl+) [ f r o m 8aZr decay]; m e a s u r e d T~/a,EV, V(X-ray),flV-,(mass)y-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . Say d e d u c e d levels,J,~r,tCC, v - m u l U p o l a r i t y , T ~ / a u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . 83Zr d e d u c e d isomer,T~/a. S4Zr(fl +) [ f r o m S4Fe(aaS,ap)]; m e a s u r e d T~/2,7(X-ray)-coin. 85Zr(fl +) [ f r o m 58Ni(aaS,n4p)]; m e a s u r e d T~/ 2 , f i T - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305.

A 82Br

AND

=

82

NUCLEAR REACTIONS 79,8~Br(n,7),(n,X),E=0.05-10 keV; m e a s u r e d t r a n s m i s s i o n , E % l % 8°,SaBr d e d u c e d < PV > , a v e r a g e l e v e l s p a c i n g , r e s o n a n c e s , r e s o n a n c e p a r a m e t e r s , s - w a v e strength f u n c t i o n s . A r e a a n a l y s i s , M o n t e Carlo c a l c u l a t i o n . JNSTA 18 745. NUCLEAR REACTIONS ~6 8o,82Se(p,n),E=19,20,22,25 MeV; m e a s u r e d cr(En),cr(0). 76,8°,SeBr d e d u c e d a n a l o g e x c i t a t i o n m e c h a n i s m . C o u p l e d - c h a n n e l s c a l c u l a t i o n . PRVCA 26 889. NUCLEAR REACTIONS 76Ge(mC,2nc~),E=42-52 MeV; m e a s u r e d Ev,Iv,recoil. aaKr levels deduced T1/ 2 , c o n f i g u r a t i o n s . E n r i c h e d targets. T w o - q u a s i p a r t i c l e plus rotor m o d e l , i n t e r a c t i n g boson approximation,cranked s h e l l m o d e l . ZPAAD 304 335. NUCLEAR REACTIONS 63Cu(19F,2n~),E=58 MeV; m e a s u r e d recoil. 27A1,64,66Zn,7°72,74,76Ge(SaKr, 8eKr'),(84Kr,84Kr'),E=l15,118 MeV; m e a s u r e d C o u l o m b exeitation,cr(E),DSA; d e d u c e d s t o p p i n g p o w e r f o r Kr i n AI,Zn,Ge,Ge in Ge,Zn in Zn. 76,8a,84Kr level d e d u c e d B(E2),Twe. NUPAB 376 246. NUCLEAR REACTIONS 78,e°,sa,a4Kr(p,t),E=51.9 MeV; m e a s u r e d ~(0). 76 78 8o,8aKr d e d u c e d octupole state splittings,enhaneement f a c t o r s . DWBA a n a l y s i s , i n t e r a c t i n g b o s o n m o d e l . PYLBB 113 21. RADIOACTIVITY sl,sam,Sa,s4,~4mRb,Sa,S5mSr; m e a s u r e d T1/2,E7,I V. 87msr,a4mcl; m e a s u r e d TW2. S p a l l a t i o n r e a c t i o n p r o d u e t s , R b C l t a r g e t s . IJARA 33 456.

35

KEY

NUMBERS

A

83Sr

D 82De36:

Say

D 82De36:

8~Zr

D 82De36:

D 82Me01:

83Se

D 82Me01: R 82Br18:

83Br

R 82Ze02:

SSKr

R 82Es01:

SaRb

D 82Gr07: 82Po04: R 82Fa12:

=

82

KEYWORDS

continued

RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(3aS,n~pa),5°cr(a2s,n2p),E=123 MeV]; m e a s u r e d ~ - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,Tw2, ~/-multipolarity,7-branching. 8Oy(fl+) [ f r o m 54Fe(a2s,np),E=123 MeV]; m e a s u r e d T1/2,77-, fl~/-coin; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,rr,T1/e,ICC. SlZr(fl+) [ f r o m 54Fe(32S,na),E=123 MeV]; 8ty(fl+) [ f r o m 81Zr decayS; m e a s u r e d T l / a , f l - e n d p o i n t energies, fl~-,7(X-ray)-coin; d e d u c e d Q(EC),QFl,log f t , m a s s e x c e s s . 81Sr d e d u c e d levels,J,Tr,T1/2, 7 - b r a n c h i n g . 82Zr(fl+),SZY(fl+) E f r o m SeZr decay3; m e a s u r e d T1/2,flT-coin,ET; d e d u c e d m a s s excess. 8aZr d e d u c e d Q(EC). 82Sr d e d u c e d levels,J,rr,Tt/2 u p p e r l i m i t , 7 - b r a n c h i n g . 83Zr(fl+) [ f r o m 5*Fe(SeS,n2p)],eSY(fl+) [ f r o m 54Fe(aes,3p)3,Samy(fl+) [ f r o m 83Zr decayS; m e a s u r e d Tt/a,ET, 7(X-ray),fl~-,(mass)~-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d l e v e l s , J , r r , I C C , 7 - m u l t i p o l a r i t y , T l / ~ u p p e r l i m i t . 8asr d e d u c e d l e v e l s . 83Zr d e d u c e d isomer,T1/a. 84Zr(fl+) [ f r o m 54Fe(aaS,2p)3; m e a s u r e d T~/a,7(X-ray)-coin. 85Zr(fl+) [ f r o m ~8Ni(seS,n4p)3; m e a s u r e d Tt/ 2 , f l ~ - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. RADIOACTIVITY ~gSr(fl +) [ f r o m 54Fe(a2S,n~pa),5°Cr(32S,n2p),E=123 MeVS; m e a s u r e d 7~/-, (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d l e v e l s , J j r , I C C , T w 2 , 7-multipolarity,7-branching. S0y(fl+) [ f r o m 54Fe(SaS,np),E=123 MeV]; m e a s u r e d T1/2,77-, f i T - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,~r,T1/2,lCC. SlZr(fl+) [ f r o m 54Fe(32S,na),E=123 MeV]; 81y(fl+) [ f r o m SlZr decayS; m e a s u r e d T~/~,fl-endpoint energies, f l ~ / - , ~ ( X - r a y ) - c o i n ; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . S~Sr d e d u c e d levels,J,Tr,T1/2, 7 - b r a n c h i n g . a~Zr(fl+),S2Y(fl +) [ f r o m S2Zr d e c a y ] ; m e a s u r e d T~/2,flT-eoin,ET; d e d u c e d m a s s excess. 8aZr d e d u c e d Q(EC). 8aSr d e d u c e d levels,J,Tr,T~/a u p p e r l i m i t , 7 - b r a n c h i n g . 83Zr(fl+) [ f r o m 54Fe(aaS,n2p)],SaY(fl+) [ f r o m 54Fe(aaS,3p)3,S3my(fl÷) [ f r o m 83Zr decayS; measured TI/z,E % 7(X-ray),fl~/-,(mass)7-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . Say d e d u c e d l e v e l s , J , r r , I C C , ~ - m u l t i p o l a r i t y , T ~ / a u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . 83Zr d e d u c e d i s o m e r , T t / a . 84Zr(fl+) [ f r o m 54Fe(aeS,ap)]; m e a s u r e d T t / a , 7 ( X - r a y ) - c o i n . SSZr(fl+) [ f r o m 5SNi(32S,n4p)]; m e a s u r e d T~/ 2,fl~/-coin; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(a2S,n2pa),5°Cr(aaS,n2p),E=123 MeV]; m e a s u r e d ~ 7 - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,T~/a, 7 _ m u l t i p o l a r i t y , ~ / _ b r a n c h i n g . S0y(fl+) [ f r o m 54Fe(aaS,np),E=t23 MeVS; m e a s u r e d T~/z,7"~-, fl-~-coin; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8SSr d e d u c e d levels,J,~r,Tl/e,ICC. 8~Zr(fl+) [ f r o m 54Fe(S2S,na),E=123 MeV]; e~y(fl+) [ f r o m S~Zr decay]; m e a s u r e d T t / 2 , f l - e n d p o i n t energies, flT-,~(X-ray)-coin; d e d u c e d Q(EC),QFl,log f t , m a s s e x c e s s , atSr d e d u c e d levels,J,Tr,Tl/a, v - b r a n c h i n g . 82Zr(fl+),S2Y(fl+) [ f r o m S2Zr d e c a y ] ; m e a s u r e d Tl/2,flT-coin,ET; d e d u c e d m a s s excess. 8aZr d e d u c e d Q(EC). SaSr d e d u c e d levels,J,~r,Tt/2 u p p e r l i m i t j / - b r a n c h i n g . SaZr(fl+) [ f r o m 54Fe(aaS,n2p)],aaY(fl+) [ f r o m 54Fe(aeS,3p)],SamY(fl+) [ f r o m SaZr decayS; m e a s u r e d Tt/e,ET, T(X-ray),flT-,(mass)2-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d levels,J,Tr,ICC, 7 - m u l t i p o l a r i t y , T t / 2 u p p e r l i m i t . 8aSr d e d u c e d l e v e l s . 8aZr d e d u c e d isomer,T~/2. S4Zr(fl+) [ f r o m 54Fe(aaS,ap)]; m e a s u r e d Tx/z,T(X-ray)-coin. 85Zr(fl+) [ f r o m 58Ni(sas,n4p)3; m e a s u r e d TI/ 2 , f i T - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305.

A

83As

AND

=

83

RADIOACTIVITY 83As; m e a s u r e d E%IT,T1/2. 83Se d e d u c e d levels,J,rr. Ge(Li) d e t e c t o r s . PRVCA 25 682. RADIOACTIVITY 83As; m e a s u r e d ET,I%Tt/2. 83Se d e d u c e d levels,J,Tr. Ge(Li) d e t e c t o r s . PRVCA 35 682. NUCLEAR REACTIONS 82Se,Se(nj/),E=0.O06-40 keV; m e a s u r e d ~ ( c a p t u r e ) vs E. BaSe d e d u c e d r e s o n a n c e s . PRVCA 26 969. NUCLEAR REACTIONS 82Se(7Li,2na),(TLi,4n),E=32.5 MeV; 82Se(6Li,na),(6Li,3n),E=27 MeV; m e a s u r e d E T , I T ( 0 ) , a ( E , E T ) , 7 7 - c o i n . SSBr,85Rb d e d u c e d l e v e l s , J j r , y r a s t b a n d s . E n r i c h e d t a r g e t , G e ( L i ) d e t e c t o r s . PRVCA 25 1379. NUCLEAR REACTIONS S°Se(a,nT),E=10,12.8,14.8 MeV; m e a s u r e d ET,IT,7~/-coin,-y(0),a(ET). S3Kr d e d u c e d I e v e l s , T - b r a n c h i n g , J , T r . P a r t i c l e - r o t o r m o d e l . PHSTB 25 15. RADIOACTIVITY 81,82m,Sa,e4,S4raRb,S3,eSmSr; m e a s u r e d T1/a,ET,I7. 87mSr,34rac1; m e a s u r e d T~/2. S p o l i a t i o n r e a c t i o n p r o d u e t s , R b C l t a r g e t s . IJARA 33 456. RADIOACTIVITY Sasr [ f r o m Rb(p,xn),E=36,40 MeV]; m e a s u r e d E % I T , 7 7 - c o i n , c e n t r o i d s h i f t s . saRb l e v e l s d e d u c e d 7 - b r a n c h i n g r a t i o s . H y p e r p u r e Ge,Ge(Li) d e t e c t o r s . NCIAA 69 62. NUCLEAR REACTIONS S2Kr(p,7),s3,86Kr(p,n),E=3.8 MeV; m e a s u r e d E%I%DSA. 86Rb level d e d u c e d Tt/2. 83Rb l e v e l s d e d u c e d T t / a , 7 - b r a n c h i n g , c o l l e c t i v i t y , c o n f i g u r a t i o n . N a t u r a l Kr gas t a r g e t . PRVCA 26 1740.

36

KEY

NUMBERS

A 83Sr

D 82De36

82Gr07 82Po04 83y

D

83De36

S3Zr

D

82De36

R 82Re01

82Za04 S4Rb

D 82Gr07

84SF

R 82De05

=

83

KEYWORDS

continued

RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(32S,n2pa),S°Cr(32S,n]p),E=123 MeV]; m e a s u r e d 7 7 - , (X-ray)-/-eoin; deduced m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,T1/2, -/-multipolarity,-/-branching. 80y(fl+) [ f r o m 54Fe(aas,np),E=123 MeVS; m e a s u r e d TI/a,-/-/-, f l - / - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,Tr,Tl/z,ICC. 81Zr(fl+) [ f r o m 54Fe(SeS,na),E=123 MeV]; Siy(fl+) [ f r o m 81Zr decay]; m e a s u r e d T l / 2 , f l - e n d p o i n t energies, f l - / - , - / ( X - r a y ) - c o i n ; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d l e v e l s , J j r , T l / a , - / - b r a n c h i n g . 8~Zr(fl+),82Y(fl +) [ f r o m 8eZr d e c a y ] ; m e a s u r e d Tl/2,fl-/-coin,E7; d e d u c e d m a s s e x c e s s . SZZr d e d u c e d Q(EC). 82Sr d e d u c e d levels,J,Tr,Tl/a u p p e r l i m i t , - / - b r a n c h i n g . 83Zr(fl+) [ f r o m 54Fe(SZS,n2p)3,S3Y(fl+) [ f r o m S4Fe(SeS,3p)],SSmY(fl+) [ f r o m 83Zr decay]; m e a s u r e d T~/z,E-/, -/(X-ray),fl-/-,(mass)-/-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d tevets,J,Tr,ICC, - / - m u l t i p o l a r i t y , T i / 2 u p p e r l i m i t . 83Sr d e d u c e d levels. SSZr d e d u c e d i s o m e r , T l / 2 . S4Zr(fl+) [ f r o m S4Fe(SeS,]p)]; m e a s u r e d T l / 2 , 7 ( X - r a y ) - c o i n . SSZr(fl+) [ f r o m SSNi(seS,n4p)3; m e a s u r e d Ti/ 2 , f l - / - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. RADIOACTIVITY 81,82m,83,s4,84mRb,83,85mSr; m e a s u r e d Ti/a,E-/,I-/. 87mSr,34mCl; m e a s u r e d Tl/a. S p a l l a t i o n r e a c t i o n p r o d u c t s , R b C 1 t a r g e t s . IJARA 33 456. RADIOACTIVITY 83Sr [ f r o m Rb(p,xn),E=36,40 MeVS; m e a s u r e d ET,I-/,-/-/-coin,centroid s h i f t s . S3Rb l e v e l s d e d u c e d - / - b r a n c h i n g r a t i o s . H y p e r p u r e Ge,Ge(Li) d e t e c t o r s . NCIAA 69 62. RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(SeS,n2pa),5°Cr(32S,n2p),E=123 MeVS; m e a s u r e d 7 7 - , (X-ray)-/-eoin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,T1/2, -/-multipolarity,-/-branching. 80y(fl+) [ f r o m S4Fe(3aS,np),E=123 MeV]; m e a s u r e d T1/2,-/-/-, f i T - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). S°Sr d e d u c e d levels,J,Tr,Tl/e,ICC. 81Zr(fl+) [ f r o m 54Fe(SZS,na),E=133 MeV]; 8iy(fl+) [ f r o m 81Zr decay3; m e a s u r e d T 1 / z , f l - e n d p o i n t energies, flT-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81sr d e d u c e d levels,J,Tr,Tl/e, - / - b r a n c h i n g . 82Zr(fl+),eZY(fl +) [ f r o m 82Zr decay3; m e a s u r e d Tl/a,fl-/-coin,E-/; d e d u c e d m a s s e x c e s s . S]Zr d e d u c e d Q(EC). 82Sr d e d u c e d levels,J,Tr,T,/e u p p e r l i m i t , 7 - b r a n c h i n g . 83Zr(fl+) [ f r o m 54Fe(32S,n]p)],S3Y(fl+) [ f r o m 54Fe(3ZS,3p)],83my(fl+) [ f r o m SSZr decay]; m e a s u r e d T1/2,E% -/(X-ray),fl-/-,(mass)7-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d levels,J,~r,ICC, - / - m u l t i p o l a r i t y , T l / 2 u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . SSZr d e d u c e d isomer,T1/2. 84Zr(fl+) [ f r o m 54Fe(32S,2p)3; m e a s u r e d T1/2,-/(X-ray)-coin. 85Zr(fl+) [ f r o m 58Ni(32S,n4p)]; m e a s u r e d T~/ 2 , f l - / - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305. RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(3aS,n2pc~),5°Cr(SZS,n2p),E=123 MeVS; m e a s u r e d 7 7 - , (X-ray)7-coin; d e d u c e d m a s s e x c e s s , Q ( E C ) , l o g f t . 79Rb d e d u c e d levels,J,Tr,ICC,Tl/z, -/-multipolarity,-/-branching. SOy(fl+) [ f r o m 54Fe(3aS,np),E=123 MeV]; m e a s u r e d Tl/z,-/-/-, f l - / - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,Tr,Tl/a,ICC. SlZr(fl+) [ f r o m 54Fe(aas,na),E=133 MeVS; 81y(fl+) [ f r o m 8lZr decay]; m e a s u r e d T l / 2 , f l - e n d p o i n t energies, f l - / - , - / ( X - r a y ) - c o i n ; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d levets,J,~T,T1/e, - / - b r a n c h i n g . 82Zr(fl+),SaY(fl+) [ f r o m 8aZr d e c a y ] ; m e a s u r e d Ti/a,flT-coin,E-/; d e d u c e d m a s s e x c e s s . 82Zr d e d u c e d Q(EC). 82Sr d e d u c e d levels,J,rr,Tl/z u p p e r l i m i t , - / - b r a n c h i n g . 83Zr(fl+) [ f r o m S4Fe(aaS,n2p)],SaY(fl +) [ f r o m S4Fe(3~S,3p)],83my(fl+) [ f r o m 83Zr decay]; m e a s u r e d Ti/z,E-/, -/(X-ray),flT-,(mass)-/-coin; d e d u c e d Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d levels,J,zr,ICC, - / - m u l t i p o l a r i t y , T l / ~ u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . 8~Zr d e d u c e d isomer,T~/z. S4Zr(fl+) [ f r o m S4Fe(32S,]p)3; m e a s u r e d T l / 2 , - / ( X - r a y ) - c o i n . 85Zr(fl+) [ f r o m SSNi(saS,n4p)]; m e a s u r e d T~/ 2 , f l - / - c o i n ; d e d u c e d Q(EC),mass e x c e s s . ZPAAD 307 305.

A 84Kr

AND

=

84

NUCLEAR REACTIONS S3Cu(19F,]na),E=58 MeV; m e a s u r e d recoil. STAI,64,66Zn,7°,72,74,TSGe(82Kr, SaKr'),(84Kr,a4Kr'),E=l15,118 MeV; m e a s u r e d C o u l o m b excitation,(r(E),DSA; d e d u c e d s t o p p i n g p o w e r f o r Kr in A1,Zn,Ge,Ge in Ge,Zn in Zn. 76,sa,S4Kr level d e d u c e d B(E]),T1/2. NUPAB 376 346. NUCLEAR REACTIONS 82Se(c~,]n),E=16.5-27.3 MeV; m e a s u r e d ET,lT,-/(t),-/(0,H,t ). S4Kr d e d u c e d i s o m e r Ti/2,J,~r,/z. RRPQA 27 33. RADIOACTIVITY sl S]m,Sa,s4,s4mRb,S3,SSmSr ; m e a s u r e d T1/2,E-/,tT. 87mSr,a4mCl; m e a s u r e d T1/a. S p a l l a t i o n r e a c t i o n p r o d u c t s , R b C 1 t a r g e t s . IJARA 33 456. NUCLEAR REACTIONS 76Ge(laC,4n),E=48-60 MeV; SlBr(6Li,3n),E=19-33 MeV; m e a s u r e d E-/,I-/, - / - / - c o i n , 7 ( 0 ) , D S A , r e c o i l . 84Sr d e d u c e d l e v e l s , J , r r , T l / 2 , B ( E ] ) , b a n d s t r u c t u r e . Enriched t a r g e t , C e ( L i ) d e t e c t o r s . PRVCA 25 226.

37

KEY

NUMBERS

A 84Zr

D

82De36

D 82Li09 82Re08 82Re10

85Br

D

82LiO9

85Kr

D

82Li09

85Rb

R 82Fa09

82Ze02

85Sr

D 82Gr07

85Zr

D 82De36

D 82Li09 82Re08 82Re10

S6Br

D 82A101

82Li09

86KF

D 82Li09

84

continued

=

85

RADIOACTIVITY 85,86,87,88Se [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g d - d e c a y , ss,a6,aT,88Br, ss,a6,aT,BaKF l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY 85,86,ST,88,89Se [ f r o m a35U(n,F)]; m e a s u r e d E7,IT,T1/2. 89Se d e d u c e d t r a n s i t i o n . O n - l i n e , f a s t gas j e t s y s t e m s . NUIMA 197 427. RADIOACTIVITY 85,86,87,88Se [ f r o m f i s s i o n ] ; m e a s u r e d ET,IT; d e d u c e d c u m u l a t i v e yields. Gas j e t s y s t e m . RRALA 51 339. RADIOACTIVITY ss,s6,av,SOSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g B - d e c a y . ss,s6,aT,SSBr, 8s,ss,87,SSKr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e I7. RRALA 50 399. RADIOACTIVITY 8s,8s,s7,SSSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,17 f o l l o w i n g B - d e c a y . ss,ss,aT,SSBr, 85,sS,aT,SaKr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e IT. RRALA 50 399. NUCLEAR REACTIONS a4Kr(p,7),E=l.85-2.87 MeV; m e a s u r e d ET,I7,77-coin,a(ET),DSA. aSRb(a,a'), E=3 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n . 85Rb d e d u c e d l e v e l s , 7 - b r a n c h i n g ratios,T,/2. N a t u r a l Kr gas t a r g e t . PRVCA 25 2309. NUCLEAR REACTIONS a S S e ( T L i , S n a ) , ( T L i , 4 n ) , E = 3 2 . 5 MeV; a S S e ( 6 L i , n a ) , ( S L i , 3 n ) , E = 2 7 MeV; measured E 7 , I 7 ( 0 ) , a ( E , E T ) , 7 7 - c o i n . aaBr,aSRb d e d u c e d l e v e l s , J , z r , y r a s t b a n d s . E n r i c h e d t a r g e t , G e ( L i ) d e t e c t o r s . PRVCA 25 1379. RADIOACTIVITY 81,8am,83,s4,s4mRb,S3,sSmsr; m e a s u r e d Tt/a,ET,17. 87mSr,34mCl; m e a s u r e d TI/2. S p a l l a t i o n r e a c t i o n p r o d u c t s , R b C l t a r g e t s . IJARA 33 456.. RADIOACTIVITY 79Sr(fl+) [ f r o m 54Fe(32S,nSpa),SOCr(3aS,nSp),E=123 MeV]; m e a s u r e d 7 7 - , (X-ray)T-coin; deduced m a s s e x c e s s , Q ( E C ) , l o g f t . 7ORb d e d u c e d levels,J,Tr,ICC,T,/z, 7-multipolarity,7-branching. 8°Y(B+ ) [ f r o m 54Fe(32S,np),E=123 MeV3; m e a s u r e d T , / 2 , 7 7 - , f l 7 - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,Tr,Tl/a,ICC. SlZr(fl+) [ f r o m 54Fe(32S,na),E=123 MeV]; mY(B+) [ f r o m mZr d e c a y ] ; m e a s u r e d T t / 2 , f l - e n d p o i n t e n e r g i e s , fl7-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d l e v e l s , J , ~ r , T t / e , 7 - b r a n c h i n g . 8eZr(fl+),SaY(fl+) [ f r o m SZZr d e c a y ] ; m e a s u r e d T t / e , f l 7 - c o i n , E T ; d e d u c e d m a s s e x c e s s , aaZr d e d u c e d Q(EC). 82Sr d e d u c e d l e v e l s , J j r , T t / a u p p e r l i m i t , 7 - b r a n c h i n g . . S3Zr(fl+) [ f r o m 54Fe(3aS,n2p)],a3Y(fl +) [ f r o m 54Fe(3SS,3p)],a3my(fl+) [ f r o m S3Zr d e c a y ] ; m e a s u r e d T1/z,ET, T(X-ray),fl7-,(mass)7-coin; deduced Q ( E C ) , m a s s e x c e s s . 83y d e d u c e d levels,J,~r,ICC, 7 multipolarity,Tt/2 u p p e r l i m i t . S3Sr d e d u c e d l e v e l s . S3Zr d e d u c e d i s o m e r , T 1 / 2 . 84Zr(fl+) [ f r o m 54Fe(3eS,Sp)3; m e a s u r e d T 1 / z , 7 ( X - r a y ) - c o i n . 85Zr(fl +) [ f r o m 58Ni(32S,n4p)3; m e a s u r e d Tl/ 2 , f i T - c o i n ; d e d u c e d Q ( E C ) , m a s s e x c e s s . ZPAAD 307 305.

A 86Se

=

KEYWORDS

RADIOACTIVITY ~°Sr(fl +) [ f r o m 54Fe(3eS,nSpa),5°Cr(aSS,nSp),E=123 MeV]; m e a s u r e d 7 7 - , (X-ray)7-coin; deduced m a s s e x c e s s , Q ( E C ) , l o g f t . 7ORb d e d u c e d levels,J,vr,ICC,Tl/2, 7-multipolarity,7-branching. B°Y(B+) [ f r o m S4Fe(32S,np),E=123 MeV3; m e a s u r e d T i / 2 ~ 7 7 - , f i T - c o i n ; d e d u c e d log f t , Q ( E C ) , m a s s excess,Q(fl). 8°Sr d e d u c e d levels,J,rr,Tl/2,ICC. 81Zr(fl+) [ f r o m 54Fe(3SS,na),E=133 MeV]; Sly(d+) [ f r o m alZr decayS; m e a s u r e d T t / e , f l - e n d p o i n t e n e r g i e s , flT-,7(X-ray)-coin; d e d u c e d Q(EC),Qfl,log f t , m a s s e x c e s s . 81Sr d e d u c e d levels,J,Tr,T1/2, 7 - b r a n c h i n g . 82Zr(fl+),aZY(fl +) [ f r o m 8aZr d e c a y 3 ; m e a s u r e d T i / 2 , f l 7 - c o i n , E T ; d e d u c e d m a s s e x c e s s . 82Zr d e d u c e d Q(EC). 82Sr d e d u c e d l e v e l s , J j r , T t / s u p p e r l i m i t , T - b r a n c h i n g . 83Zr(fl+) [ f r o m 54Fe(aSs,nSp)],SaY(fl+) [ f r o m 54Fe(aaS,3p)],Samy(fl +) [ f r o m 83Zr decay3; m e a s u r e d Tt/z,E7, 7(X-ray),flT-,(mass)7-coin; deduced Q ( E C ) , m a s s e x c e s s . Say d e d u c e d levels,J,rr,ICC, 7-multipolarity,T,/s u p p e r l i m i t . 83Sr d e d u c e d l e v e l s . 83Zr d e d u c e d i s o m e r , T t / 2 . 84Zr(fl+) [ f r o m 54Fe(aeS,Sp)]; m e a s u r e d T l / a , 7 ( X - r a y ) - c o i n . 65Zr(fl+) [ f r o m 5eNi(sSS,n4p)3; m e a s u r e d Tl/ 2 , f l V - c o i n ; d e d u c e d Q ( E C ) , m a s s e x c e s s . ZPAAD 307 305.

A 85Se

AND

=

86

RADIOACTIVITY 8s,ss,sv,SSSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g B - d e c a y . s5,s6,87,SSBr, ss,s6,87,8aKr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e I7. RRALA 50 399. RADIOACTIVITY 85,86,87,88,89Se [ f r o m 235U(n,F)3; m e a s u r e d E 7 , I T , T t / 2 . *SSe d e d u c e d t r a n s i t i o n . O n - l i n e , f a s t gas j e t s y s t e m s . NUIMA 197 427. RADIOACTIVITY ss,ss,sT,SSSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7; d e d u c e d c u m u l a t i v e yields. Gas j e t s y s t e m . RRALA 51 339. RADIOACTIVITY 86,87,88,89BF,SD,91,92,S3Kr,89,91,92,93,94 R D,93,94,OSsF,94,95,96y,134Sb, 136,137,138,1391, 13713813914°,141Xe,138~13%i40,141,142Cs; m e a s u r e d a v e r a g e Eft. F i s s i o n p r o d u c t s , B - s t r e n g t h f u n c t i o n s i n p u t , S i - L i d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 85,86,87,SSSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g B - d e c a y . 85,86,87,88Br, 85,86,sv,SaKF l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY 85,86,87,88Se [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g fl d e c a y . 85,86,87,88Br, 85,86,87,88Kr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e I7. RRALA 50 399.

38

KEY

NUMBERS

A

86Rb

R 82Fa12:

D 82Li09: 8£Re08: 8~RelO:

S~Br

D 82A101:

82Li09: 87KF

D 8~Li09:

87Sr

D 82Gr07: R 8~Fa08:

82Hi11:

8~InOl:

82P104

D 82Li09 82Re08 82RelO

88Br

D 82A101

82Li09 88KF

D 82Li09

8aRb

D 82De08

88Sr

R 82Hill 82TiOl

82VaO5 88ZF

D 81Ju03

86

continued

=

:

87

RADIOACTIVITY 85,86,87,883e [ f r o m f i s s i o n ] ; m e a s u r e d 85,ae,aT,SSKr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e I% RADIOACTIVITY 85,86,87,88,893e [ f r o m 835U(n,F)]; transition. On-line,fast gas j e t s y s t e m s . NUIMA 197 RADIOACTIVITY 95,86,87,883e [ f r o m f i s s i o n ] ; m e a s u r e d j e t s y s t e m . RRALA 51 339.

E7,I7 f o l l o w i n g f l - d e c a y . 85,86,87,88Br, RRALA 50 399. measured E T , I T , T I / a . 893e d e d u c e d 427. E7,I7; d e d u c e d c u m u l a t i v e yields. Gas

RADIOACTIVITY 86,87,88,89Br,SS,91,92,93Kr,89,91,92,93,94R b,93,94,95Sr,94,95,96y,134Sb,136,137,138,139I,

137,138,139,140,141Xe,138,13g,140,141,142Cs; m e a s u r e d average Eft. Fission p r o d u c t s , f - s t r e n g t h f u n c t i o n s i n p u t , S i - L i detector s y s t e m . NSENA 80 74. RADIOACTIVITY 85,se,87,SSSe [ f r o m fission]; measured E7,17 following f - d e c a y . 85,s6,87,SSBr, ss,86,87,88Kr levels deduced 7 - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY ss,86,sT,SSSe [ f r o m fission]; measured E7,17 following f-decay, as,86,sT,a8Br, 95,86,aT,88Kr levels deduced 7 - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY 8t,83m,83,84,84mRb,83,85mSr; measured Tt/2,ET,17. 87mSr,34mc]; measured TI/2. Spallation reaction products,RbCl targets. IJARA 33 456. NUCLEAR REACTIONS 9aMo,9°Zr,86Sr,74Se(n,2n),(7,n),E:14.5 MeV; measured (r(isomer)/~(ground state). 93Mo,91Zr,87SF,75Se deduced level d e n s i t y spin dependence p a r a m e t e r . Compound n u c l e u s decay calculations. YAFIA 35 257. NUCLEAR REACTIONS 86,SVSr(n,7),E=3-200 keV; m e a s u r e d (r(capture); deduced c a p t u r e m e c h a n i s m . 87,883r deduced resonances,L,Fn,FT. Statistical model. AUJPA 35 267. NUCLEAR REACTIONS 883r('2C,12C),('ZC,'2C'),(12C,'3C),E:80 MeV; m e a s u r e d ~(0),(r(E(~zC)), a(E(13C)): deduced optical model parameters. ~aC level deduced spin alignment. 873r levels deduced L,CzS,configurations. ZPAAD 305 135. NUCLEAR REACTIONS 49Ti,51V,59Co,e7Sr,93Nb,2°gBi(e,e),E=175-325,500 MeV; m e a s u r e d cr(0,E). 49Ti,stv,aTSF,93Nb deduced valence n u c l e o n tins,charge radii. PWBA,DWBA a n a l y s e s , m e s o n exchange effects. PRVCA 25 ~318.

A

88Se

KEYWORDS

NUCLEAR REACTIONS 8aKr(p,7),s3,a6Kr(p,n),E=2.8 MeV; m e a s u r e d ET,IT,DSA. 86Rb ievel d e d u c e d T~/z. 83Rb l e v e l s d e d u c e d Twa,7-branching,eolleetivity,configurationo Natural Kr g a s t a r g e t . PRVCA 26 1740.

A

87Se

AND

=

88

RADIOACTIVITY ss,86,sv,883e [ f r o m f i s s i o n ] ; m e a s u r e d E7,17 f o l l o w i n g f l - d e c a y . 85,86,87,88Br, 85,s6,sT,SSKr l e v e l s d e d u c e d - y - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY 85,86,87,88,893e [ f r o m 235U(n,F)]; m e a s u r e d ET,IT,T1/2. 893e d e d u c e d transition. On-line,fast gas j e t s y s t e m s . NUIMA 197 427. R A D I O A C T I V I T Y 85,86,87,883e [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7; d e d u c e d c u m u l a t i v e yields. Gas j e t s y s t e m . RRALA 51 339. RADIOACTIVITY 86,87,s8,89Br,89,91,92,93Kr,89,91,93,93,94 Rb,93,94,953r,94,95,96y,1343b,i 36,137,138,139I, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; measured average Eft. F i s s i o n p r o d u e t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 85,86,87,8SSe [ f r o m f i s s i o n ] ; m e a s u r e d E-/,I7 f o l l o w i n g f l - d e e a y . 85,86,87,aaBr, 85,86,87,88Kr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e 17. RRALA 50 399. RADIOACTIVITY ss,s6,sv,eSSe [ f r o m f i s s i o n ] ; m e a s u r e d E7,I7 f o l l o w i n g f l - d e e a y . 85,8e,sv,SSBr, 85,86,aT,88Kr l e v e l s d e d u c e d 7 - b r a n c h i n g , a b s o l u t e I7. RRALA 50 399. R A D I O A C T I V I T Y 28Al,aOF,38cl,SSRb [ f r o m ZVAl,tgF,svCt,S7Rb(d,p),E=l-6.5 MeV]; m e a s u r e d Eft, flT-coin,fl-endpoint energies,Qfl. H y p e r p u r e Ge d e t e c t o r , o n - l i n e s e p a r a t i o n . NUIMA 192 261. NUCLEAR REACTIONS 8 e , S V S r ( n , 7 ) , E = 3 - 2 0 0 k e V ; m e a s u r e d or(capture); deduced capture mechanism, sT,883r d e d u c e d r e s o n a n e e s , L , F n , F T . S t a t i s t i c a l m o d e l . A U J P A 35 267. NUCLEAR REACTIONS 9z,94,96,98,1°OMo,g°,ge,94Zr(6Li,SB),E=90 MeV; m e a s u r e d cr(E(SB)),cr(O), ss,90 923r,9°,9z,94,96,98ZF d e d u c e d c h a r a c t e r i s t i c s of s t r o n g t r a n s i t i o n s . Magnetic spectrometer, enriched t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. NUCLEAR REACTIONS 883r(e,e0,E=36,42,50 MeV; m e a s u r e d c r ( E ( e ' ) , 0 - 1 6 5 ° ) , f o r m f a c t o r . 8aSr d e d u c e d i s o b a r r o l e i n M1 t r a n s i t i o n strength quenching. ZPAAD 305 231. R A D I O A C T I V I T Y 88Zr [ f r o m 89y(p,2n),E=17.2 MeV]; m e a s u r e d I(ee),ET,I% 8aZr l e v e l s d e d u c e d B(E0)flB(E2). ZPAAD 303 147.

39

KEY

NUMBERS

A

89Se

D 82Re08

89Br

D 82A101

89Kr

D 82A101

89Rb

D 82A101

89Sr

D 82Me04

89y

J

82Ha21

R 81Va24 82Dy01 82Me02

82Sa19

82Sc08

89Nb

R 82DiO9

R 82Ti01

9OZr

R 82Be18: 82Co09:

82Cr02: 82Dj04:

82Dy01: 82Fall: 82GaO2:

82Ma30:

82Na06:

=

KEYWORDS

89

RADIOACTIVITY 85,66,87,88,89Se [ f r o m a35U(n,F)3; m e a s u r e d ET,IT,T1/2. aSSe d e d u c e d transition. On-line,fast gas j e t s y s t e m s . NUIMA t97 427. RADIOACTIVITY ss,87,ss,SSBr,SS,Sl,sa,93K r,89,91,92,93,94 R b,93,94,95Sr,94,95,96y,134Sb,136,137,13s,13sI, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; measured average Eft. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 86,87,88,89Br,a9,91,92,93Kr,89,91,9a,93,94 R b,93,94,95Sr,94,95,96y,134Sb,136,137,138,139I, 137,138,139,146,141Xe,138,139,14°,141,142Cs; measured average Eft. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 86,87,s8,89Br,a9,91,sa,93K r,89,9~,92,93,94 R b,93,94,95Sr,94,95,96y,134Sb,136,137,138,1391, 137,138,139,14°,141Xe,138,139,149,141,142Cs; measured average Eft. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 89St; m e a s u r e d 7 - e m i s s i o n p r o b a b i l i t y f o l l o w i n g f l - d e c a y . 4~r fl c o u n t i n g . I J A R A 33 77. NUCLEAR MOMENTS e9y; m e a s u r e d o p t i c a l h f s ; d e d u c e d m a g n e t i c h y p e r f i n e interaction c o n s t a n t s , g . L e v e l c r o s s i n g o p t o g a l v a n i e s p e c t r o s c o p y . PRLTA 48 1326. NUCLEAR REACTIONS 89Y(-y,p),E=14-24 MeV b r e m s s t r a h l u n g ; m e a s u r e d a ( E ) a b s o l u t e . 89y d e d u c e d T(<) GDR c o m p o n e n t Fp. N a t u r a l t a r g e t . PRVCA 24 2499. NUCLEAR REACTIONS 88Sr(p,'y),E=2.2-3.7 MeV; 89Y(p,7),E=2.6-3.3 MeV; m e a s u r e d ~(E). 89y,S°Zr d e d u c e d l e v e l d e n s i t y . NUPAB 378 293. NUCLEAR REACTIONS 8 9 y ( p o l a r i z e d p , p ' ) , E = 2 1 . 1 MeV; m e a s u r e d a(E,0),A(E,0); d e d u c e d effective interaction. 8Sy l e v e l s d e d u c e d d e f o r m a t i o n parameters. M i c r o s c o p i c DWBA a n a l y s e s . NUPAB 376 183. NUCLEAR REACTIONS i6~24Mg~a~Si~4~Ar~4~4~4~Ca~46~4~5~Ti~54~56Fe~58~66~6a~64Ni~89Y~9~r~98~1~M~ 1 4 4 S m , 2 ° s P b , 2 ° S B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d G(0),A(0); d e d u c e d optical model parameters. ~6~24Mg~28Si~4~Ar~4~44~48Ca~46~48~5~Ti~54~56Fe~58~6~62~64Ni~89Y~9~Zr~98~M~44Sm~ a°sPb,2°SBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 9 4 4 . NUCLEAR REACTIONS 89y,9%r(e,e'),E n o t given; m e a s u r e d ~(0) vs m o m e n t u m t r a n s f e r . 89Y,9°Zr l e v e l d e d u c e d e f f e c t i v e E5 t r a n s i t i o n charge,current densities,configuration. PYLBB 112 40. NUCLEAR REACTIONS 96Zr(p,2n),E=18-26 MeV; m e a s u r e d ET,IT(E),77-coin; 89y(3He,3n),E=33-43 MeV; m e a s u r e d E T , I T ( E , t ) , 7 7 - c o i n ; 9 ° Z r ( 3 H e , 3 n p ) , E = 4 3 MeV; m e a s u r e d E T , I T ( O ) , T T - c o i n . 89Nb d e d u c e d levels,J,Tr,T1/2. E n r i c h e d Zr t a r g e t s , G e ( L i ) , h y p e r p u r e Ge d e t e c t o r s . S h e l l m o d e l . ZPAAD 306 171.

A 90St

AND

=

90

NUCLEAR REACTIONS 92,94,96,s8,1°°Mo,9°,se,94Zr(SLi,SB),E=90 MeV; m e a s u r e d a(E(SB)),a(0), ss,9o, 92Sr,9°,ss,94,96,SeZr d e d u c e d c h a r a c t e r i s t i c s of s t r o n g t r a n s i t i o n s . Magnetic spectrometer, e n r i c h e d t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. NUCLEAR REACTIONS 9 ° Z r ( 7 , 7 ' ) , E = 8 4 9 6 keV; I I S S n ( 7 , 7 ' ) , E = 6 3 2 5 , 6 9 8 8 keV; 12OSn('y,7'),E=6730 keV; m e a s u r e d ET,IT,77(e),a. 9°Zr,lls,la°Sn transitions d e d u c e d FT,T1/s. IANFA 46 57. NUCLEAR REACTIONS 9°,92Zr(a,a),(a,a'),E=104 MeV; m e a s u r e d a(0). 9°,92Zr d e d u c e d i s o s c a l a r quadrupole,hexadecapole transition rates. Anharmonic vibrator model,coupled-channels m e t h o d . ZPAAD 305 351. NUCLEAR REACTIONS 9°,9a,94,9%r(p,p'),E=200 MeV; m e a s u r e d a(0). 9°,ss,94,9%r d e d u c e d l e v e l s , F , p o s s i b l e g i a n t M1 r e s o n a n c e . M i c r o s c o p i c DWIA a n a l y s i s . PRVCA 26 87. NUCLEAR REACTIONS 51V,SS,6°,6SNi,6SZn,S°,ss,s4,g6Zr,92,g4,s6,sa,l°°Mo,l~°,124Sn,14°Ce(p,p'),E=200 MeV; m e a s u r e d cr(0). 51V,5S,s°,62Ni,SSZn,9°,sz,94,SSZr,92,94,ss,ss,iOOMo,12o,124Sn,.~4°Ce d e d u c e d resonances,F,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS SSSr(p,7),E=2.2-3.7 MeV; 89y(p,7),E=2.6-3.3 MeV; m e a s u r e d a(E). SSy,9°Zr d e d u c e d l e v e l d e n s i t y . NUPAB 378 293. NUCLEAR REACTIONS 9OZr(e,e'),E=37.2,60.6 MeV; m e a s u r e d a ( 0 = l S 0 ° ) . 9°Zr d e d u c e d M2 t r a n s i t i o n , B ( M 1 ) u p p e r l i m i t . PRVCA 26 1304. NUCLEAR REACTIONS 9°Zr,~SOSn,144Sm,2°sPb(p,p'),E=800 MeV; m e a s u r e d a(0). 9°Zr,te°Sn,~44Sm, a°spb,4°Ca,SeNi d e d u c e d d e f o r m a t i o n lengths,neutron,proton matrix element ratios. Optical m o d e l , D W B A a n a l y s e s . PRVCA 25 408. NUCLEAR REACTIONS 9~,t°°Mo(14C,14C),(14C,14C'),(14C,lsO),94,96,SaMo(14C,isO),E=71 MeV; m e a s u r e d a(0),a(E(160)); deduced optical model parameters, so,se,94,ss,SaZr levels deduced spectroscopic amplitudes. DWBA a n a l y s i s . PRVCA 26 500. NUCLEAR REACTIONS SSZn,9°,92,94Zr,94,ss,se,lO°Mo,124Te,138Ba,14aCe,14SNd,lS°Sm,a32Th(p,t),E=52 MeV; m e a s u r e d a ( E t , 0 ) . SSZn,SO,9~Zr,92,s4,96Mo,14OCe,144Nd,148Sm,23°Th d e d u c e d d e e p t w o - h o l e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513.

40

KEY

NUMBERS

A 90Zr

R 82Sa19

82Sc08

82TaO5

82TalO 82Ti01

90Nb

R 82Fi09 82Hu01 82TaO5

83Vi05

9OMo

D 810x01 R 82De34

9OTc

D 810xO1

D 82A101

=

90

KEYWORDS

continued

NUCLEAR REACTIONS i•••••Mg••8Si•4•Ar•4o•44•48Ca•46•48•5•Ti•54•5••e•5••6••••••4Ni•e9Y•9•Zr•9••1••M•• 1 4 4 S m , Z ° a P b , 2 ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model parameters. 160,24Mg,28Si,4°A r,4°,44,48Ca,46,48,5OTi,54,56Fe,58,6°,62,64 Ni,89y,9°Zr,98,1°°Mo,144Swi, a°8pb,Z°9Bi d e d u c e d p o i n t n u c l e o n distribution. PRVCA 26 9 4 4 . NUCLEAR REACTIONS agY,9°Zr(e,e'),E n o t g i v e n ; m e a s u r e d a t 0 ) v s m o m e n t u m t r a n s f e r . 89Y,g°Zr level deduced effective E5 t r a n s i t i o n charge,current densities,configuration. PYLBB 112 40. NUCLEAR REACTIONS lZC,160,a7Al,asSi,4°Ca,46Ti,9°Zr(aHe,t),(aHe,aHe'),E=130,170 MeV; m e a s u r e d a(Et),a(E(aHe)),o'(0), leo,27Al,asSi,4°Ca,4STi,9°Zr deduced T=0,GQR. i2N,ISF,27Si,2aP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,GDR. P R V C A 25 1253. NUCLEAR REACTIONS 9 ° Z r ( a , a ' ) , E = 9 9 . 3 MeV; m e a s u r e d a(Ea'),aT(O ). 9°Zr d e d u c e d r e s o n a n c e octupole character,J,w,7-branching. PRLTA 48 1791. NUCLEAR REACTIONS 9a,94,ae,9e,l°°Mo,9°,ga,O4Zr(aLi,aE),E=90 MeV; m e a s u r e d ~ ( E ( a B ) ) , a ( 0 ) . s8,90 92Sr,9°,92,94,96,98Zr d e d u c e d c h a r a c t e r i s t i c s of strong transitions. Magnetic spectrometer enriched t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. NUCLEAR REACTIONS 9 % r ( 3 H e , t ) , E = 4 3 . 4 MeV; m e a s u r e d G(0). 9°Nb d e d u c e d l e v e l s , J , r r . DWBA a n a l y s i s . NUPAB 385 4 4 9 . NUCLEAR REACTIONS 9 ° Z r ( p , n ) , E = 7 . 8 MeV; m e a s u r e d I ( c e ) , T l / a . 9°mNb d e d u c e d n o f e e d i n g isomer. Activation technique,mini-orange spectrometer. PRVCA 25 671. NUCLEAR REACTIONS 12C,l~O,e7A1,2aSi,4OCa,46Ti,9°Zr(3He,t),(SHe,3He'),E=130,170 MeV; m e a s u r e d a(Et),a(E(aHe)),a(0), teO,eTAl,SsSi,4°Ca,46Ti,9°Zr d e d u c e d T=O,GQR. tZN,lSF,aTsi,ZSP,4°Sc,46V, 9°Nb d e d u c e d IAS o f T=I,G D R . PRVCA 25 1253. NUCLEAR REACTIONS 14C(p,rr-),E=183 MeV; 180(pjr-),E=191 MeV; 42,48Ca,89y,gOZr(pjr-),E=206 MeV; m e a s u r e d ~r(0,E(w)),a(0). 150,19Ne,43,49Ti,9°Nb,91Mo d e d u c e d h i g h - s p i n state excitation mechanism. P R L T A 49 1314. R A D I O A C T I V I T Y 9°,9°mTc [ f r o m 92Mo(p,3n),E=43 MeV3; m e a s u r e d T1/z,flT-,TT-coin,ET,IT; d e d u c e d Q(EC),log f t . 9°Mo d e d u c e d l e v e l s , J , T r , 7 - b r a n c h i n g . ZP A A D 303 63. NUCLEAR REACTIONS 9 ° Z r ( a H e , 3 n T ) , E = 3 3 - 4 3 MeV; m e a s u r e d E T , I T ( 0 T , t ) , 7 ~ / ( t ) , n T - c o i n . 9°Mo deduced levels,T1/a,J,rr. Enriched target,Ge(Li),hyperpure Ge d e t e c t o r s . Shell-model a n a l y s i s . NUPAB 388 303. R A D I O A C T I V I T Y 9°,96mTc E f r o m 92Mo(p,3n),E=43 MeV3; m e a s u r e d T i / 2 , f l T - , 7 7 - c o i n , E % I T ; d e d u c e d Q(EC),log f t . 9°Mo d e d u c e d l e v e l s , J , T r , T - b r a n c h i n g . ZP A A D 303 63.

A 91Kr

AND

=

91

R A D I O A C T I V I T Y 86,87,ss,soBF,Sg,91,92,93KF,89,91,92,93,94Rb,93,94,95SF 94,95,96y 134Sb 136 137,138,139I, Eft. F i s s i o n products,fi-strength

137,138,139,140,141Xe,138,139,140,141,142Cs; m e a s u r e d average functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. 9~Rb

D 82AI01

9~Zr

R

9tNb

D 82Na17:

82Fa08:

R 82Ma04:

91Mo

R 82Ma07: 82Vi05:

R A D I O A C T I V I T Y 86 , 87 , 88 , 89 BT . 89. 91 . . 92 93 K r . 89. 91 . .92. 93 94 Rb, 93 , 94 , 95 S t , 94 , 95 , 96 Y, 134 Sb . 136 . 137 . . 138 139 I, 137 . 138 . 139 . . 140 141 Xe . 138 . 139 . .140. 141 142 Cs; m e a s u r e d average Eft. F i s s i o n products,fl-strength functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. NUCLEAR REACTIONS 9aMo,g°Zr,S%r,74Se(n,2n),(T,n),E=14.5 MeV; m e a s u r e d ~ ( i s o m e r ) / g ( g r o u n d s t a t e ) . 93Mo,91Zr,~TSr,75Se d e d u c e d level density spin dependence parameter. Compound nucleus decay calculations. Y A F I A 35 257. R A D I O A C T I V I T Y mNb(EC) [ f r o m M o ( n , p ) , E = r e a c t o r 3 ; m e a s u r e d E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d T~/2. Activation,mass spectrometry techniques. R A A C A 30 185. NUCLEAR REACTIONS 28Si,54Fe,SSNi(3He,3He),(3He,d),E=90 MeV; 9 ° Z r ( S H e , 3 H e ) , ( S H e , d ) , E = 8 9 . 3 MeV; ie4Sn(SHe,SHe),(SHe,d),E=89.8 MeV; m e a s u r e d ~ (0); d e d u c e d o p t i c a l p o t e n t i a l s . 29P,55Co, 59Cu,91Nb,125Sb l e v e l s d e d u c e d spectroscopic factors. DWBA a n a l y s e s . Enriched,natural t a r g e t s . NUPAB 373 377. NUCLEAR REACTIONS 9 2 M o ( 3 H e , a ) , E = 2 5 MeV; m e a s u r e d G ( E a , 0 ) . 91Mo d e d u c e d l e v e l s , L , C 2 S , configuration. Enriched target,magnetic spectrometer. DWBA a n a l y s i s . J P H G B 8 361. NUCLEAR REACTIONS 14C(p,Tr-),E=183 MeV; 180(p,Tr-),E=191 MeV; 42,4aCa,SgY,O°Zr(p,~r-),E=206 MeV; m e a s u r e d ¢(O,E(Tr)),a(e). t50,19Ne,43,49Ti,g°Nb,elMo d e d u c e d h i g h - s p i n state excitation mechanism. P R L T A 4 9 1314.

A 92Kr

D 8fiA101:

=

R A D I O A C T I V I T Y 86,87,a8,89Br,89,91,92,93Kr,89,91,92,93,94R b,93,94,95Sr,94,95,96y 134Sb,136,137 138 1391, measured average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 86,87,88,89BF,so,91,92,93K r,89,91,92,93,04 R b,93,94,95Sr 94,95,96y,134Sb 136,I37,138,139i, 137,138,139,14°,141Xe,138,139,140,141,142Cs; m e a s u r e d average Eft. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74.

137,138,139,14°,141Xe,t38,139,14°,141,14eCs; 9aRb

D 82A101:

92

41

KEY

NUMBERS

A 92Sr

D 82Kr11:

R 82Ti01:

92Zr

R 81Ju03:

82Co09:

82Cr02: 82Dj04:

82Ka22:

82Ka27 82Ma30

82Na06

82Ti01

9~Mo

D 82Be20:

R 82Dj04:

82Na06:

D 82A101:

93Rb

D 82A101

82Krli

93Sr

D 82A101

82Krll

93Nb

D 81L101 8~Re09

R 82Av05:

=

92

KEYWORDS

continued

RADIOACTIVITY 93,94,95,96,97,98,99,100Rb [ f r o m a35U(n,F)]; m e a s u r e d E3',l-/,fl-delayed n - / - , f l T - , -/-/-coin; deduced fl-strength function r o l e . 92,93,94,95,9°,97,98Sr levels deduced delayed neutron branching r a t i o s . ZPAAD 306 239. NUCLEAR REACTIONS 99,94,ga,gs,l°OMo,gO,92,94Zr(SLi,SB),E=90 MeV; m e a s u r e d cr(E(aB)),cr(O). 88,90 92Sr,9°,92,94,gs,gaZr d e d u c e d c h a r a c t e r i s t i c s of s t r o n g t r a n s i t i o n s . Magnetic spectrometer, enriched t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. NUCLEAR REACTIONS 92Zr(p,p'),E=7.08 MeV; 94Zr(p,p'),E=8.11 MeV; m e a s u r e d I(ce),ET,IT,Tl/2 for 0 + states; deduced monopole strengths. 92,94Zr l e v e l s deduced B(E0)/B(E2), configurations. S i - L i d e t e c t o r p l u s m a g n e t i c l e n s e l e c t r o n s p e c t r o m e t e r . ZPAAD 303 147. NUCLEAR REACTIONS 99,92Zr(a,a),(a,a'),E=104 MeV; m e a s u r e d a(O). 9°,92Zr d e d u c e d i s o s c a l a r quadrupole,hexadecapole transition rates. Anharmonic vibrator model,coupled-channels m e t h o d . ZPAAD 305 351. NUCLEAR REACTIONS 90,92,94,96Zr(p,p'),E=200 MeV; m e a s u r e d or(0). 9°,92,94,99Zr d e d u c e d levels, F , p o s s i b l e g i a n t M1 r e s o n a n c e . M i c r o s c o p i c DWIA a n a l y s i s . PRVCA 26 87. NUCLEAR REACTIONS 51V,58,s9,S2Ni,SSZn,99,92,94,gSzr,ga,94,96,gs,lO0Mo,i29,124Sn,149Ce(p,p,),E=200 MeV; m e a s u r e d a ( 0 ) . SiV,5a,s9,62Ni,SSZn,9°,92,°4,gSzr,ga,94,9°,gs,199Mo,ia°,124Sn,t49Ce d e d u c e d resonances,F,T,Ml character. NUPAB 388 1. NUCLEAR REACTIONS 144Sm(3He,n),E=15.3 MeV; SaNi,92Zr(p,p'),E=7.08 MeV; m e a s u r e d I(ce), ( c e ) ( t ) . 146Gd,92Zr l e v e l d e d u c e d T1/2. C e n t r o i d t i m i n g method,magnetic plus Si-Li combination electron spectrometer,composite Ni,Zr t a r g e t . NUIMA 200 253. NUCLEAR REACTIONS 9 2 Z r ( p , p ' ) , E = l 1 5 MeV; m e a s u r e d a(Ep'),cr(0). 92Zr d e d u c e d GDR,GQR, octupole,monopole,hexadecapole g i a n t r e s o n a n c e s , E W S R . DWBA a n a l y s i s . PRVCA 26 1733. NUCLEAR REACTIONS 99,199Mo(14C,14C),(14C,14C'),(t4C,lsO),94,96,gaMo(14C,lS0),E=71 MeV; m e a s u r e d cr(0),cr(E(ls0)); deduced optical model parameters. 9°,92,94,96,98Zr l e v e l s deduced spectroscopic amplitudes. DWBA a n a l y s i s . PRVCA 26 500. NUCLEAR REACTIONS SSZn,99,92,94Zr,94,gs,98,1°°Mo,la4Te,13aBa,14aCe,146Nd,iSOSm,aa2Th(p,t),E=52 MeV; m e a s u r e d cr(Et,O). 66Zn,9°,9aZr,ga,94,gSMo,149Ce,144Nd,148Sm,239Th d e d u c e d d e e p t w o - h o l e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513. NUCLEAR REACTIONS 99,94,gs,ge,l°°Mo,gO,92,94Zr(SLi,SB),E=90 MeV; m e a s u r e d cr(E(SB)),cr(O). 88,90 92Sr,9°,92,94,gs,98Zr d e d u c e d c h a r a c t e r i s t i c s of s t r o n g t r a n s i t i o n s . Magnetic spectrometer, e n r i c h e d t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. RADIOACTIVITY Nd,Mo,Ge; m e a s u r e d E-/,I'y; d e d u c e d n o e v i d e n c e f o r n e u t r i n o l e s s p r o c e s s , r i g h t h a n d e d c u r r e n t f r a c t i o n l i m i t s . 148,15°Nd,92,1°OMo d e d u c e d l i m i t on d o u b l e f l - d e c a y Tl/ 2. 7aGe d e d u c e d l i m i t o n n e u t r i n o l e s s d o u b l e f l - d e c a y T1/2. NCLTA 33 273. NUCLEAR REACTIONS 51V,SS,so,saNi,68Zn,9°,o2,o4,96Zr,ga,94,gs,98,1OOMo,12o,la4Sn,140Ce(p,p'),E=200 MeV; m e a s u r e d or(0). 51V,SS,so,aaNi,68Zn,gO,92,94,gSZr,92,94,gs,ga,lOOMo,lZo,124Sn,~40Ce d e d u c e d r e s o n a n c e s , F , T , M 1 c h a r a c t e r . NUPAB 388 1. NUCLEAR REACTIONS 69zn,gO,9~,94Zr,94,gs,gs,i°OMo,la4Te,13SBa,t42Ce,~4SNd,iS°Sm,23aTh(p,t),E=52 MeV; m e a s u r e d a ( E t , 0 ) , aSZn,96,gaZr,ga,94,gSMo,~4°Ce,144Nd,148Sm,a3OTh d e d u c e d d e e p t w o - h o l e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513.

A 93KF

AND

=

93

RADIOACTIVITY 86,87,88,89BF,89,91,92,O3K r,89,91,92,93,94 R b,93,94,95Sr,94,o5,96y,134Sb 136 137,138 139I, t37,t38,139,140,141Xe,138,139,14O,t41,142Cs; m e a s u r e d a v e r a g e Ep. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 86 87,s8,89Br,89 9t,92,93Kr 89,9192,93,94Rb,93 94,95Sr 94,95,96y134Sb136,137,138,t391 ' 137,138,139,140,14IXe,138,139,140,141,142Cs; measured average Ep. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 93,94,95,96,97,98,99,1°°Rb [ - f r o m 235U(n,F)]; m e a s u r e d E - / , I - / , f l - d e l a y e d n v - , f l T - , - / - / - c o i n ; deduced D - s t r e n g t h function r o l e . 92,93,94,95,96,97,98Sr levels deduced delayed neutron branching r a t i o s . ZPAAD 306 239. RADIOACTIVITY 86~7~88~89B~89~9~,92~93K~89~9~92~93,94Rb,93~94~95S~94~95,96Y~34Sb~36~37~3~~39~ 137,138,139,14°,141Xe,138,139,14°,141,142Cs; measured average Ep. F i s s i o n p r o d u c t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. RADIOACTIVITY 93,94,95,96,97,98,99,1°°Rb [ f r o m 235U(n,F)]; m e a s u r e d E v , I - / , f l - d e l a y e d n - / - , f l - / - , -/y-coin; deduced fl-strength function r o l e . 92,93,94,95,96,97,98Sr levels deduced delayed neutron branching r a t i o s . ZPAAD 306 239. RADIOACTIVITY 93r"Nb; m e a s u r e d TI/a. X - r a y d e c a y o b s e r v a t i o n s . RRALA 50 113. RADIOACTIVITY 93mNb; m e a s u r e d I(ce); d e d u c e d ICC s u b s h e l l r a t i o s , t r a n s i t i o n conversion probability. Low e n e r g y X - r a y , e l e c t r o n spectrometer,high purity Ge,Si Li d e t e c t o r s , 4 7 r proportional c o u n t e r . I J A R A 33 537. NUCLEAR REACTIONS 9 3 N b ( n , n ' ~ / ) , E = r e a c t o r ; m e a s u r e d ET,IT,T(0). 93Nb l e v e l s d e d u c e d 6. IANFA 46 947.

42

KEY

NUMBERS

A 93Nb

R 82PI04:

93Mo

R

93Tc

R 81Aul0:

82Fa08:

B2Fil4:

D

82AI01:

82Krll:

94Sr

D

82AI01:

82Kr07:

82Krll:

94y

D 82A101:

94Zr

R 81Ju03

82Cr02

82Dj04

82M230

82Ti01

94Mo

R

81P106: 82Dj04:

82Na06:

94Tc

D

82Be01

R 81Aul0

94RU

R 82No06

=

93

KEYWORDS

continued

NUCLEAR REACTIONS 49Ti,51V,59Co,STsr,gaNb,e09Bi(e,e),E=175-325,500 MeV; m e a s u r e d cr(0,E). 49Ti,51V,STSr,93Nb d e d u c e d valence nucleon rms,charge radii. PWBA,DWBA analyses,meson exchange effects. PRVCA 25 2318. N U C L E A R R E A C T I O N S 92Mo,9°Zr,86Sr,VdSe(n,2n),(T,n),E=14.5 MeV; m e a s u r e d cr(isomer)/(~(ground state). 93Mo,9~Zr,S7Sr,75Se d e d u c e d level density spin dependence parameter. Compound nucleus decay calculations. Y A F I A 35 2 5 7 . NUCLEAR REACTIONS 93Nb(SHe,xn),E=14-36 MeV; measured a(E) for x=2,3; deduced preequilibrium process role. 93,94Tc d e d u c e d isomer production ratios. Activation technique. Hybrid,e×citon models. J I N C A 4 3 2611. N U C L E A R R E A C T I O N S 4aCa,92Mo(c~,t),E=26-30 MeV; 4SCa,gaMo(aHe,d),E=16 MeV; m e a s u r e d absolute (~(0). 49Se,93Tc l e v e l d e d u c e d normalizations. Enriched targets. N U P A B 3 8 9 18.

A 94Rb

AND

=

94

R A D I O A C T I V I T Y 86,87,88,e9Br,89,91 92,93Kr 89 91 92 93,94Rb 93 94 9 5 S r 94 95 96y 134Sb 136 t37 138 1391, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; measured average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector system. N S E N A 80 7 4 . R A D I O A C T I V I T Y 93,94,95,96,97,gs,99,1°°Rb [ f r o m Z35U(n,F)]; m e a s u r e d Ev,IT,fl-delayed nT-,fl-y-, "yv-eoin; deduced fl-strength function r o l e . 92,93,94,95,96,97,98Sr l e v e l s deduced delayed neutron branching ratios. ZPAAD 396 239. R A D I O A C T I V I T Y 86•8••8••89Br••9•9••9••93Kr•89•9• 9••93••4R••93 94••5S• 94•95•96Y••34Sb •36•137••38••3•I• /37,tss,t39,14°,t41Xe,13s,139,14°,t41,142Cs; measured average Eft. F i s s i o n produets,fl-strength functions input,Si-Li detector system. NSENA 80 7 4 . R A D I O A C T I V I T Y 95Rb E f r o m m a s s s e p a r a t o r ] ; measured fl-delayed nT-coin,Ev,TT-eoin. 94Sr deduced levels,J,~,v-branching. Tof,3He ionization chamber,Ge(Li) spectrometer. Z P A A D 305 93. R A D I O A C T I V I T Y 93,94,95,9s,97,98,99100Rb E f r o m 2 3 5 U ( n , F ) ] ; m e a s u r e d Ev,IT,fl-delayed nT-,flT-, -~7-coin; deduced fl-strength function role. 92,93,94,95,9s,97,gSSr l e v e l s d e d u c e d delayed neutron branching ratios. ZPAAD 306 239. R A D I O A C T I V I T Y 86 , 87 , 88 , 89 B r . 89. .91. 92 93 K r . B9. 91 . .92. 93 94 R b , 93 , 94 , 95 S r , 94 , 95 , 9S Y, 134 S b . 136 . 137 . . 138 139 I, 137 138 139 140 141 138 139 140 141 142 . . . . Xe . . . . . Cs; m e a s u r e d average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector system. N S E N A 80 7 4 . N U C L E A R R E A C T I O N S 9 2 Z r ( p , p ' ) , E = 7 . 0 8 MeV; 9 4 Z r ( p , p ' ) , E = 8 . 1 1 MeV; m e a s u r e d I(ce),ET,I%Tw2 for 0 + states; deduced monopole strengths. 9e,94Zr levels deduced B(E0)/B(E2), configurations. Si-Li detector plus magnetic lens electron spectrometer. Z P A A D 3 0 3 147. N U C L E A R R E A C T I O N S 9 ° , g a , 9 4 , 9 % r ( p , p ' ) , E = 2 0 0 MeV; m e a s u r e d cr(0). 9°,92,94,96Zr d e d u c e d levels, F,possible giant M1 r e s o n a n c e . Microscopic DWIA analysis. P R V C A 3 6 87. NUCLEAR REACTIONS Slv,SS,6°,SaNi,68Zn,9°,~a,94,96Zr,Oa,9496,ga,tOOMo,12o,~24Sn,idOCe(p,p%E=~00 MeV; measured (7(0). 5 1 V , 5 8 , 6 D , S 2 N i , 6 8 Z n , 9 ° , 9 2 9 4 , 9 6 Z r , 9 2 9 4 , g s , 9 8 , 1 0 0 M o 1 2 0 , 1 2 4 S n , 1 4 0 C e deduced resonances,F,T,M1 character. N U P A B 3 8 8 I. N U C L E A R R E A C T I O N S 92,1°°Mo(14C,14C),(14C,14C'),(14C,160)94,969aMo(14CISo),E=71 MeV; m e a s u r e d o-(0),a(E(160)); deduced optical model parameters. 9°,92,94,96,98Zr levels deduced spectroscopic amplitudes. DWBA a n a l y s i s . P R V C A 26 5 0 0 . N U C L E A R R E A C T I O N S 92 94 96 98 100 Mo 99 92 94 Z r ( 6 Li 8 B) E=9O MeV" m e a s u r e d o r ( E (8B ) ) ( 7 ( 0 ) 88 90 9aSF . 90. 92 . . 94. 96 98 Z r d e d u c e d c h a r a c t e r i s t i•c~s .' o f s t'r o n g' t r a n s i t i.o '.n s . Magnetic s p e c ~t r o- m e"t e r , * enriched target. DWBA a n a l y s i s . NUPAB 376 309. N U C L E A R R E A C T I O N S 92,94,97,98Mo(t,p),E=17 MeV; m e a s u r e d cr(0). 94,96,9fl,l°OMo d e d u c e d l e v e l s , J , ~,two-nueleon transfer strengths. DWBA a n a l y s i s . PRVCA 24 2475. N U C L E A R R E A C T I O N S 51V,SS,6°,SaNi,68Zn,g°,92,94,96Zr,O2,o4,gs,98,1OOMo,12o,~24Sn,14OCe(p,p,),E=200 MeV; m e a s u r e d G ( 0 ) . 51V,58,6°,62Ni,68Zn,9°,92,94 96Zr,ga,94,gs,gs,i0OMo,lZ0 124Sn,140Ce d e d u c e d resonanees,F,T,M1 character. N U P A B 3 8 8 1. NUCLEAR REACTIONS 68zn,g°,92,94Zr,94,96,9s,~°°Mo,124Te,13SBa,142Ce,14SNd,lSOSm,23aTh(p,t),E=52 MeV; m e a s u r e d (7(Et,0). S S Z n , 9 ° , 9 2 Z r , g a , 9 4 , 9 6 M o , 1 4 ° C e a 4 4 N d , 1 4 8 S m a 3 O T h d e d u c e d deep two-hole states. Enriched targets. N U P A B 3 7 6 513. R A D I O A C T I V I T Y 94Tc E f r o m 93Nb(a,3n),E=45 MeV]; measured ET,I%7(0),cr(E~/),TT-coin,TI/2; deduced levels,J,Tr,7-branching. NUPAB 373 483. NUCLEAR REACTIONS 93Nb(3He,xn),E=14-36 MeV; measured (r(E) f o r x=2,3; deduced preequilibrium process role. 93,94Te d e d u c e d isomer production ratios. Activation technique. Hybrid,exciton models. J I N C A 4 3 2611. NUCLEAR REACTIONS 58Ni(4°Ca,n2p),E=135 MeV; m e a s u r e d ET,I-/,vv-eoin,fl-delayed Ep,Ip, P7 coin,pT(t). 95pd deduced isomer decay,J,Tr,T1/a,Q(EC),log ft,v-multipolarity. 95Rh deduced Iv,v-branching. 94RO l e v e l d e d u c e d J , T r , ~ / - b r a n c h i n g . Enriched t a r g e t . Z P A A D 305 289.

43

KEY

NUMBERS

A g4Rh

94pd

D 82Ku15

D

82Ku15

D 82Kr07

82Krll

95Sr

D 82A101

82Krll 95y

D 82A101

82PRO1 95Rh

D 82Ku15

R 82No06

95pd

D 82Ku15:

R 82No06:

D 82Kr11:

96Sr

D 82Krll:

96y

D 82A101:

96Zr

D 81Zd01:

R 82Cr02:

94

continued

I(X-ray); deduced log f t . 95,SSRh,SS,SsPd d e d u c e d levels,JJr,'~-branching. On-line mass separation. Z P A A D 308 21. R A D I O A C T I V I T Y 94Rh(f+p)•94Pd(f+)•(EC)•95mPd(fl+p)•9••d(•+)•(EC)•96Ag(•+p)•97Cd(fl+p)•97 Ag(•+)' ~SAg(fl+),99Cd(fl+p),eSmAg(f+),(EC),'°2In(fl+),(Ee),i°OIn(fl+p) [ f r o m 5 s , 6 ° , ~ a N i , ~ 3 , ~ S C u ( 4 ° C a , x n y p ) , E=4 MeV/nucleon]; measured T1/~,ET,I~,fl-delayed Ep,Ip,fl~,-,p(X-ray)-coin,E(X-ray), l(X-ray); deduced log f t . 95,SSRh,SS,ssPd d e d u c e d levels,Jjr,7-branching. On-line mass separation. Z P A A D 308 21.

=

95

R A D I O A C T I V I T Y 95Rb [ f r o m m a s s s e p a r a t o r 3 ; m e a s u r e d f l - d e l a y e d n ' 7 - c o i n , E % ~ / ~ / - c o i n . 94Sr deduced levels,J,Tr,7-branching, Tof,3He i o n i z a t i o n e h a m b e r , G e ( L i ) s p e c t r o m e t e r . ZPAAD 305 93. R A D I O A C T I V I T Y 93,94,95,96,97,98,99,1°°Rb [ f r o m a35U(n,F)3; m e a s u r e d E%l%fl-delayed nT-,fl~-, ~/~/-coin; d e d u c e d fl-strength function r o l e . 92,sa,94,95,96,97,SSSr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y 86,ST,SS,S9Br,8°,91,92,93Kr,89,91,92,93,94 R b,93,94,95Sr,94,95,96y,134Sb,136,137,138,139I, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 93,94,95,9s,97,98,°9,1°ORb [ f r o m 235U(n,F)3; m e a s u r e d ET,l%f-delayed n~-,f~/-, ~7-coin; deduced f-strength function r o l e . 92,93,94,95,96,97,SSSr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y ~7~88~89Br'~9~9~'9a~93Kr'89'9~92~93~94Rb'93'94~95Sr~94~95~9~Y~34Sb~3~37~3~'~39I~ 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average Eft. F i s s i o n products,f-strength functions input,Si-Li detector s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 95my,13'mSb [ f r o m 238U(~/,F),E=50 MeV b r e m s s t r a h l u n g ] ; m e a s u r e d E%I%T,/~. Pulsed electron beam,rotating 238U t a r g e t , G e ( L i ) s p e c t r o m e t e r . NUIMA 192 4 4 7 . R A D I O A C T I V I T Y 94Rh(fl+p)~94Pd(f+)~(EC)~95mPd(f+p)~96Pd(fl+)~(EC)~6Ag(f+p)~97Cd(~+p)~97Ag(~+)~ 9SAg(fl+),99Cd(fl+p),99mAg(f+),(EC),l°2In(f+),(EC),lO°In(f+p) [ f r o m 5 s , s ° , S e N i , 6 3 , S 5 C u ( 4 ° C a , x n y p ) , E=4 MeV/nucleon]; measured Tl/~,E~/,IT,fl-delayed Ep,Ip,flT-,p(X-ray)-coin,E(X-ray), l(X-ray); deduced log f t . 95,96Rh,SS,ssPd d e d u c e d levels,Jjr,7-branching. 0n-line mass separation. Z P A A D 308 21. NUCLEAR REACTIONS 5 8 N i ( 4 ° C a , n 2 p ) , E = 1 3 5 MeV; m e a s u r e d E T , I ~ / , 7 " y - c o i n , f l - d e l a y e d Ep,Ip, pT-coin,p~,(t). 95pd d e d u c e d isomer decay,Jjr,T1/2,Q(EC),log ft,~-multipolarity. 95Rh deduced I%~/-branching. 94Ru l e v e l d e d u c e d J J r , ~ / - b r a n e h i n g . E n r i c h e d t a r g e t . ZPAAD 305 289. R A D I O A C T I V I T Y 94R h(fl+ p),94 P d ( f +),(EC),95m P d ( f + p ) , 9 6 p d ( f +),(EC),SSA g ( f + p),97Cd(fl + p ) , 9 7 A g ( f +), SSAg(t~+),99Cd(fl+p),99mhg(13+),(EC),l°aln(l~+),(EC),l°OIn(f+p) [from 58,a°,62Ni,63,65Cu(4°Ca,xnyp), E=4 MeV/nucleon3; measured Tl/e,E'y,IT,fl-delayed Ep,Ip,fT-,p(X-ray)-coin,E(X-ray), I(X-ray); deduced log f t . 95,96Rh,SS,SSpd d e d u c e d levels,J,rr,7-branching. 0n-line mass separation. Z P A A D 308 21. NUCLEAR REACTIONS 5 a N i ( 4 ° C a , n 2 p ) , E = 1 3 5 MeV; m e a s u r e d E ~ , I ~ , , ~ / ' y - c o i n , f l - d e l a y e d Ep,Ip, p ' y - c o i n , p T ( t ). 95pd d e d u c e d isomer decay,Jjr,Tl/z,Q(EC),log ft,3'-multipolarity. 95Rh deduced I%7-branching. 94Ru l e v e l d e d u c e d J , T r , ~ / - b r a n c h i n g . E n r i c h e d t a r g e t . Z P A A D 305 289.

A 96Rb

=

KEYWORDS

R A D I O A C T I V I T Y 94Rh(f+p)~94Pd(fl+)~(EC)~95mPd(f+p)~9~Pd(f+)~(EC)~96Ag(f+p)~9~Cd(fl+p)~97Ag(f+)~ 98Ag(f+),99Cd(fl+p),99mAg(f+),(EC),l°aIn(fl+),(EC),~°°In(fl+p) Cfrom 5 a , 6 ° , S Z N i , s a , 6 5 C u ( 4 ° C a , x n y p ) , E=4 MeV/nucleon]; measured T,/a,E~,I3,,fl-delayed E p , I p , f ' y - , p ( X - r a y ) - c o i n , E ( X - r a y ) ,

A 95Rb

AND

=

96

R A D I O A C T I V I T Y 93,94,95,96,97,98,99,1°°Rb [ f r o m 235U(n,F)]; m e a s u r e d E~,,I~/,fl-delayed n 3 ' - , f l ' y - , "y~-eoin; deduced fl-strength function r o l e . 92,93,94,95,96,97,9eSr l e v e l s deduced d e l a y e d neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y 93,94,95,96,97,98,99,1°°Rb [ f r o m 235U(n,F)J; m e a s u r e d E%I%fl-delayed n~-,fl~/-, 77-coin; deduced fl-strength function r o l e . g2,93,94,ss,96,97,gSSr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y es,eT,ee,eSBr,e9,sl,oa,93Kr,e9,st,92,93,94 R b,93,94,95Sr,g4,95,g°Y,t34Sb,136,137,13s,139I, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average Ep. F i s s i o n products,fl-strength functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 96Zr; m e a s u r e d d o u b l e f l - d e c a y T , / z l i m i t . IANFA 4 5 1856. NUCLEAR REACTIONS 9o,sa,94,SSZr(p,p'),E=200 MeV; m e a s u r e d a(0). 9°,92,94,96Zr d e d u c e d l e v e l s , F , p o s s i b l e g i a n t M1 r e s o n a n c e . M i c r o s c o p i c DWIA a n a l y s i s . P R V C A 26 87.

44

KEY

NUMBERS

A 96ZF

R 82Dj04:

82Ma30:

82Ti01:

96Nb

R 81Ar24:

96Mo

R

81F106: 82Dj04:

83Na06:

9SRh

D 82Ku15:

96pd

D 82Ku15:

9SAg

D 82Ku15:

D 82Krll:

97Sr

D 82Kr11:

97Tc

R 82Ka26:

97pd

R 82Fe01:

9TAg

D 82Ku15:

97Cd

D 82Ku15:

D 82Ka03:

96

continued

=

97

R A D I O A C T I V I T Y 93,94,95,96,97,98,99,t°°Rb [ f r o m 235U(n,F)3; m e a s u r e d E ` / , I T , f l - d e l a y e d n ` / - , f l T - , -/-/-coin; deduced fl-strength function r o l e . 92,93,94,95,96,97,98Sr levels deduced delayed neutron branching r a t i o s . ZPAAD 306 239, R A D I O A C T I V I T Y 93,s4,95,96,97,98,99,~°°Rb [ f r o m ZaSu(n,F)3; m e a s u r e d E % ! 7 , f l - d e l a y e d n - / - , f l - / - , -/-/-coin; deduced fl-strength function r o l e . 92,93,94,95,96,97,988F levels deduced delayed neutron branching r a t i o s . ZPAAD 306 239. NUCLEAR REACTIONS 97Mo(p,n-/),E=2-5.2 MeV; m e a s u r e d E % l % n ` / - , ` / - / - c o i n , - / ( 0 ) . 97Tc d e d u c e d l e v e l s , J , r r , d . E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . PRVCA 26 1451. NUCLEAR REACTIONS 96Ru(3He,2n),E ~ 20 MeV; m e a s u r e d ET,I%`/`/-eoin. 97pd deduced levels,J,rr, configuration. ZFAAD 305 57. R A D I O A C T I V I T Y 94Rh(fl+p)~94~d(fl+)~(E~)~95mPd(~+p)~96Pd(~)~(EC)~96Ag(~+p)~97Cd(~+p)~97Ag(~+)~ 98Ag(fl+),99Cd(fl+p),99mAg(fl+),(EC),l°aIn(fl+),(EC),l°9In(fl+p) [ f r o m s s , 6 ° , S a N i f i 3 , 6 5 C u ( 4 ° C a , x n y p ) , E=4 M e V / n u c l e o n 3 ; measured Tt/z,ET,I-/,fl-delayed Ep,lp,flT-,p(X-ray)-coin,E(X-ray), I ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,96,98Pd d e d u c e d l e v e l s , J , r r , ` / - b r a n c h i n g . On-line mass s e p a r a t i o n . ZPAAD 308 21. R A D I O A C T I V I T Y 94Rh(fl+p)~94Pd(fl+)~(EC)~95mPd(~+p)~96~d(~+)~(EC)~96Ag(~+p)~97Cd(~+p~'97Ag(~+)' 9aAg(fl+),99Cd(fl+p),99mAg(fl+),(EC),tOeIn(fl+),(EC),l°°In(fl+p) [ f r o m 5s,6°,SaNifi3,65Cu(49Ca,xnyp), E=4 M e V / n u c l e o n ] ; measured Tl/z,E-/,I-/,fl-delayed E p , I p , f l - / ~ , p ( X - r a y ) - c o i n , E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,96,sSpd d e d u c e d l e v e l s , J , r r , ` / - b r a n c h i n g . On-line mass s e p a r a t i o n . ZPAAD 308 21.

A 9SRb

=

KEYWORDS

NUCLEAR REACTIONS 51V,58,69,62Ni,68Zn,9°,gz,94,96Zr,92,94,9s,98,1°gMo,12°,124Sn,14°Ce(p,p'),E=200 MeV; m e a s u r e d a(O). 51V,58,6°,6~Ni,SSZn,96,92,94,96zr,gE,94,96,98,i99Mo,129,124Sn,14°Ce d e d u c e d resonances,F,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 92,1°°Mo(14C,14C),(14C,14C'),(14C,160),94,96,gSMo(14C,160),E=71 MeV; m e a s u r e d cr(0),cr(E(160)); d e d u c e d optical model parameters. 99,92,9%96,gSzr l e v e l s d e d u c e d spectroscopic amplitudes. DWBA a n a l y s i s . PRVCA 26 fi00. NUCLEAR REACTIONS 9a,94,96,go,166Mo,99,92,94Zr(SLi,SB),E=90 MeV; m e a s u r e d cr(E(SB)),cr(0). 88,90 9ZSr,9°,92,94,96,98Zr d e d u c e d c h a r a c t e r i s t i c s o f s t r o n g t r a n s i t i o n s . M a g n e t i c s p e c t r o m e t e r , enriched t a r g e t . DWBA a n a l y s i s . NUPAB 376 309. NUCLEAR REACTIONS 199Mo(p,n-/),E=l.2-3.6 MeV; 9 6 Z r ( p , n T ) , E = l . 3 - 5 . 1 MeV; m e a s u r e d ET,I`/, cr(ET). 1°°Te,96Nb d e d u c e d l e v e l s , c o n f i g u r a t i o n . P a r a b o l i c r u l e . FZKAA 13 38. NUCLEAR REACTIONS 92,94,97,96Mo(t,p),E=17 MeV; m e a s u r e d ~(0). 94,96,99,re°Ms d e d u c e d levels,d, rr,two-nucleon transfer s t r e n g t h s . DWBA a n a l y s i s . PRVCA 24 2475. NUCLEAR REACTIONS 51V,SS,~°,SaNi,68Zn,96,92,94,96Zr,92,94,96,gs,l°9Mo,leg,le4Sn,149Ce(p,p'),E=200 MeV; m e a s u r e d or(0). 51V,SS,69,62Ni,68Zn,99,92,94,96Zr,92,94,96,98,1°°Mo,lZ°,124Sn,14OCe d e d u c e d resonances,r,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 66Zn,99,92,94Zr,94,ge,gs,19°Mo,lZ4Te,138Ba,*42Ce,146Nd,15°Sm,~3aTh(p,t),E=52 MeV; m e a s u r e d ¢r(Et,0). 6%n,9°,gazr,gZ,9%96Mo,~4°Ce,~4~Nd,~4SSm,aa°Th d e d u c e d d e e p t w o - h o I e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513. R A D I O A C T I V I T Y 94Rh(fl~p)~4Pd(fl+)~(E~)~95mPd(~+p)~96Pd(~+~(E~)'96Ag(~+p)~97Cd(~+p)~97Ag(~+)~ 99Ag(fl+),99Cd(fl+p),99mAg(fl+),(EC),~°~In(fl+),(EC),~69In(fl+p) [ f r o m 58,~°,SZNifi3,aSCu(4°Ca,xnyp), E=4 M e V / n u c l e o n ] ; measured T ~ / u , E T , I - / , f l - d e l a y e d EpJp,flT-,p(X-ray)-coin,E(X-ray), I(X-ray); deduced log f t . 95,96Rh,98,ssPd d e d u c e d l e v e l s , J , r r , - / - b r a n c h i n g . On-line mass s e p a r a t i o n . ZPAAD 3011 21. R A D I O A C T I V I T Y 94 Rh(fl +p), 04 Pd(fl +),(EC), 95m Pd(fl + p), 96 Pd(fl +),(EC), 96 Ag(fl + p), 97 Cd(fl +p), 97 Ag(fl +), 96Ag(fl+),99Cd(fl+p),SamAg(fl+),(EC),l°eln(fl+),(EC),l°°In(fl+p) [ f r o m 58,6°,SaNi,Sa,65Cu(49Ca,xnyp), E=4 M e V / n u c l e o n ] ; measured T~/e,ET,I-/,fl-delayed Ep,Ip,flT-,p(X-ray)-coin,E(X-ray), I ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,96,ssPd d e d u c e d l e v e l s , J , T r , 7 - b r a n c h i n g . 0n-line mass s e p a r a t i o n . ZPAAD 308 21. RADIOACTIVITY 94Rh(fl~p)~94Pd(~+)'(EC)~95rnPd(~+p)~96Pd(~+)~(EC)~96Ag(~+p)~97Cd(~+p)'9~Ag(~+)~ 9SAg(fl+),99Cd(fl+p),99mAg(fl+),(EC),~°~In(fl+),(EC),~°SIn(fl+p) [ f r o m 58,e6,SaNi,63,SSCu(46Ca,xnyp), E=4 M e V / n u e l e o n 2 ; measured T,/z,ET,I-/,fl-delayed EpJp,flT-,p(X-ray)-coin,E(X~ray), I ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,96,sSpd d e d u c e d l e v e l s , J , r r , - / - b r a n c h i n g . On-line mass s e p a r a t i o n . ZPAAD 308 21.

A 97Rb

AND

=

98

R A D I O A C T I V I T Y 98Rb [ f r o m i s o t o p e s e p a r a t o r 3 ; 9SSr [ f r o m 98Rb(fl-decay),isotope s e p a r a t o r ] ; 9Sy [ f r o m 98Sr(fl-decay),isotope separator]; measured ET,I`/,I(ee),7`/(O),fl`/(t). 9SZr d e d u c e d levels,Tl/z,,/-branching,B(EE),B(EO),J,Tr,shape c o e x i s t e n c e . ZPAAD 304 293.

45

KEY

NUMBERS

A 98Rb

D 82Krll:

98St

D 82Ka03:

82Krll: 9Sy

D 82Ka03:

98Zr

D 82Ka03:

R 82Ma30:

82Ti01

98Mo

82Dj04

82Sa19

98Tc

R 82Ar12

~spd

D 82Ku15

R 82Th01

9SAg

D 82Ku15

D 82Krlt

99y

D 82Mo16

99Zr

D 82Ba36

99Nb

D 83Ba36

99Mo

D 80Yal0 81Si15 81Yo08 82Ba36

R 81F106

=

98

KEYWORDS

continued

R A D I O A C T I V I T Y 93,94,95,96,97,ss,99,1°°Rb [ f r o m SaSU(n,F)]; m e a s u r e d Ev,Iv,fl-delayed nT-,flV-, 7~/-coin; deduced B-strength function r o l e . 92,93,g4,ah,as,97,SaSr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y 9ORb [ f r o m i s o t o p e s e p a r a t o r 3 ; 9aSr [ f r o m 9 a R b ( f l - d e c a y ) , i s o t o p e s e p a r a t o r ] ; Say [ f r o m 9SSr(fl-decay),isotope separator3; measured E-y,I^/,I(ce),77(0),flT(t). SaZr d e d u c e d levels,Tl/z,7-branehing,B(E2),B(EO),J,Tr,shape c o e x i s t e n c e . Z P A A D 3 0 4 293. R A D I O A C T I V I T Y 93,94,95,96,97,98,99,100Rb [ f r o m ZaSu(n,F)]; m e a s u r e d ET,IT,fl-delayed nT-,flT-, 7~-coin; deduced B-strength function r o l e . 92,g2,94,ah,aS,97,gSsr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y 9SRb [ f r o m i s o t o p e s e p a r a t o r ] ; 9SSr [ f r o m 9 S R b ( f l - d e c a y ) , i s o t o p e s e p a r a t o r ] ; Say [ f r o m 9asr(fl-decay),isotope separator3; measured E T , l % I ( c e ) , 7 ~ ( 0 ) , f l T ( t ) . 9SZr d e d u c e d levels,Tl/z,v-branching,B(E2),B(E0),J,rr,shape coexistence. Z P A A D 3 0 4 293. R A D I O A C T I V I T Y 9SRb [ f r o m i s o t o p e s e p a r a t o r 2 ; aesr [ f r o m a S R b ( f l - d e c a y ) , i s o t o p e s e p a r a t o r ] ; Say [ f r o m 9asr(fl-decay),isotope separator2; measured ET,IT,I(ce),77(0),fl~/(t). aSZr d e d u c e d levels,Tl/e,v-branching,B(E2),B(E0),J,rr,shape c o e x i s t e n c e . Z P A A D 3 0 4 293. NUCLEAR REACTIONS se,I°°Mo(14C,14C),(14C,laC'),(14C,160),94,ss,aSMo(14C,160),E=71 MeV; m e a s u r e d a(0),ff(E(leo)); deduced optical model parameters. 9°,ss,94,9e,98Zr levels deduced spectroscopic amplitudes. DWBA a n a l y s i s . P R V C A 26 500. NUCLEAR REACTIONS 92,94,96,9s,t°°Mo,9°,sa,94Zr(SLj,SB),E=90 MeV; m e a s u r e d a(E(SB)),~(0). 88,90, 92Sr,9°,ga,s4,96,SSZr d e d u c e d characteristics of strong transitions. Magnetic spectrometer, enriched t a r g e t . DWBA a n a l y s i s . N U P A B 376 309. NUCLEAR REACTIONS 51v,SS,6°,SaNi,SaZn,9°,9z,g4,aSzr,aa,94,os,os,l°°Mo,le°,la4Sn,14°Ce(p,p'),E=200 MeV; m e a s u r e d o'(0). 51v,SS,6°,SZNi,68Zn,SD,as,a4,96Zr,SZ,94,os,sa,l°SMo,leo,124Sn,14°Ce d e d u c e d resonances,F,T,Ml character. N U P A B 388 1. NUCLEAR REACTIONS 1 ~ ' ~ 4 M g ~ a ~ S i ' 4 ~ A r ~ 4 ~ 4 ~ 4 ~ C a ' 4 6 ~ 4 ~ ' ~ T i ~ 6 F e ' ~ a ~ 6 ~ ' 6 a ' 6 4 N i ~ Y ~ 9 ~ Z r ~ 9 ~ ' 1 ~ M ~ 1 4 4 S m , Z ° s p b , Z O O B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model parameters. 160,24 Mg,aaSi,4° A r,4°,44,4 SCa,46,4a,5°Ti,54,56Fe,hS,6°,ea,64 Ni,SSy,96zr,gS,1 ° ° M s , 1 4 4 S i n , Z°spb,a°aBi deduced point nucleon distribution. P R V C A 26 9 4 4 . NUCLEAR REACTIONS a S M o ( p , n ) , E = 2 . 4 - 4 MeV; m e a s u r e d ET,IT,I(ee),~r(ET,E). aSTc deduced levels,J,~r,7-branching,?-multipolarity. Ge(Li),hyperpure Ge d e t e c t o r s , S i - L i spectrometer. PHSTB 26 57.

RADIOACTIVITY ~Rh(fl+p)~4~d(fl+)~(E~95m~d(~+p)~6~d(~+)~(E~)~6Ag(~+p)~97Cd(~+p)~7 ~g(~+)~ aaAg(fl+),aacd(fl+p),gamAg(fl+),(EC),lOZIn(fl+),(EC),l°°In(fl+p) [ f r o m 5 s , 6 ° , 6 Z N i , S a , S h C u ( 4 ° C a , x n y p ) , E=4 MeV/nucleon]; measured Tl/z,ET,I%fl-delayed Ep,Ip,flV-,p(X-ray)-coin,E(X-ray), I(X-ray); deduced log f t . 95,gSRh,as,aSpd d e d u c e d levels,J,rr,v-branching. On-line mass separation. Z P A A D 308 21. NUCLEAR REACTIONS 9 S R u ( 1 6 0 , l ¢ C ) , ( 1 6 0 , 1 a C ) , ( 1 6 0 , l Z C ) , l o g p d ( l e 0 , t 4 C ) , E = 7 0 MeV; m e a s u r e d o-(E(IzC)),a(E(laC)),a(E(14C)). 9s,oa,l°°Pd d e d u c e d level,Q,mass excess, l°6cd deduced mass e x c e s s . Q3D m a g n e t i c spectrometer. P R V C A 25 331. R A D I O A C T I V I T Y ~4Rh(fl+p)'94~d(fl+)~(EC)~5m~d(~+p)~sPd(~+)~(EC)'~Ag(~+p)~7Cd(~+p)~7 Ag(~+)~ 92Ag(fl+),99Cd(fl+p),agmAg(fl+),(EC),l°zIn(fl+),(EC),laoIn(fl+p) [ f r o m 5 s , 6 ° , 6 Z N i , S a , S 5 C u ( 4 a C a , x n y p ) , E=4 MeV/nucleon]; measured T1/a,E%I%fl-delayed Ep,Ip,fl~-,p(X-ray)-eoin,E(X-ray), I(X-ray); deduced log f t . 05,9SRh,96,aspd d e d u c e d levels,J,~r,v-branching. On-line mass separation. Z P A A D 308 21.

A SSRb

AND

=

99

R A D I O A C T I V I T Y 93,94,95,96,97,98,99,1°°Rb [ f r o m Za5U(n,F)3; m e a s u r e d E v , I ~ / , f l - d e l a y e d n~/-,flV - , VT-coin; deduced B-strength function r o l e . 9e,93,94,95,s6,97,9SSr l e v e l s d e d u c e d delayed neutron branching r a t i o s . Z P A A D 306 239. R A D I O A C T I V I T Y Say(B-); m e a s u r e d E v , I v ( t ) F / V - c o i n ; d e d u c e d i s o m e r T 1 / z , l e v e l s , v - b r a n c h i n g , rotational b a n d . Z P A A D 306 183. fiT(t). 99Nb,SSMo l e v e l s d e d u c e d T1/a, R A D I O A C T I V I T Y 99Zr(fl-) [ f r o m 99y d e c a y ] ; m e a s u r e d B(X). Z P A A D 306 113. R A D I O A C T I V I T Y 99Zr(B-) [ f r o m 99y d e c a y ] ; m e a s u r e d f i r ( t ) . 99Nb,99Mo l e v e l s d e d u c e d Tl/2, B(X). Z P A A D 306 113. R A D I O A C T I V I T Y 99M0; m e a s u r e d ET,IT; deduced B - b r a n c h i n g . 99Te l e v e l s d e d u c e d 7 b r a n c h i n g . YTHLD 2 41. E%1% gSTc t r a n s i t i o n d e d u c e d a b s o l u t e I% JRACB 67 61. R A D I O A C T I V I T Y gSMo; m e a s u r e d R A D I O A C T I V I T Y 99Mo [ f r o m 9SMo(n,v)3; m e a s u r e d E v , l % E ( X - r a y ) , I ( X - r a y ) . 99mTc d e d u c e d d e c a y dependence on chemical effects. Molybdenum m e t a l , M o O 3 t a r g e t s . R R A L A 48 303. R A D I O A C T I V I T Y 99Zr(fl-) [ f r o m 99y d e c a y ] ; m e a s u r e d fl~,(t). 99Nb,SaMo l e v e l s d e d u c e d T1/e, B(X). Z P A A D 306 113. NUCLEAR REACTIONS 9z,a4,97,aSMo(t,p),E=17 MeV; m e a s u r e d or(0). 94,ss,gg,i°aMo d e d u c e d l e v e l s , J , ~r,two-nucleon transfer strengths. DWBA a n a l y s i s . P R V C A 24 2 4 7 5 .

46

KEY

NUMBERS

AND

A 99Mo

R 82Ha41

99Tc

D 80Yal0 81Si15 81Yo08 82Ge01

99Rh

R 82Ka15

99pd

R 82Th01

99Ag

D 82Ku15

99Cd

D 82Ku15

D 82Krll

XOOMo

D 82Be20

R 81FI06 82Dj04

82Sa19

,00T.c

R 8IAr24: 82Ma27:

1OORu

R 82Co15:

19opd

R 82An09:

82Th01:

~OOin

D 82Ku15:

99

continued

NUCLEAR REACTIONS l ° ° M o ( p o l a r i z e d d,t),98Mo(polarized d,p),E=16 MeV; m e a s u r e d a(0),a(Ep), cr(Et); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 99Mo l e v e l s d e d u c e d J,Tr,S. PRVCA 26 834. R A D I O A C T I V I T Y 99Mo; m e a s u r e d E%Iv; d e d u c e d f l - b r a n c h i n g . 9gTc levels d e d u c e d v - b r a n c h i n g . YTHLD 2 41. RADIOACTIVITY 99Mo; m e a s u r e d E%I% 99Te t r a n s i t i o n d e d u c e d a b s o l u t e IV. JRACB 67 61. R A D I O A C T I V I T Y 99Mo [ f r o m 9SMo(n,v)3; m e a s u r e d E % l % E ( X - r a y ) , I ( X - r a y ) . 99mTc d e d u c e d decay dependence on chemical effects. Molybdenum m e t a l , M o 0 3 t a r g e t s . RRALA 48 303. R A D I O A C T I V I T Y 99roTe; m e a s u r e d I(ee); d e d u c e d c h e m i c a l enviornment e f f e c t o n E3 transition. ZETFA 82 362. NUCLEAR REACTIONS 9~,gSMo(SLi,3n),E=18-34 MeV; m e a s u r e d E v , I T , 3 ' ( 0 ) , n 3 , - , 7 ~ - c o i n . 99,~°lRh d e d u c e d levels,J,Tr. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . PRVCA 26 138. NUCLEAR REACTIONS 9 S R u ( ' ~ 0 , ~ 4 C ) , ( l S O , t ~ C ) , ( ~ O , ~ a C ) , ~ ° 4 p d ( ~ O , ~ 4 C ) , E = 7 0 MeV; m e a s u r e d ~(E(~eC)),o'(E(~3C)),a(E(14C)). °s,o9,t°°Pd d e d u c e d l e v e l , Q , m a s s e x c e s s . '°6Cd d e d u c e d m a s s e x c e s s . Q3D m a g n e t i c s p e c t r o m e t e r . PRVCA 25 331. RADIOACTIVITY 94Rh(fl+p)~94~d(fl+)'(EC)~95mPd(~+p)~96Pd(~+)'(EC)'9~Ag(~+p)~7Cd(~+p)~ Ag(~+)' ~SAg(fl+),~gCd(fl+p),9~mAg(fl+),(EC),t°aIn(fl+),(EC),'°°In(fl+p) [ f r o m 5s,~°,SaNi,63,65Cu(4°Ca,xnyp), E=4 M e V / n u c l e o n ] ; measured T~/a,Ev,lv,fl-delayed Ep,Ip,flV-,p(X-ray)-coin,E(X-ray), l ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,9~,osPd d e d u c e d l e v e l s , J , ~ r , v - b r a n e h i n g . On-line mass s e p a r a t i o n . ZPAAD 308 21. RADIOACTIVITY 94Rh(fl+p)~94~d(fl+)~(EC)~5m~d(fl+p)~9~Pd(~+)~(~C)?6Ag(~+p)~9~Cd(~+p)~97 Ag(~+)~ ~aAg(fl+),99Cd(fl+p),99mAg(fl+),(EC),~°aIn(fl+),(EC),i°°In(fl+p) ~ f r o m 56,~°,~aNi,~a,~5Cu(4°Ca,xnyp), E=4 M e V / n u c l e o n 3 ; measured T~/e,Ev,I',/,fl-delayed E p , I p , f l ~ - , p ( X - r a y ) - c o i n , E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d log f t . 95,gSRh,ga,9spd d e d u c e d l e v e l s , J , ~ T , 7 - b r a n c h i n g . 0n-line mass s e p a r a t i o n . ZPAAD 308 21.

A lOORb

=

KEYWORDS

=

100

RADIOACTIVITY 93,94,95,96,97,98,99,1°°Rb [ f r o m 235U(n,F)]; m e a s u r e d E 3 ' , i v , f l - d e l a y e d n T - , f l T - , 7V-coin; deduced fl-strength function r o l e . 9a,93,94,95,gs,97,gaSr l e v e l s d e d u c e d d e l a y e d neutron branching r a t i o s . ZPAAD 3[36 239. R A D I O A C T I V I T Y Nd,Mo,Ge; m e a s u r e d E%I~/; d e d u c e d n o e v i d e n c e f o r n e u t r i n o l e s s p r o c e s s , r i g h t h a n d e d c u r r e n t f r a c t i o n l i m i t s . ~48,15°Nd,92,1°°Mo d e d u c e d l i m i t on d o u b l e f l - d e c a y T~/ 2. 76Ge d e d u c e d l i m i t o n n e u t r i n o l e s s d o u b l e f l - d e c a y Tt/a. NCLTA 33 273. NUCLEAR REACTIONS 9a,94,gv,gSMo(t,p),E=17 MeV; m e a s u r e d or(0). 94,96,99,1°°Mo d e d u c e d levels,J, w,two-nucleon transfer s t r e n g t h s . DWBA a n a l y s i s . PRVCA 24 2475. NUCLEAR REACTIONS 51v,SS,S°,62Ni,aazn,g°,ga,94,96Zr,ga,94,96,gs,i°°Mo,12°,124Sn,14OCe(p,p,),E=200 MeV; m e a s u r e d (7(0). 51V,58,6°,82Ni,aSZn,9°,92,94,gSZr,92,949s,98,10OMo,120,124Sn,14OCe deduced resonanees,F,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 16~'~4Mg'a~Si'4~Ar'4~44~48Ca~4~4~5~Ti~54~56Fe~5~'6~4Ni'~9Y~9~Zr~'~M~ 1 4 4 S m , a ° s P b , a ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d cr(0),A(0); d e d u c e d optical model parameters. 160,24Mg,28Si,4°Ar,4°,44,48Ca,46,48,5°Ti,54,SaFe,58,6°,sa,S4Ni 89y 9OZr,98,1OOMo 144Sm, 2°8pb,2°gBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944. NUCLEAR REACTIONS l ° ° M o ( p , n T ) , E = l . 2 - 3 . 6 MeV; 9SZr(p,n-),),E=l.3 5.1 MeV; m e a s u r e d E%1% a ( E v ) , l°°Tc,gSNb d e d u c e d l e v e l s , c o n f i g u r a t i o n . P a r a b o l i c r u l e . FZKAA 13 38. NUCLEAR REACTIONS 9 9 T c ( n , 7 ) , E = 2 . 6 5 - 2 0 0 0 keV; m e a s u r e d o r ( c a p t u r e ) v s E. l°°Tc d e d u c e d resonances,resonance parameters. NSENA 81 530. NUCLEAR REACTIONS 9 9 R u ( n , F ) , E = 1 0 . 0 5 , 2 5 . 2 2 , 5 7 . 1 t , 8 1 . 6 2 , 1 9 8 . 9 eV; l ° l R u ( n , v ) , E = 1 5 . 9 , 4 2 . 2 8 , 52.13,61.81,66.82,112.5,197.3 eV; m e a s u r e d E~/,Iv. l ° ° , l ° 2 R u d e d u c e d l e v e l s , J , w . N a t u r a l Ru t a r g e t . NUPAB 385 301. NUCLEAR REACTIONS Fe,59Co,6°Ni,Sa,SSCu,89Y,gO,m,gaZr,93Nb,95Mo(lSO,xnyp),E=56,64 MeV. Fe,59Co, 6 ° N i , a 3 , 6 5 C u , a g Y , g ° , 9 1 , g a Z r , 9 3 N b , 9 5 M o ( l a C , x n y p ) , E = 4 8 MeV; m e a s u r e d ET,IV,7(t),centroid shifts. 76,7a,74,76Se,74,76,78Kr,l°°,l°a,l°4pd,l°4,1°6,1°8Cd d e d u c e d yrast cascade delay times. t°sCd d e d u c e d i s o m e r s , T 1 / a . PYLBB 113 209. NUCLEAR REACTIONS 9 6 R u ( 1 6 0 , 1 4 C ) , ( 1 6 0 , 1 3 C ) , ( 1 6 0 , l a C ) , l ° 4 p d ( 1 6 0 , 1 4 C ) , E = 7 0 MeV; m e a s u r e d a(E(laC)),cr(E(laC)),cr(E(14C)). 9a,99,1°oPd d e d u c e d l e v e l , Q , m a s s e x c e s s . 196Cd d e d u c e d mass e x c e s s . Q3D m a g n e t i c s p e c t r o m e t e r . PRVCA 25 331. R A D I O A C T I V I T Y 94Rh(fl+p)'94Pd(fl+)~(EC)'95mPd(~+p)~96Pd(~+)~(EC)~96Ag(~+p)~7Cd(~+p)'~7Ag(~+)~ 96Ag(fl+),99Cd(fl+p),99mAg(fl+),(EC),l°aIn(fl+),(EC),l°gln(fl+p) [ f r o m 58,6°,SaNi,63,65Cu(4°Ca,xnyp), E=4 M e V / n u c l e o n 3 ; measured Tl/a,ET,IT,fl-deIayed Ep,lp,flT-,p(X ray)-coin,E(X-ray), I ( X - r a y ) ; d e d u c e d log f t . 95,96Rh,96,gsPd d e d u c e d l e v e l s , J , T r , 7 - b r a n c h i n g . On-line mass s e p a r a t i o n . ZPAAD 308 21.

47

KEY

NUMBERS

A

*O~Ru

R 82K102:

/OiRh

R 82Ka15:

R 82De03:

*O~Ru

R 82Co15:

*gapd

R 82An09:

~Oaln

D 82Ku15:

D 81Mul8: 820h04:

R 82Be19: lO3Rh

D 81Mul8: 820h04:

D 82Ke05:

lO4Mo

D 82Ke05:

tO4Ru

R 82Ha13: 82St09:

lo4pd

R 82An09:

lo4Cd

D 82P105:

=

a(E,ET), 99,*°*Rh

102

=

103

R A D I O A C T I V I T Y la3Ru; m e a s u r e d - / ( 0 , t ) , o r i e n t e d n u c l e i i n Fe; d e d u c e d J,/z. l ° 3 R h l e v e l s d e d u c e d J,~. HYIND 11 127. R A D I O A C T I V I T Y t°3Ru [ f r o m l ° a R u ( n , 7 ) 3 ; m e a s u r e d Efl,Ifl,I(ce); d e d u c e d log ft,Ifl, t°3Ru,l°3Rh l e v e l s d e d u c e d J,w. J U P S A 51 43. NUCLEAR REACTIONS i°aRu(d,p),(d,d),E=45 MeV; l°4Ru(p,d),(p,p),E=29 MeV; m e a s u r e d a(O). l°3Ru deduced levels. Enriched t a r g e t s . DWBA a n a l y s i s . NUPAB 379 93. RADIOACTIVITY i°3Ru; measured 7(0,t),oriented n u c l e i i n Fe; d e d u c e d J,/z. i ° 3 R h l e v e l s d e d u c e d J,6. HYIND 11 127. R A D I O A C T I V I T Y *°3Ru [ f r o m l ° 2 R u ( n , 7 ) ] ; m e a s u r e d Efl,Ifl,I(ce); d e d u c e d log ft,Ifl, l°3Ru,l°3Rh l e v e l s d e d u c e d J,Tr. J U P S A 51 43.

A lO4Nb

101

NUCLEAR REACTIONS l°°Mo(3He,p),E=25 MeV; m e a s u r e d a(Ep,O); t°4Ru(d,a),E=20 MeV; m e a s u r e d Ea. l°2Tc d e d u c e d levels,L,Jjr. Split-pole spectrograph,enriched t a r g e t . DWBA a n a l y s i s , s h e l l m o d e l . P R V C A 25 146. NUCLEAR REACTIONS 9 9 R u ( n , 7 ) , E = 1 0 . 0 5 , 2 5 . E 2 , 5 7 . t l , 8 1 . 6 2 , 1 9 8 . 9 eV; l ° l R u ( n , 7 ) , E = 1 5 . 9 , 4 2 . 2 8 , 52.13,61.81,66.82,112.5,197.3 eV; m e a s u r e d E'/,IT. *9°,t°2Ru d e d u c e d levels,Jjr. Natural Ru t a r g e t . N U P A B 385 301. NUCLEAR REACTIONS Fe,59Co,6°Nifi3,65Cu,S9y,9°,gl,gazr,93Nb,95Mo(160,xnyp),E=56,64 MeV. Fe,59Co, ~°Ni,63,~SCu,agY,go,gl,gZzr,93Nb,95Mo(~aC,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t),centroid shifts. 7°,?2,74,76Se,74,76,78Kr,l°°,l°a,t°4pd,la4,1°6,1°8Cd d e d u c e d yrast cascade delay times. l°6Cd d e d u c e d i s o m e r s , T ~ / a . PYLBB 113 209. R A D I O A C T I V I T Y 94R~(fl+p)~4Pd(fl+)~(EC)~9~mPd(~+p)~96Pd(~+)~(EC)~96Ag(~+p)~9~Cd(~+p)~97Ag(~+)~ 98Ag(fl+),99Cd(fl+p),99mAg(fl+),(EC),i°aIn(fl+),(EC),ta°In(fl+p) [ f r o m 5 s , 6 ° , ~ Z N i f i 3 , ~ S C u ( 4 ° C a , x n y p ) , E=4 MeV/nucleon3; measured T1/~,ET,IT,fl-delayed Ep,Ip,flT-,p(X-ray)-coin,E(X-ray), I(X-ray); deduced log f t . 95,96Rh,98,98pd d e d u c e d levels,J,rr,7-branching. On-line mass separation. Z P A A D 308 21.

A la3Ru

=

KEYWORDS

NUCLEAR REACTIONS l°aMo(c~,3n),E=34-46 MeV; l°°Mo(3He,2n),E=10-18 MeV; m e a s u r e d a(ET,0),77-coin. ~°~Ru d e d u c e d l e v e l s , J j r , 8 . N U P A B 376 4 6 3 . NUCLEAR REACTIONS 9s,9aMo(~Li,3n),E=18-34 MeV; m e a s u r e d ET,IT,7(0),nT-,77-coin. deduced levels,J,Tr. Enriched t a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 26 138.

A

*OaTc

AND

=

104

R A D I O A C T I V I T Y l°4Nb [ f r o m Z3~U(n,F)3; m e a s u r e d E 7 , 1 7 , E ( X - r a y ) , I ( X - r a y ) , I ( c e ) , 7 7 - , T ( X - r a y ) - , (ce)(X-ray)-coin,fl-deeay TI/2, l°4Mo d e d u c e d l e v e l s , J , T r , 7 - b r a n e h i n g . Gas filled magnetic separator. Interacting b o s o n m o d e l . Z P A A D 306 161. R A D I O A C T I V I T Y J°4Nb [ f r o m Z35U(n,F)3; m e a s u r e d E%IT,E(X-ray),I(X-ray),I(ce),TT-,T(X-ray)-, (ce)(X-ray)-eoin,fl-decay Tl/2, t°4Mo d e d u c e d l e v e l s , J j r , 7 - b r a n c h i n g . Gas filled magnetic separator. Interacting b o s o n m o d e l . Z P A A D 306 161. NUCLEAR REACTIONS l°°Mo(TLi,2np),(TLi,nd),(TLi,t),154Sm(TLi,4np),(TLi,3nd),iTLi,Ent),E=48 MeV; m e a s u r e d ET,IT,77-,7(particle)-coin. *O4Ru,156Gd d e d u c e d l e v e l s . P R V C A 25 1699. NUCLEAR REACTIONS l ° 4 R u ( a ° a P b , a ° S p b ' ) , E = 4 . 6 M e V / n u c l e o n ; measured a(ET,07,0p),77-coin, Coulomb excitation, t°4Ru deduced levels,J,B(E2),quadrupole moment. Enriched targets. N U P A B 383 429. NUCLEAR REACTIONS Fe,59Co,6°Ni,6a,SSCu,OgY,9°,gt,92Zr,gaNb,95Mo(160,xnyp),E=56,64 MeV. Fe,59Co, 6°Ni,63,SSCu,89Y,9°,gi,gazr,93Nb,OSMo(*UC,xnyp),E=48 MeV; m e a s u r e d ET,17,7(t),centroid shifts. 7°,72,74,76Se,74,76,78Kr,t°°,l°~,l°4pd,l°4,*°6,1°8Cd d e d u c e d y r a s t c a s c a d e d e l a y t i m e s . l°6Cd d e d u c e d i s o m e r s , T 1 / a . PYLBB 113 209. R A D I O A C T I V I T Y ~o4Cd(fl+)~(EC)~1~4~n(fl+)~(EC)~i~Sn(EC)~(fl+ )~1~6Sn(~C)~(fl+ )'l~6Sb(EC)~(fl+ )~

l~S~(E~)~(~+)~j~9Te(EC)~(~+p)~(a)~(~+)~1j~Te(~+)~(EC)~(a)~1~Te(~+)~(EC)~oI(~+)~(~+p)~(~)~ ltaI(fl+),(o~),llaxe(fl+),(fl+p),(EC),(a),ll4Cs(fl+),(a),(fl+p) [ f r o m 5 6 N i ( S S N i , x n y p ) ] ; m e a s u r e d

Ea, Ep,flT-,flp-coin; deduced Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass separation,enriched t a r g e t s , s u r f a c e barrier Si,plastic scintillator,Ge(Li) detectors. N U P A B 388 91. NUCLEAR REACTIONS Fe,59Co,S°Ni,S3,S5Cu,a9Y,9°,gl,9aZr,g3Nb,95Mo(t60,xnyp),E=56,64 MeV. Fe,59Co, SONi,63,aSCu,89y,9°,gl,92Zr,g3Nb,gSMo(l~C,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t),centroid shifts. 79,72,74,76Se,74,76,78Kr,la°,l°2,1°4pd,l°4,1°6,1°sCd d e d u c e d yrast cascade delay times. l°6Cd d e d u c e d i s o m e r s , T 1 / 2 . PYLBB 113 209. fl-delayed

R 82An09:

48

KEY

NUMBERS

A

lO4cd

R 82Cr01

lO4in

D

82P105

AND

=

104

KEYWORDS

continued

NUCLEAR REACTIONS Ho,IIz,H4,1~sCd(p,t),E=42 MeV; m e a s u r e d cr(Et). ~06Cd(p,t),E=42 MeV; measured (~(Et),Q. ll°,ila,li4,iis,l°sCd d e d u c e d t w o - p a r t i c l e p i c k u p f r o m d e e p o r b i t s , l°4Cd deduced mass excess. Split-pole spectrograph,position sensitive proportional counter. P a i r i n g m o d e l . PYLBB 109 8. R A D I O A C T I V I T Y ~4Cd(fi+)~(EC)~1~4~n(fl+)~(EC)~i~Sn(EC)~(fl+)~1~Sn(EC)~(fl+)~sSb(EC)~(fl+)~

~9Sb(EC)~(~+)~9Te(EC)~(~+p)~(a)~(~+)~i~e(~+)~(EC)~(a)~2~e(~+)~(EC)'1~(~+)'(~+p)~(a)~ ~taI(fi+),(a),HaXe(fl+),(fl+p),(EC),(a),i14Cs(B+),(a),(fl+p) [ f r o m 5 S N i ( 5 8 N i , x n y p ) 3 ; m e a s u r e d Ea, B-delayed Ep,fl~/-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

A lOSAg

R 78Za13

~O5in

D 82Va21

~SSSn

D

82P105

=

Q~x,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastic scintillator,Ge(Li) detectors.

105

NUCLEAR REACTIONS i ° s p d ( p , n T ) , E = 6 . 0 5 MeV; m e a s u r e d I(ce). l°SAg l e v e l s d e d u c e d Jjr,ICC. Enriched targets,double-focusing beta-spectrometer. PIFLD 8 51. R A D I O A C T I V I T Y l°5In(fl+),l°SIn(fl+),lOTIn(fl+),(EC),~SSIn(fl+),(EC) [ f r o m Mo(14N,xn)]; m e a s u r e d - / ( 0 , T ) , o r i e n t e d n u c l e i , E T , I 7 . 105 1o6107,108in l e v e l s d e d u c e d /z,J,~r,eonfiguration. On-line separation,dilution refrigerator. PRLTA 49 1390. RADIOACTIVITY 1~Cd(fl+)~(EC)~i~4In(fl+)~(EC)~i~Sn(EC)'(fl+)~Sn(EC)'(fl+)~i~sS~(EC)'(fl+)~

~~9S b( EC )~( ~+ )~i ~9Te( EC )~( ~+ p )~( ~x)~( ~+ )'11~Te( ~+ )~( EC )'( a )~i i~T e( ~+ )~( EC )~1i~ ( ~+ )~( ~+ p )~( a )~ ~13I(fl+),(c~),liaXe(fl+),(fl+p),(EC),(a),~14Cs(fl+),(c~),(fl+p) [ f r o m 5 S N i ( a S N i , x n y p ) ] ; m e a s u r e d Ea, B-delayed Ep,flT-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

A tOSRh

D 82Ka10

loSpd

D 82Ka10

losCd

J

81Wel5

R 82An09

82Cr01

82Th01:

lOSln

D 82Va21:

lOSSn

D

82P105:

=

Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastic scintillator,Ge(Li) detectors.

106

RADIOACTIVITY l°SRh [ f r o m l°6Ru B - d e c a y 3 ; m e a s u r e d E%IT,~/-coin,T~(0),oriented nuclei. i°spd deduced levels,J,Tr,6,7-branching. JUPSA 51 23. RADIOACTIVITY i°6Rh [from 1°SRu B-decay]; measured E%l%7T-eoin,~/7(0),oriented nuclei. i°6pd deduced levels,Jflr,d,~f-branching. JUPSA 51 23. NUCLEAR MOMENTS I°6,1°s,li°,llz,li4,1~sCd; measured optical isotope shifts; deduced rms charge radii,subshell effects. Doppler-free saturation spectroscopy. ZPAAD 303 87. NUCLEAR REACTIONS Fe,59Co,6°Ni,63,SSCu,89y,9°,91,9~Zr,93Nb,95Mo(160,xnyp),E=56,64 MeV. Fe,59Co, 6 ° N i , 6 3 , a 5 C u , 8 9 Y , s ° , a ~ , S a Z r , S a N b , a S M o ( l a C , x n y p ) , E = 4 8 MeV; m e a s u r e d E%IT,~(t),centroid shifts. 7°,72,74,76Se,74,76,78Kr,l°°,l°2,1°4pd,l°4,1°6,1°sCd d e d u c e d yrast cascade delay times. l°sCd d e d u c e d i s o m e r s , T 1 / a . PYLBB 113 209. NUCLEAR REACTIONS l l ° , l 1 2 , 1 1 4 , i i s c d ( p , t ) , E = 4 2 MeV; m e a s u r e d cr(Et), l ° s C d ( p , t ) , E = 4 2 MeV; measured cr(Et),Q, ll°,l12,114,11s,l°sCd d e d u c e d t w o - p a r t i c l e p i c k u p f r o m deep o r b i t s , l°4cd deduced mass excess. Split-pole spectrograph,position sensitive proportional counter. P a i r i n g m o d e l . PYLBB 109 8. NUCLEAR REACTIONS S S R u ( l S 0 , 1 4 C ) , ( i S o , l a C ) , ( l S O , l e C ) , l o 4 p d ( l s O / 4 C ) , E = 7 0 MeV; m e a s u r e d cr(E(leC)),a(E(13C)),a(E(14C)). 98,99,1°°Pd d e d u c e d l e v e l , Q , m a s s e x c e s s , l°sCd d e d u c e d mass e x c e s s . Q3D m a g n e t i c s p e c t r o m e t e r . PRVCA 25 331. R A D I O A C T I V I T Y l°5In(fl+),l°SIn(fl+),lO~In(fl+),(EC),l°SIn(fl+),(EC) [ f r o m Mo(14N,xn)]; m e a s u r e d 3 ~ ( 0 , T ) , o r i e n t e d n u c l e i , E ' y , I T , l°5,1°s,iOT,lOSIn l e v e l s d e d u c e d /z,J,Tr,configuration. 0n-line separation,dilution refrigerator. PRLTA 49 1390. R A D I O A C T I V I T Y 1~4Cd(fl+)~(EC)~i~4~n(fl+)~(EC)~1~5Sn(EC)~(fl+)~i~Sn(EC)~(fl+)~1~S~(EC)'(fl+)'

t~9Sb( EC )'( ~+ )~i~9~e( EC )~(~+ p )~( a )'( ~+ )'~i~Te(~+ )~( EC )~( a )~ii2T e( ~+ )~( EC )~1ioI(~+ )'(~+ p )'(a )~ il3I(fl+),(a),I13Xe(fl+),(fl+p),(EC),(a),H4Cs(fl+),(a),(fl+p) [ f r o m 5 S N i ( S S N i , x n y p ) 3 ; m e a s u r e d Ea,

loSSb

D 82P105:

B-delayed Ep,fl-y-,flp-coin; deduced Qa,Q(EC),(Q(EC)-Sp),mass excess. 0n-line mass separation,enriched targets,surface barrier Si,plastic scintillator,Ge(Li) detectors. NUPAB 388 91. R A D I O A C T I V I T Y i~4Cd(fl+ )~(EC)~1~4~n(fl+ )~(EC)~1~5Sn(EC)~(fl+ )~1~Sn(EC)~(fl+ )~1~S~(EC)~(fl+)~

I°9Sb(EC),(fl+),1°STe(EC),(fl+p),(a),(fl+),11OWe(fl+),(EC),(a) llaI(fl+),(a),l13Xe(fl+),(fl+p),(EC),(a),H4Cs(fl+),(a),(fl+p) B-delayed Ep,fl'y-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

49

II2Te(fl+),(EC),lloi(fl+),(fl+p),(c~),

[from 5SNi(SSNi,xnyp)]; measured Ea, Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastic scintillator,Ge(Li) detectors.

KEY

NUMBERS

A lOTcd

D 82Gi04:

tO7in

D 81Bu23:

82VaE1

iOTSn

D 81Bu23

R 82Le07

lOSAg

D 82Ma13 R 81Mi17

lOacd

J

81We15

R 81Gu16

82An09

rOSin

D 82Va21

D 82Aw03: 82Br19:

lOgAg

D 82Aw03: 82Br19:

logCd

D 82Gi04:

82Ci07: R 82AvO7: lO9sn

D 82Jo03:

:ogSb

D 82P105:

107

=

108

NUCLEAR REACTIONS 1°8,Xl°pd(4°Ar,4°Ar'),E=120,129.1 MeV; m e a s u r e d E~/,Iv,7-yields,Coulomb excitation,7(0), l°8,1t°pd deduced levels,v-branching,B(E2),multiphonon vibrational character. Boson expansion,interacting b o s o n m o d e l . P R V C A 25 1865. R A D I O A C T I V I T Y l°SmAg; m e a s u r e d i s o m e r d i p o l e E7. NUIMA 195 621. NUCLEAR REACTIONS 1QTAg(n,-f),E n o t g i v e n ; m e a s u r e d E ' y , I % v v - c o i n . l°SAg d e d u c e d levels,J,Tr, configuration. F Z K A A 13 41. NUCLEAR MOMENTS 1°6,~°8,tl°,112,tt4,116Cd; m e a s u r e d optical isotope shifts; deduced rms charge radii,subshell effects. Doppler-free saturation spectroscopy. Z P A A D 303 87. NUCLEAR REACTIONS 7 S G e ( 9 ~ S , X ) , ( 3 2 S , F ) , E = 1 5 8 , 1 7 8 , 1 9 8 , 2 1 8 , 2 2 5 MeV; m e a s u r e d absolute a(fusion),~(evaporation),a(reaction) v s E. l°sCd d e d u c e d s y m m e t r i c fission,deep inelastic, relaxed component process separation. Tof spectrometer. F Z K A A 13 66. NUCLEAR REACTIONS Fe,59Co,6°Ni,63,SSCu,89Y,g°,gt,92Zr,93Nb,95Mo(~60,xnyp),E=56,64 MeV. Fe,~gCo, S°Ni,e3,65Cu,S9y,9°,9',9~Zr,93Nb,9~Mo(12C,xnyp),E=48 MeV; m e a s u r e d Ev,lT,v(t),centroid shifts. 7°,72,74,TSSe,74,76,78Kr,l°°,l°2,1°4pd,l°4,1°S,l°Scd d e d u c e d yrast cascade delay times. l ° s C d d e d u c e d i s o m e r s , T x / ~ . PYLBB 113 209. R A D I O A C T I V I T Y ~°SIn(fi+),~°eIn(fl+),~°~In(fl+),(EC),~SIn(fl+),(EC) [ f r o m Mo(~4N,xn)3; m e a s u r e d V(0,T),oriented n u c l e i , E v , I ' y , l°5,1°6,1°7,1°SIn l e v e l s d e d u c e d p,J,~r,configuration. On-line separation,dilution refrigerator. P R L T A 49 1390.

A logpd

=

KEYWORDS

R A D I O A C T I V I T Y 1°7,1°9Cd [ f r o m ~°7,~°gAg(p,n),E=6 MeV3; m e a s u r e d Ev,I~,I(ce). 1°7Cd d e d u c e d ICC f o r E2/M1 mixed transition,penetration parameter,effective core polarization dependent g. Z P A A D 306 57. R A D I O A C T I V I T Y l°TSn [ f r o m t°6Cd(a,3n),E=48 MeV]; m e a s u r e d Ev,l%-y3'-coin; d e d u c e d log ft. i°TIn d e d u c e d l e v e l s , J , T r . Ge(Li) d e t e c t o r s , G e ( L i ) , N a I ( T 1 ) anticoincidence spectrometer, enriched t a r g e t s . IANFA 45 2128. R A D I O A C T I V I T Y l°SIn(fl+),~°°In(fl+),l°TIn(fl+),(EC),l°SIn(fl+),(EC) [from Mo(laN,xn)3; measured V(0,T),oriented nuclei,Ev,I7. ,05 lO6,~o?,1O8in l e v e l s d e d u c e d tt,J;Tr,configuration. On-line separation,dilution refrigerator. P R L T A 49 1390. R A D I O A C T I V I T Y ~°TSn [ f r o m 1°sCd(c~,3n),E=48 MeV]; m e a s u r e d E v , I v , v ~ , - c o i n ; d e d u c e d log f t . :°7In deduced l e v e l s , J , T r . Ge(Li) d e t e c t o r s , G e ( L i ) , N a I ( T l ) anticoincidence spectrometer, enriched t a r g e t s . IANFA 4 5 2128.

A ~oepd

AND

=

109

R A D I O A C T I V I T Y l°9Pd; m e a s u r e d EV,I'y. 1°gAg d e d u c e d l e v e l s , J , ~ , v - b r a n c h i n g , ~ / - m u l t i ' p o l a r i t y , 6,1CC. I n t e r n a l conversion d a L a i n p u t . A T K O A 24 123. R A D I O A C T I V I T Y l°9pd(fl-) [ f r o m l ° s p d ( n , v ) ] ; m e a s u r e d V~/(t),flT(t). l°9Ag l e v e l d e d u c e d T1/2. Hyperpure Ge,Ge(Li),plastic scintillator d e t e c t o r s . P R V C A 26 1302. R A D I O A C T I V I T Y l°gPd; m e a s u r e d EV,Iv. 1°gAg d e d u c e d l e v e l s , J , ~ , v - b r a n c h i n g , v - m u l t i p o l a r i t y , 6,ICC. I n t e r n a l conversion d a t a i n p u t . A T K O A 24 123. R A D I O A C T I V I T Y l°gPd(fl-) [ f r o m l ° s P d ( n , v ) 3 ; m e a s u r e d v v ( t ) , f l v ( t ) . ~°~Ag l e v e l d e d u c e d T,/z. Hyperpure Ge,Ge(Li),plastic scintillator d e t e c t o r s . P R V C A 26 1302. R A D I O A C T I V I T Y i°7,1°9Cd [ f r o m t°~,l°gAg(p,n),E=6 MeV3; m e a s u r e d Ev,IT,I(ce). :°TCd d e d u c e d ICC f o r E2/M1 mixed transition,penetration parameter,effective core polarization dependent g. Z P A A D 306 57. R A D I O A C T I V I T Y l°gCd(EC) [ f r o m l ° 9 A g ( p , n ) , E = 6 MeV3; m e a s u r e d I(ce),Ev,Iv,ICC; d e d u c e d penetration parameter. NCIAA 70 15. NUCLEAR REACTIONS l°gAg(p,n~f),E=3.4,3.9 MeV; m e a s u r e d EV,Iv,DSA. l°gCd l e v e l s d e d u c e d TI/a. P R V C A 26 1310. R A D I O A C T I V I T Y t°9Sb(fl+),(EC) [ f r o m 92Mo(2°Ne,xnyp),E=190 MeV; 5SNi(SSNi,xnyp),E=290 MeV]; measured E~/,Iv,TI/a,VV-,~/(X-ray)-,Vfl-coin,Q(EC); deduced log f t . 1°9Sn d e d u c e d levels. H2Sb(fl+),(EC) [ f r o m 9 2 M o ( 2 9 N e , x n y p ) , E = 1 9 0 MeV; 5 S N i ( S S N i , x n y p ) , E = 2 9 0 M e V ] ; m e a s u r e d fl+-endpoint energies,Q(EC). Helium jet transport. J P H G B 8 1405. R A D I O A C T I V I T Y i~4~d(fl~)~(EC)~i~4In(fl+)~(EC)~5Sn(E~)~(fl+)~1~eSn(EC)~(fl~)~l~eSb(EC)~(fl+)~

~o9S~(EC)~(~+ )~1~9~e(EC)'(~+p)~(a)~(~+ ) ~ i ~ e ( ~ + )~(EC)'(c~)'ii~Te(~+ )'(EC)'~1~I(~+ )~(~+p)~(a)~ 113I(fl+),(a),H3Xe(fl+),(fl+p),(EC),(a),X14Cs(fl+),(a),(fl+p) [from 5SNi(SeNi,xnyp)3; measured Ea, fl-delayed Ep,flV-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

50

Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastie scintillator,Ge(Li) detectors.

KEY

NUMBERS

A legTe

D 82P105:

AND

=

109

A R 82Le07

li0Ag

D 80Ru03 R 81Su12

11oCd

D 80Ru03 J

81Wel5

R 82Cr01

n01n

R 82Mu01

li0Te

D 82P105

continued

R A D I O A C T I V I T Y 1~4Cd(fl~)~(EC)~4In(fl+)~(EC)~1~5Sn(EC)~(fl+)~sSn(EC)~(fl+)~i~sSb(EC)~(fl+)~ i~9Sb( EC )~(~+ )'i~9Te( EC )~( ~+ p )~( c~)~(~+ ) ' i i ~ e ( ~+ )~( EC )'( c~)'i1zTe( ~+ )~( EC )~'i~I(~+ )~(~+ p )~( a )~ uaI(fl+),(cO,iiaxe(fl+),(fl+p),(EC),(cO,n4cs(fl+),(cO,(fl+p) [ f r o m 5SNi(SSNi,xnyp)]; measured E a, fl-delayed Ep,flT-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

11opd

KEYWORDS

Q(~,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastic scintillator,Ge(Li) detectors.

110

NUCLEAR REACTIONS ios,u°pd(4°Ar,4°Ar'),E=120,129.1 MeV; measured ET,l%7-yields,Coulomb excitation,7(0). 1°e,li°Pd deduced l e v e l s , 7 - b r a n c h i n g , B ( E 2 ) , m u l t i p h o n o n v i b r a t i o n a l character. Boson expansion,interacting boson mode]. PRVCA 35 1865. RADIOACTIVITY 134Cs(fl-); ll°rnAg(/3-); measured -y-y(0),oriented nuclei, la4Ba,u°Cd !eveI deduced d(E2/MI). NUIMA 173 489. NUCLEAR REACTIONS 1°9Ag(n,7),E not given; measured ET,17,1(ce),TT-eoin. U°Ag deduced levels,configuration. FZKAA 13 39. RADIOACTIVITY 134Cs(fl-); ll°mAg(/~-); measured 77(0),oriented nuclei, la4Ba,u°Cd level deduced d(E2/MI). NUIMA 173 489. NUCLEAR MOMENTS l°S,l°S,ll°,llZ,ll4,116Cd; measured optical isotope shifts; deduced r m s charge radii,subshell effects. Doppler-free s a t u r a t i o n spectroscopy. ZPAAD 303 87. NUCLEAR REACTIONS 11°,l12,114,11sCd(p,t),E=42 MeV; measured G(Et). i°sCd(p,t),E=42 MeV; measured cr(Et),Q, u°,lla,lt4,us,i°6Cd deduced two-particle pickup f r o m deep orbits. I°4Cd deduced mass excess. Split-pole spectrograph,position sensitive proportional counter. Pairing model. PYLBB 109 8. NUCLEAR REACTIONS u°,u4,uScd(p,n),E=25 MeV; measured cr(0), n°,n4,nSln deduced IAS,J,rr. Enriched targets. Coupled-channels,DWBA analyses. NUPAB 377 163. RADIOACTIVITY '~4Cd(fl+)~(EC)~i~4In(fl+)~(EC),'~5Sn(EC)~(fl+)~1~6Sn(EC),(fl+),i~6Sb(EC),(fl+),

i ~9S~( EC )~( ~+ ) ~ 9 T e( EC )~( ~+ p )~( ~t )~( ~+ )~i'~T e(~+ )~( EC)~( a ) ~ T e(~+ )~( EC )~I1~( ~+ )~( ~+ p )~( ~ )~ it3I(fl+),(cc),naxe(fl+),(fl+p),(EC),(a),n4cs(fl+),(a),(fl+p) [from 5SNi(SSNi,xnyp)]; measured Ea,

11o I

D 82PI05

fl-delayed Ep,flT-,flp-coin; deduced Q(~,Q(EC),(Q(EC)-Sp),mass excess. On-line mass separation,enriched targets,surface barrier Si,plastic scintillator,Ge(Li) detectors. NUPAB 388 91. R A D I O A C T I V I T Y 184Cd(fl+)'(EC)~1~4In(fl+)~(EC)'i~5Sn(EC)~(fl+)~1~6Sn(EC)'(fl+)'1~sS~(EC)~(fl+)'

1~9S~(EC)~(~+)~t~9Te(EC)~(~+p)~(a)~(~+)~i1~e(~+)~(EC)~(c~)~i~Te(~+)~(EC)~i~(~+~(~+p)~(a)~ lt3I(fl+),(~),llaXe(fl+),(fl+p),(EC),(a),ll4Cs(fl+),(a),(fl+p) fl-delayed Ep,flT-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

A

nICd

R 82Kr06

UIIn

J

lllSn

R 82F102

82Nu01

82Ga17

J

81We15

R 83Cr01

HaSn

R 81Go17

111

NUCLEAR REACTIONS i l i c d ( % T ' ) , E ~, r e s o n a n c e ; m e a s u r e d ET,!%cr(E); d e d u c e d n o n r e s o n a n t process dominance,isomer excitation probability, n l C d l e v e l d e d u c e d F. P h o t o a c t i v a t i o n , S°Co s o u r c e . PRVCA 25 2{397. NUCLEAR MOMENTS l i l I n ; m e a s u r e d NMR; d e d u c e d Knight shift i n Cu,g. B r u t e force orientation,implantation in Cu,electromagnetic separator. PRLTA 49 347. NUCLEAR REACTIONS u z , n 4 , u 5 , i l s , u T , u s , u ° , l a ° , l a 2 , 1 Z 4 S n ( p , d ) , E = 2 0 MeV; m e a s u r e d cT(Ep),cr(0). 112,114,116,118,12°,122,1~4Sn d e d u c e d occupation probabilities, n i 113 114 115 116 117 118 119 121 le3Sn d e d u c e d l e v e l s , J j r , S . F i n i t e - r a n g e DWBA a n a l y s i s . C J P H A 60 438. NUCLEAR REACTIONS n a S n ( p o l a r i z e d d , t ) , E = 4 0 MeV; m e a s u r e d cr(Et),cr(0),A(0); d e d u c e d valence,inner-hole components, i n s n d e d u c e d levels,L,J,Tr,CZS. E n r i c h e d target,polarized beam,magnetic spectrometer. DWBA a n a l y s i s . NUPAB 381 40.

A lizCd

=

[from 5SNi(5SNi,xnyp)]; measured E~, Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastie scintillator,Ge(Li) detectors.

=

113

NUCLEAR MOMENTS 1°6,1°s,ll°,ila,il4,11aCd; measured optical isotope shifts; deduced r m s charge radii,subshell effects. Doppler-free s a t u r a t i o n spectroscopy. ZPAAD 303 87. NUCLEAR REACTIONS u°,lle,li4,11sCd(p,t),E=42 MeV; measured •(Et). i°6Cd(p,t),E=42 MeV; measured cr(Et),Q, t1°,na,n4,us,1°sCd deduced two particle pickup f r o m deep orbits, i°4Cd deduced mass excess. Split-pole spectrograph,position sensitive proportional counter. Pairing model. PYLBB 109 8. NUCLEAR REACTIONS ii°Cd(a,2n),E=27 MeV; measured T(0,H,t). UaSn level deduced g, configuration. IANFA 45 2116.

51

KEY

NUMBERS

A

li2Sn

R 82F102:

11aSb

R 82Ma29:

UaTe

D 82P105:

AND

=

112

KEYWORDS

continued

NUCLEAR REACTIONS 112,114,115,116,117,118,119,120,122,124 Sn (p,d), E-a0- MeV; m e a s u r e d a(Ep),~(0). ll~ 114 116 118 130 122 124Sn d e d u c e d occupation probabilities. 111 113 114 115 116 117 110 119 121 123Sn d e d u c e d l e v e l s , J J r , S . F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS l°3Rh(12C,3n),E=50 MeV; m e a s u r e d Iv(O,t,H). naSb d e d u c e d i s o m e r level quadrupole moment. Pulsed beam,recoil implantation in Sb,Sn single crystal, polycrystalline I n f o i l . PRVCA 26 493. RADIOACTIVITY 1•4Cd(fl+)•(EC)•1•4•n(fl+)•(EC)•••5Sn(EC)•(fl+)•1•6Sn(EC)•(fl+)••••Sb(EC)•(fl+)•

1 ~ S b ( EC )~( ~+ ) ~ 1 ~ e( EC )~( ~+ p )~( a )~( ~+ )~1~T ~( ~+ )~( EC )~( ~ )'1~2~e( ~+ )~( EC )~ ~ I ( ~+ )~( ~+ p )~( a )~ 11al(fl+),(a),n3xe(fl+),(fl+p),(EC),(a),l14Cs(fl+),(a),(fl+p) [ f r o m 58Ni(SSNi,xnyp),l; m e a s u r e d E(x, fl-delayed Ep,flV-,flp-coin; deduced separation,enriched targets,surface NUPAB 388 91.

A ll3Ag

D 82Br10:

ll3cd

D 82Br10:

l131n

D 811102:

U3Sn

D 81Go17: 81Se15:

R 82F102:

1131

D 82P105:

=

Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier Si,plastie scintillator,Ge(Li) detectors.

113

RADIOACTIVITY 113m,l14,115rn,llb,l16m,l16,117m,llV,llSAg [ f r o m U(n,F),E=14 MeV,a49Cf(n,F), E = t h e r m a l , C d ( n , p ) , E = 1 4 MeV'I; m e a s u r e d E v , I T , v - y - , f l V - , T ( X - r a y ) - c o i n . ll3m,llbm,ll6m,ll7,11~'mAg deduced T1/a,Qfl,Ifl,log f t . USAg d e d u c e d average T I / 2 . 113,nb,n6Cd d e d u c e d levels, v-branching. F a s t c h e m i c a l s e p a r a t i o n . RAACA 30 1. RADIOACTIVITY 113m,l14,i15rn,llb,l16m,II6,117m,llV,llSAg [ f r o m U(n,F),E=14 MeV,249Cf(n,F), E = t h e r m a l , C d ( n , p ) , E = 1 4 MeV,l; m e a s u r e d E v , I v , v V - , f l V - , v ( X - r a y ) - c o i n . 113m,l15m,llSrn,l17,117mAg deduced T1/2,Qfl,Ifl,log f t . 116Ag d e d u c e d average T I / 2 . 113,ns,l16Cd d e d u c e d levels, " y - b r a n c h i n g . F a s t c h e m i c a l s e p a r a t i o n . RAACA 30 1. RADIOACTIVITY u 3 m I n [ f r o m U3Sn d e c a y ] ; m e a s u r e d d o u b l e e l e c t r o n s u m s p e c t r a ; d e d u c e d decay mechanisms. FZKAA 13 331. RADIOACTIVITY U3Sn [ f r o m m C d ( a , 2 n ) , E = 2 7 MeV,l; m e a s u r e d V(0,H,t). 113Sn level d e d u c e d g, configuration. IANFA 45 2116. RADIOACTIVITY 69Ge [ f r o m 56Fe(160,n2p),E=56 MeV]; n 3 s n [ f r o m 16°Mo(160,3n),E=56 MeV,l; measured 7(0,H,T); d e d u c e d q u a d r u p o l e interaction constants f o r Ge i n T1,Sn i n Sn. Recoil i m p l a n t a t i o n . ZPBBD 45 29. NUCLEAR REACTIONS lla,l14,11s,lls,llv,lls,ug,la0,la2,124Sn(p,d),E-20_ MeV; m e a s u r e d a(Ep),~(0). 112,114,116,118,12°,122,124Sn deduced occupation probabilities. 111,113,114,115,116,117,116,119121 123Sn d e d u c e d l e v e l s , J j v , S . F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. RADIOACTIVITY l ° 4 C d ( f l + ),(EC), 104 I n ( f l + ),(EC), 105 S n ( E C ) , ( f l + ), 106 S n ( E C ) , ( f l + ), 106 S b ( E C ) , ( f l + ),

18~Sb(EC)~(~+)'1~9~e(EC)~(~+p)~((x)'(~+)~1i8Te(~+)'(~C)'(a)~1~Te(~+)~(EC)'118I(~+)~(~+p)'((x)'

ll3Xe

D 83P105:

113I(fl + ) , ( a ) , 113 Xe(fl + ),(fl + p ) , ( E C ) , ( a ) , 114 Cs(fl + ),(a),(fl + p) [ f r o m 58Ni(SSNi,xnyp)]; measured Ecx, fl-delayed Ep,flV-,flp-coin; deduced Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass separation,enriched targets,surface barrier Si,plastic seintillator,Ge(Li) detectors. NUPAB 388 91. RADIOACTIVITY 184Cd(fl+ )•(EC)•i84In(fi+)•(EC)•i•5Sn(EC)•(fl+)•1••Sn(EC)•(fl+ )•18sS•(EC)'(fl+ )• 100 S D ( E C ) , ( f l + ), 109 We(EC),(fl + p ) , ( ~ ) , ( f l + ), 110 Te(fl + ) , ( E C ) , ( ~ ) , 112 We(fl + ) , ( E C ) , l 1 8 I ( f l + ) , ( f l + p ) , ( a ) , 113 I(fl + ) , ( a ) , 113Xe(fl + ),(fl + p ) , ( E C ) , ( a ) , 114 Cs(fl + ),(¢x),(fl +p) [ f r o m 58Ni(58Ni,xnyp),l; m e a s u r e d Ea, Ê-delayed Ep,fl-/-,flp-coin; deduced Q(~,Q(EC),(Q(EC)-Sp),mass excess. On-line mass separation,enriched targets,surface barrier Si,plastic scintillator,Ge(Li) detectors. NUPAB 388 91.

A li4Ag

D 82Br10:

ll4cd

J

81Welb:

R 82Cr01:

82Hu08: 82Sc09:

=

114

RADIOACTIVITY l13m,l14,115m,llS,l16rn,l16,117m,l17,118Ag [ f r o m U(n,F),E=I4 MeV,a49Cf(n,F), E=thermal,Cd(n,p),E=I4 MeV,l; m e a s u r e d E%I%vv-,flT-,7(X-ray)-coin. 113rn,115m,l16m,117,117mAg deduced T1/a,Qfl,lp,log ft. llSAg d e d u c e d average TI/2. I13,115,116Cd d e d u c e d levels, v - b r a n c h i n g . Fast chemical separation. R A A C A 30 I. NUCLEAR MOMENTS 1°6,1°s,11°,ila,l14,116Cd;m e a s u r e d optical isotope shifts; d e d u c e d r m s charge radii,subshell effects. Doppler-free saturation spectroscopy. Z P A A D 303 87. NUCLEAR R E A C T I O N S u°,na,11%ilsCd(p,t),E=42 MeV; m e a s u r e d ~(Et). 1°sCd(p,t),E=42 MeV; m e a s u r e d ~(Et),Q. 11°,I12,114,116,I°6Cdd e d u c e d two-particle p i c k u p f r o m deep orbits. I°4Cd d e d u c e d m a s s excess. Split-pole spectrograph,position sensitive proportional counter. Pairing model. P Y L B B 109 8. NUCLEAR REACTIONS n3Cd(n,v),E=thermal; m e a s u r e d E'y,Iv,TV(0),oriented nuclei, n 4 C d d e d u c e d levels,7-branching,J,Tr,~,B(E0)/B(E2). J P H G B 8 1107. NUCLEAR REACTIONS n a C d ( n , - y ) , ( n , e - ) , E = t h e r m a l ; uaCd(n,-Y),E=2,24 keV; m e a s u r e d ET,I7, l(ce). 114Cd d e d u c e d l e v e l s , T - b r a n c h i n g ratio,J,~r,T1/a,B(E0),B(E2). T w o - p a r t i c l e , t w o - h o l e core c o u p l i n g c a l c u l a t i o n s . PYLBB 110 364.

52

KEY

NUMBERS

A

114In

D 83Nu02: R 82Mu01:

l~4Sn

R 82F102:

u4Sb

R

82Dull

83Va07

I~4Cs

D 83P105

=

114

deduced

occupation

82Br10

115Cd

D

83Br10

115in

D

82Gr17

J

82Ji01

R 78Av08 HSSn

R 82FI02

82La12

D

82A129

82Br10

~i6Cd

D 82Br10

J

81We15

111 ,13 114 115 t16 117 118 119 121

RADIOACTIVITY 164Cd(ft+)~(E~)~i94~n(ft+)~(EC)~1~5Sn(EC)~(ft+)~'6~Sn(EC)~(ft+)~1~Sb(E~)~(ft+)~ 199Sb(EC),(ft+),l°gTe(EC),(ft+p),(a),(fi + ), 119 T e ( f l + ) , ( E C ) , ( a ) , 112 T e ( f l + ) , ( E C ) , 119 I(fl + ) , ( f t + p ) , ( a ) , 113I(fl +) , ( a ) , 113Xe(fl +),(ft +p ) , ( E C ) , ( a ) , 114Cs(fl +),(a),(ft +p) [ f r o m 58Ni(5SNi,xnyp)]; measured Ea,

=

Qa,Q(EC),(Q(EC)-Sp),mass excess. On-line mass barrier St,plastic scintillator,Ge(Li) detectors.

115

R A D I O A C T I V I T Y 113m,l14,115rn,l15,116m,l16,11?m,ilT,llSAg [ f r o m U(n,F),E=t4 MeV,a49Cf(n,F), E=thermal,Cd(n,p),E=14 MeV]; m e a s u r e d E%I-/,77-,ftV-,-/(X-ray)-coin. U3m,llSm,U6m,nT,nTmAg deduced T1/~,Qft,Ift,log f t . 118Ag d e d u c e d a v e r a g e TI/2. li3,115,H6Cd d e d u c e d levels, 7-branching. Fast chemical separation. R A A C A 30 1. R A D I O A C T I V I T Y 113m 1 1 4 , 1 1 5 m , n s , u 6 m , l 1 6 , U T m , n T , l l S A g [ f r o m U(n,F),E=I4 MeV,249Cf(n,F), E=thermal,Cd(n,p),E=14 MeV]; m e a s u r e d ET,I-y,'/7-,ftV-,7(X-ray)-coin. n3m,nsm,n6m,n?,n?mAg deduced Tl/2,Qfl,Ifl,log f t . 118Ag d e d u c e d average T1/2. 119,115,116Cd d e d u c e d levels, -/-branching. Fast chemical separation. R A A C A 30 1. RADIOACTIVITY n61n(ft-) [from U 5 I n ( p o l a r i z e d n,-/)]; m e a s u r e d Ifl(0,T,t). n6,115In d e d u c e d quadrupole moment r a t i o . N u c l e a r s p i n r e l a x a t i o n t e c h n i q u e , I n P s i n g l e c r y s t a l . NUPAB 386 56. NUCLEAR MOMENTS n5In; m e a s u r e d hfs; d e d u c e d electric q u a d r u p o l e m o m e n t , d i p o l e , q u a d r u p o l e interaction constants. High resolution laser spectroscopy. Z P A A D 306 7. NUCLEAR REACTIONS 1 1 5 I n ( n , n ' v ) , E = f a s t ; measured E T , I v . 115In d e d u c e d levels,Jflr, T-branching. Ge(Li) d e t e c t o r , n a t u r a l t a r g e t s . PIFLD 8 18. NUCLEAR REACTIONS n a , l 1 4 , 1 1 5 , n e , n T , n s , l l g , 1 2 9 , 1 2 z , l e 4 S n ( p , d ) , E = 2 0 MeV; m e a s u r e d a(Ep),G(0). 112,114,116,118,12°,1~2,124Sn d e d u c e d occupation probabilities. 111,113,114 i15116,117,118,119121, 12aSn d e d u c e d l e v e l s , J , r r , S . F i n i t e - r a n g e DWBA a n a l y s i s . C J P H A 60 428. NUCLEAR REACTIONS U%n,a6spb(3He,~),E=283 MeV; m e a s u r e d (r(Ea),a(0). n S s n l e v e l s d e d u c e d CZS,lgg/2,1f5/2,1fT/2 n e u t r o n hole strength fragmentation. 2°TPb d e d u c e d n o gg/a s t r e n g t h concentration. DWBA a n a l y s i s . PYLBB 114 103.

A

116Ag

probabilities.

117 30. NUCLEAR REACTIONS n l , n 3 C d ( T L i , 4 n ) , E = 3 2 - 5 0 MeV; m e a s u r e d ET,I%7(t),a(Ev),7-/-coin,v(O). 116,114Sb d e d u c e d levels,Ti/2,J,Tr,~-branching,~/-multipolarity,6. C o r e - p a r t i c l e coupling, quasiparticle configuration m i x i n g . Z P A A D 307 a59. NUCLEAR REACTIONS n a , U S I n ( a , 3 n v ) , E = 3 6 - 4 8 MeV; n T S n ( p , 2 n - / ) , E = 1 5 - 2 5 MeV; m e a s u r e d E7,I7, ~/T-coin,IT(0,t),l(ce). 114,i16Sb d e d u c e d levels,J,Tr,T-branching,~,Tl/a,ICC. Enriched targets,Ge(Li),Si-Li detectors,mini-orange electron spectrometer. NUPAB 379 35.

A D

continued

123Sn d e d u c e d levels,Jflr,S. F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS a98pb,n6sn(afiHe),E=318 MeV; m e a s u r e d a(E(6He))a(0); d e d u c e d r e a c t i o n m e c h a n i s m . U4Sn,266pb d e d u c e d l e v e l s , J j r , L , c o n f i g u r a t i o n .Z e r o - r a n g e DWBA a n a l y s i s . PYLBB

d-delayed Ep,flT-,ftp-eoin; deduced separation,enriched targets,surface N U P A B 388 91.

115Ag

KEYWORDS

R A D I O A C T I V I T Y n 4 I n [ f r o m Ualn n e u t r o n i r r a d i a t i o n ] ; m e a s u r e d NMR,oriented n u c l e i i n Fe, d- anisott'opy; deduced #,configuration. Recoil implantation. P R V C A 26 1701. NUCLEAR REACTIONS 116,u4,116Cd(p,n),E=25 MeV; m e a s u r e d ~(0). n e , n 4 , n 6 I n d e d u c e d IAS,J,rr. Enriched targets. Coupled-channels,DWBA a n a l y s e s . N U P A B 377 163. NUCLEAR REACTIONS n a , l 1 4 , i 1 5 , u 6 , n T , n s , u g , l a ° , l a a , l a 4 S n ( p , d ) , E = 3 0 MeV; m e a s u r e d (r(Ep),cr(0). l12,114,116,118,1a6,122,124Sn

82Ge06:

AND

=

116

R A D I O A C T I V I T Y li6,1iT,lis,llg,Iao,i21Ag [ f r o m fission product mass separation]; 119,121Cd [from ngJZlAg(fl-) decay]; measured fiT-coin; deduced Qft,maximurn Ef,mass excess. Fission product mass separation,Ge(Li),Si-Li d e t e c t o r s . P R V C A 36 1157. RADIOACTIVITY 11am,n4,115m,n5,n6m,i16,117m,llT,tlSAg [from U(n,F),E=14 MeV,249Cf(n,F), E=thermal,Cd(n,p),E=14 MeV]; m e a s u r e d ET,IT,TT-,ftT-,7(X-ray)-coin. n3mJiSm,n6m,nT,nTmAg deduced T1/a,Qft,Ift,log f t . 11SAg d e d u c e d average T 1 / s . t13,ils,l16Cd d e d u c e d levels, 7-branching. Fast chemical separation. R A A C A 30 l. R A D I O A C T I V I T Y 113m 114 l15m 115 ll6m 116 llTm,l17,118Ag [ f r o m U(n,F),E=14 MeY,a49Cf(n,F), E=thermal,Cd(n,p),E=14 MeV]; m e a s u r e d E%IT,-/7-,ftT-,7(X-ray)-coin. ll3m,li5m,ll6m,llT,117rnAg deduced Tl/2,Qft,Ift,log f t . t l S A g d e d u c e d a v e r a g e T l / 2 . tia lls,116Cd d e d u c e d levels, -y-branching. Fast chemical separation. R A A C A 30 1. NUCLEAR MOMENTS to6,168,11°,l12,114,116Cd; m e a s u r e d optical isotope shifts; deduced rms charge radii,subshell effects. Doppler-free saturation spectroscopy. Z P A A D 303 87.

53

KEY

NUMBERS

A "sCd

R 82Cr01

llSin

D 81St29 82Grll

8~Grl7:

R

,ISSn

8gMu01:

R 81AIZ7:

82F10~:

'i6Sb

R 82Dull:

8eVa07:

,,6Te

R 82Ch01:

D 82A129:

82Br10:

*lVin

D 82Fu07:

"TSn

R 82F102:

1171

R 82Ga21

=

=

D 82A129

82Br10

liSSn

D 82Ka09

R 81A128

continued

117

RADIOACTIVITY " s , u v , ' l s , l l g , i z ° , ' Z l A g [ f r o m fission product mass separation]; il9,1ZlCd [ f r o m llg,'2'Ag(ft-) d e c a y ] ; m e a s u r e d f l V - c o i n ; d e d u c e d Q f t , m a x i m u m Eft,mass excess. F i s s i o n p r o d u c t m a s s s e p a r a t i o n , G e ( L i ) , S i - L i d e t e c t o r s . PRVCA 26 1157. RADIOACTIVITY ,13m ,14 1,sin , , s , , , S m 1,6,1,7m,l17,,lSAg [ f r o m U(n,F),E=14 MeV,e49Cf(n,F), E = t h e r m a l , C d ( n , p ) , E = 1 4 MeV]; m e a s u r e d E 7 , I v , 7 7 - , f 1 7 - , v ( X r a y ) - c o i n . ,,3m,l*Sm nSm tlv,,,vmAg deduced T,/2,Qft,Ift,log f t . ' l S A g d e d u c e d a v e r a g e T , / 2 . l ' 3 , " 5 , 1 ' 6 C d d e d u c e d l e v e l s , v-branching. F a s t c h e m i c a l s e p a r a t i o n . RAACA 30 1. RADIOACTIVITY l i v m , i l V I n [from l'vCd(fl-decay)]; measured EV,Iv,T1/2. T w o - s t e p s o u r c e preparation,thermal neutron capture,deuteron s t r i p p i n g o n ' t s C d t a r g e t . RAACA 30 61. NUCLEAR REACTIONS t,2 . 114. l l .s , i .s n7 . .,,8 . , , 9. , 2 0. , 2 2 t24 S n ( p , d ) , E = 2 0 MeV; m e a s u r e d cr(Ep),cr(0). 1,2 , i,4 , , i s , ,,8 ~ ,as , 122 , ,24Sn d e d u c e d occupation probabilities. 11, , ,,3 , lid , ,15 , 1,6 , 1,7 , ,,8 , ,,9 , ,2, , 123Sn d e d u c e d l e v e l s , J , v r , S . F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS n d , H 6 , n S S n ( S L i , 3 n ) , E = 3 3 MeV; m e a s u r e d Ev,Iv,a(Ev),7(0),77-coin,v(t), 7 ( 0 , H , t ) . 117,119,*a'I d e d u c e d levels,J,~r,isomer T,/a,~(E2/M1),v-branching ratio. '2'I d e d u c e d i s o m e r g. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . PRVCA 26 1101.

A llSAg

116

KEYWORDS

NUCLEAR REACTIONS i , o , * l a , t , a , t l s C d ( p , t ) , E = 4 2 MeV; m e a s u r e d a(Et). '9sCd(p,t),E=42 MeV; m e a s u r e d g(Et),Q, n ° , n z , n d , u s , l ° s C d d e d u c e d t w o - p a r t i c l e p i c k u p f r o m d e e p o r b i t s , l°dCd deduced mass excess. Split-pole spectrograph,position sensitive proportional counter. P a i r i n g m o d e l . PYLBB 109 8. RADIOACTIVITY n S m l n [ f r o m nSIn(n,v),E=thermal]; measured TI/2. AENGA 51 61. RADIOACTIVITY nSIn [ f r o m In(polarized n , v ) , E = t h e r m a l ] ; m e a s u r e d N M R , f l - a s y m m e t r y ; deduced defect induced electric field gradients,relaxation rates. Polarized source,undoped InP, I n S b , I n S b : T e s i n g l e c r y s t a l . ZPBBD 47 1. RADIOACTIVITY l l S I n ( f t - ) [ f r o m n a l n ( p o l a r i z e d n , 7 ) ] ; m e a s u r e d Ift(0,T,t). n s , U S I n d e d u c e d q u a d r u p o l e m o m e n t r a t i o . N u c l e a r s p i n r e l a x a t i o n t e c h n i q u e , I n P s i n g l e c r y s t a l . NUPAB 386 56. NUCLEAR REACTIONS n o , t ~ , i ' s C d ( p , n ) , E = 2 5 MeV; m e a s u r e d a(0). n o , u d , n S I n d e d u c e d IAS,J,~r. Enriched targets. Coupled-channels,DWBA a n a l y s e s . NUPAB 377 163. NUCLEAR REACTIONS HSSn,SSNi((x,(~),((~,c~'),E=480 MeV; ZosPb(c~,(x),((~,(~'),E=340,480 MeV; m e a s u r e d (7(0); d e d u c e d or(total), a ° s p b , n % n d e d u c e d g i a n t r e s o n a n c e e x c i t a t i o n . FZKAA 13 83. NUCLEAR REACTIONS H u , ' 1 4 , i l s , ' l s , ' l ~ , ' t s , " 9 , ' z o , ' ~ z , ' ~ d S n ( p , d ) , E = 2 0 MeV; m e a s u r e d cr(Ep),cr(0). Hz,,14,1,6,,,8,1zo,izz,,~Sn deduced occupation probabilities. , , , , ,,3 , ,,4 , ll5 , ll~ , 1,7 , 1,~ , ,,9 , ,ai , *~3Sn d e d u c e d levels,J,vr,S. F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS H l , ' 1 3 C d ( 7 L i , 4 n ) , E = 3 2 - 5 0 MeV; m e a s u r e d E v , I 7 , 7 ( t ) , ~ ( E T ) , 7 7 - c o i n , 7 ( 0 ). llS,l'dSb d e d u c e d levels,T,/a,J,rr,v-branching,v-multipolarity,6. Core-particle coupling, quasiparticle configuration m i x i n g . ZPAAD 307 259. NUCLEAR REACTIONS n d , n S I n ( a , 3 n v ) , E = 3 6 - 4 8 MeV; n V S n ( p , 2 n v ) , E = 1 5 - 2 5 MeV; m e a s u r e d E%I% 77 coin,I7(0,t),I(ce), t14,~lsSb d e d u c e d levels,J,vr,v-branching,6,T1/z,ICC. Enriched targets,Ge(Li),Si-Li detectors,mini-orange electron spectrometer. NUPAB 379 35. NUCLEAR REACTIONS nVSn(a,n),E=16,18,~0 MeV; n g S n ( a , n ) , E = 1 8 MeV; n d S n ( a , 2 n ) , E = ~ 2 , ~ 4 MeV; ~ ' S S n ( a , 2 n ) , E = ~ 2 MeV; ' ° s P d ( ' u C , 2 n ) , E = 5 8 MeV; ' 1 0 P d ( ' a C , 3 n ) , E = 4 0 , 4 5 , 4 9 , 5 ~ MeV; l ' ° C d ( ' d C , 3 n ) , E=5R MeV; m e a s u r e d 77-coin,7(0),a(E7). Hs,l~s,~2°,'aZTe,'a°Xe d e d u c e d levels,J,~r. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . PRVCA 35 813.

A llVAg

AND

118

RADIOACTIVITY llS,llV,llS,llg,12°,lZlAg [from fission product mass separation]; llg,l~lcd [ f r o m i19,121Ag(ft-) d e c a y ] ; m e a s u r e d f t V - c o i n ; d e d u c e d Q f t , m a x i m u m Eft,mass excess. F i s s i o n p r o d u c t m a s s s e p a r a t i o n , G e ( L i ) , S i - L i d e t e c t o r s . PRVCA 26 1157. RADIOACTIVITY lldm,iJ4 ll5m 115 ,16m,l,S,llVm,l17,118Ag [ f r o m U ( n , F ) , E = 1 4 MeV,Z49Cf(n,F), E = t h e r m a l , C d ( n , p ) , E = 1 4 MeV]; m e a s u r e d E v , I v , T T - , f t V - , v ( X - r a y ) - c o i n . l l 3 m , l l 5 m , l l S m , l l V , l l V m A g deduced Tl/2,Qft,Ift,log f t . llSAg d e d u c e d a v e r a g e TI/2. 1 1 3 , 1 1 5 , 1 1 6 C d deduced levels, v-branching. F a s t c h e m i c a l s e p a r a t i o n . RAACA 30 1. RADIOACTIVITY n S S b [ f r o m l z I S b ( p , d n ) i l S T e ( E C - d e c a y ) ] ; m e a s u r e d I(ce),EV,I%77(O). USSn deduced levels,J,~r,B(E0)/B(E2),relative monopole strength,v-branching. Natural target,~r square-root two iron free magnetic ft-ray spectrometer. PRVCA 25 2013. NUCLEAR REACTIONS 117Sn(polarized n,X),E ~ 0.75-2.3 eV; m e a s u r e d t r a n s m i s s i o n , d i f f e r e n c e in a(ratio) f o r o p p o s i t e h e l i c i t i e s . 11SSn d e d u c e d space parity nonconservation for p-wave r e s o n a n c e . Tof. PZETA 34 308.

54

KEY

NUMBERS

A llBSn

R 82Be18: 82Be35: 82FI02:

tiaSb

D 82Ka09:

HaTe

R 82Ch01

82Va10

D

tlCd

D 82A129

119Sn

R 82Di04

82A129

82FI02

820k01

ll Sb

D 83Sa22

iIgTe

D 82Sa22

1191

R 82Da17 82G221

tlaXe

R

82B231:

D 82A129:

l~OSn

R 8~Be18: 82Di04:

82Dj04:

continued

=

t19

RADIOACTIVITY i16,i17,118,I19,12°,121Ag [ f r o m fission product mass separation]; Iig,121Cd [ f r o m l/9,121Ag(ft-) d e c a y ] ; m e a s u r e d f i T - c o i n ; d e d u c e d Q f t , m a x i m u m Eft,mass excess. Fission product mass separation,Oe(Li),Si-Li d e t e c t o r s . PRVCA 26 1157. R A D I O A C T I V I T Y II6,1IT,IIS,IIg,lzO,12IAg [from fission product mass separation]; Itg,121Cd E f r o m II9,121Ag(ft-) d e c a y 3 ; m e a s u r e d f t T - c e i n ; d e d u c e d Q f t , m a x i m u m Eft,mass excess. Fission product mass separation,Ge(Li),Si-Li d e t e c t o r s . PRVCA 26 1157. NUCLEAR REACTIONS iZ°Sn(p,d),E=26.3 MeV; m e a s u r e d atE(d),0), n g s n d e d u c e d l e v e l s L,J,Tr,S. t2°Sn deduced occupation probabilities,quasiparticle energies. Magnetic spectrograph, enriched t a r g e t . DWBA a n a l y s i s . NUPAB 377 137. NUCLEAR REACTIONS 112,t t 4 , it5 , It0 ,117,11a, 119, leo, lea , t 2 4 S n ( p , d ) , E-20- MeV; m e a s u r e d a ( E p ) , a (0). llz,114,116,1ts,leo,taa,lZ4Sn d e d u c e d occupation probabilities, i l l ~la t~4 i t 5 lt6 l i t Jlo t19 let laaSn deduced levels,J,~,S. Finite-range DWBA a n a l y s i s . C J P H A 60 428. NUCLEAR REACTIONS n a S n ( a , a ' n ) , E = 1 0 9 MeV; m e a s u r e d a(Ea,Oa),a(Ea,Oa,On),an-coin,an(O), ~ ( 0 a , E a , 0 n , E n ) ; d e d u c e d r e a c t i o n m e c h a n i s m , nSn d e d u c e d GQR d e c a y m e c h a n i s m . PRLTA 48 1382. R A D I O A C T I V I T Y H mTe(EC) [from S b ( p , 3 n ) , E = 3 0 Me V ]; m e a s u r e d I(ce),ceT(O),TT(e). u°Sb transitions deduced subshell ICC r a t i o s , 6 , T - b r a n c h i n g . J U P S A 51 2 4 0 0 . R A D I O A C T I V I T Y n mTe(EC) [from S b ( p , 3 n ) , E = 3 0 MeV]; m e a s u r e d I(ce),ceT(O),TT(O). u Sb transitions deduced subshelt ICC r a t i o s , 6 , T - b r a n c h i n g . J U P S A 51 2 4 0 0 . NUCLEAR REACTIONS 1° Ag(13C,3n),E=52 MeV; l S t T a ( i ° 0 , 5 n ) , E = 1 0 0 MeV; m e a s u r e d IT(0,t). nI l e v e l d e d u c e d g,T1/2. 192T1 l e v e l d e d u c e d g , q u a d r u p o l e moment,Tl/2, NUPAB 383 421. NUCLEAR REACTIONS H 4 , 1 1 o , l i e S n ( ° L i , 3 n ) , E = 3 3 MeV; m e a s u r e d ET,IT,a(ET),T(0),TT-coin,T(t), 7(0,H,t). 117 It9 l a l I d e d u c e d levels,J,~r,isomer Tt/a,8(Ea/M1),T-branching ratio. 1211 d e d u c e d i s o m e r g. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . PRVCA 26 1101. NUCLEAR REACTIONS l l ° , n a C d ( t 2 C , 3 n ) , E = 5 3 - 7 5 MeV; m e a s u r e d a(E,E%O),TT-coin,TT(t), u ,lmXe deduced levels,J,Tr,T~/2. Enriched targets,Ge(Li) detectors. Interacting boson fermion m o d e l . NUPAB 383 309.

=

120

R A D I O A C T I V I T Y 116,117,118,119,12°,121Ag [ f r o m fission product mass separation]; ug,lalCd [from ug,lalAg(fl-) decay]; measured fiT-coin; deduced Qfl,maximum Eft,mass excess. Fission product mass separation,Ge(Li),Si-Li d e t e c t o r s . PRVCA 26 1157. NUCLEAR REACTIONS 9 ° Z r ( 7 , 7 ' ) , E = 8 4 9 6 k e V ; 1 1 8 8 n ( 7 , 7 ' ) , E = 6 3 2 5 , 6 9 8 8 k e V ; 1 2 ° S n ( 7 , T ' ) , E = 6 7 3 0 keV; measured ET,IT,77(0),cr. ° ° Z r , l l s , l a ° S n t r a n s i t i o n s d e d u c e d FT,TI/2. IA N FA 4 6 57. NUCLEAR REACTIONS l e ° S n ( p , d ) , E = 3 6 . 3 MeV; m e a s u r e d a t E(d),0). USn d e d u c e d l e v e l s L,J,Tr,S. iZOSn d e d u c e d occupation probabilities,quasiparticle energies. Magnetic spectrograph, enriched t a r g e t . DWBA a n a l y s i s . NUPAB 377 137. NUCLEAR REACTIONS 51V , 5o ,6o , eaNi , SOZn ,90 ,92 ,94 ,96Zr ,92 ,94 ,96 ,98 , lOOMo ,12o,124Sn ,14°Ce(p , p') , E-200MeV; m e a s u r e d a(O). 51V, 58 ,6o ,62 Nl,- 66 Zn .90. .92. 94 96 Zr .92. .94. 96 . 98 lO0 Mo, 12o ,124 Sn, 14o Ce deduced resonances,F,T,Ml

82F10~:

118

~23Sn d e d u c e d l e v e l s , J , T r , S . F i n i t e - r a n g e DWBA a n a l y s i s . C J P H A 60 428. RADIOACTIVITY tlSsb [from t2tSb(p,4n)tlSTe(EC-deeay)]; measured I ( c e ) , E ~ , I T , T T ( 0 ) . iJSSn deduced levels,J,rr,B(E0)/B(E2),relative monopole strength,T-branching. Natural target,Tr square-root two iron free magnetic ft-ray spectrometer. PRVCA 25 2013. NUCLEAR REACTIONS nTS n(a ,n),E= 16,18,20 MeV; U Sn(a,n),E=18 MeV; n ¢ S n ( a , 2 n ) , E = 3 3 , 2 4 MeV; U S S n ( a , 2 n ) , E = 3 3 MeV; 1 0 6 P d ( I a C , 2 n ) , E = 5 8 MeV; u ° P d ( t s C , 3 n ) , E = 4 0 , 4 5 , 4 9 , 5 2 MeV; u ° C d ( 1 3 C , 3 n ) , E = 5 2 MeV; m e a s u r e d T T - c o i n , T ( 0 ) , a ( E T ) . lls,n0,1ao,laaTe,la0Xe d e d u c e d levels,J,~r. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 25 813. NUCLEAR REACTIONS n ° , i l ° S n ( a , 2 n ) , E = 2 2 - 3 3 MeV; m e a s u r e d ET,IT,TT(0),a(ET,0),I(ce),linear polarization, lls,laOTe d e d u c e d levels,J,rr,7-branching,& Enriched targets,Ge(Li),Si-Li detectors. Interacting boson approximation,broken p a i r m o d e l . NUPAB 380 125.

A

~2OAg

=

KEYWORDS

NUCLEAR REACTIONS 9 ° Z r ( % T ' ) , E = 8 4 9 6 k e V ; l l a S n ( 7 , T ' ) , E = 6 3 2 5 , 6 9 8 8 k e Y ; t Z ° S n ( T , 7 ' ) , E = 6 7 3 0 keV; measured ET,IT,TT(0),cr. 9 ° Z r , U ° , l a ° S n t r a n s i t i o n s d e d u c e d FT,Tt/2. IA NF A 4 6 57. NUCLEAR REACTIONS nSSn(7,T%E=6.988 MeV; m e a s u r e d ET,IT; d e d u c e d cr. nSSn l e v e l d e d u c e d J,F,FT. Y A F I A 35 1361. NUCLEAR REACTIONS u 2 , u a , n s , t l o , u T , 1 1 8 , u g , l z o , t z 2 , 1 2 4 S n ( p , d ) , E _ 3 0 _ MeV; m e a s u r e d G(Ep),ff(0). 112,114,116,118,120,122,124Sn d e d u c e d occupation probabilities, i l l . l l a. 1t4 . H5116 . . .l i t . it0. t l.a tzl

A tlaAg

AND

character.

NUPAB

388

I.

NUCLEAR REACTIONS 112,114,115,116,117 , I18 ,119,120,122,124Sn(p, d), E-90-~ MeV; m e a s u r e d cr ( E p ) , a ( 0 ) . 112,114,116,118,12°,122,124Sn d e d u c e d occupation probabilities, l l i 113 114 115 116 117 lib 119 121 123Sn d e d u c e d tevels,J,Tr,S. Finite-range DWBA a n a l y s i s . C J P H A 60 428.

55

KEY

NUMBERS

A 12OSn

R 8~Ga02

82Gu02

12OTe

R 82Ch01

82Va10

12OXe

R 82Ch01

D 82A129:

la*Cd

D 82A129

82Fo'04

lalin

D 82Fo04

la~Sn

D 82Ha31 R 8~F102

'21Sb

D 82Ha31

12*Te

R 82Ga18

1211

R 82Ga21

82Ha46:

121Xe

R 82Ba31:

R 82F102:

122Te

R 82Ch01:

lZaXe

R 82Ha44:

120

continued

=

121

R A D I O A C T I V I T Y **6,uT,1*s,ug,*ao,121Ag [ f r o m fission product mass separation3; 119,121Cd [ f r o m n6,1alAg(ft-) d e c a y ] ; m e a s u r e d f t T - c o i n ; d e d u c e d Q f l , m a x i m u m Eft,mass excess. Fission product mass separation,Ge(Li),Si-Li d e t e c t o r s . P R V C A 26 1157. RADIOACTIVITY n6,nT,n6,ng,12°,12*Ag [from fission product mass separation3; ng,ialCd [ f r o m ng,12*Ag(ft-) d e c a y 3 ; m e a s u r e d f t y - c o i n ; d e d u c e d Q f t , m a x i m u m Eft,mass excess. Fission product mass separation,Ge(Li),Si-Li d e t e c t o r s . P R V C A 26 1157. R A D I O A C T I V I T Y 121,121mCd [ f r o m 23SU(n,F),isotope separated sources3; measured TI/2,ET,IT, I(ce),77-coin,ftT(t). lelIn deduced levels J,Tr,7-multipolarity,B(E1),B(E2 ). G e ( L i ) , hyperpure Ge,Si-Li,Nal,plastic d e t e c t o r s . N U P A B 376 389. R A D I O A C T I V I T Y 121,121mCd [ f r o m 235U(n,F),isotope separated sources3; measured TI/a,ET,IT, I(ce),77-coin,ftT(t). lZiIn deduced levels J,~,7-multipolarity,B(E1),B(E2). Ge(Li), hyperpure Ge,Si-Li,Nal,plastic detectors. N U P A B 376 389. R A D I O A C T I V I T Y 121mSn; m e a s u r e d ET,IT,E(X-ray),l(X-ray),ftT(t). l~lSb l e v e l d e d u c e d T l / e . Z P A A D 305 347. NUCLEAR REACTIONS n a , u 4 , u s , u 6 , i l T , u s , n g , 1 2 o , 1 2 2 , 1 2 4 S n ( p , d ) , E = 2 0 MeV; m e a s u r e d a(Ep),a(0). 112,114,116,118,120,122,124Sn d e d u c e d occupation probabilities, u1,1,3,**4,115116,11~,116,119,,2, 123Sn d e d u c e d l e v e l s , J j r , S . F i n i t e - r a n g e DWBA a n a l y s i s . C J P H A 60 428. R A D I O A C T I V I T Y 121mSn; m e a s u r e d E T , I T , E ( X - r a y ) , I ( X - r a y ) , f t T ( t ). 121Sb l e v e l d e d u c e d TI/2. Z P A A D 305 347. NUCLEAR REACTIONS 124,13°Te(3He,cx),E=70 MeV; m e a s u r e d a(Ec~,0). 122,124,13°Te(p,d),E=42 MeV; measured a(0). 121,12~,1~9Te d e d u c e d levels,L,J,Tr,CzS. Enriched targets,magnetic spectrometer. DWBA,inner-shell a n a l y s i s . N U P A B 381 173. NUCLEAR REACTIONS u ~ , n 6 , n S S n ( 6 L i , 3 n ) , E = 3 3 MeV; m e a s u r e d ET,IT,a(ET),7(0),77-coin,7(t), 7(0,H,t). ~7,1~9,1~lI d e d u c e d levels,J,Tr,isomer T,/2,6(E2/M1),7-branching ratio, lziI d e d u c e d i s o m e r g. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 26 1101. NUCLEAR REACTIONS lal Sb( 3He,3n),E=24.3,27.5,29.9,32.0 MeV; m e a s u r e d E(7),I(7),g(E,ET,07), 3HeT(t),77-coin,IT(0,t,H). 1ali d e d u c e d levels,J,~r,T,/z,g. Enriched 121Sb t a r g e t , G e ( L i ) detectors. Core-quasiparticle coupling calculations. N U P A B 389 341. NUCLEAR REACTIONS no,u2Cd(12C,3n),E=52-75 MeV; m e a s u r e d a ( E , E T , 0 ) , 7 7 - c o i n , 7 7 ( t ). l19,1~lXe deduced levels,J,w,T~/2. Enriched targets,Ge(Li) detectors. Interacting boson fermion m o d e l . N U P A B 383 309.

A IZaSn

=

KEYWORDS

NUCLEAR REACTIONS 90Zr,la°Sn,144Sm,aOSpb(p,p'),E=800 MeV; m e a s u r e d a(0). 9°Zr,la°Sn,~44Sm, Z°epb,4°Ca,56Ni d e d u c e d d e f o r m a t i o n lengths,neutron,proton matrix element ratios. Optical m o d e l , D W B A a n a l y s e s . P R V C A 25 498. NUCLEAR REACTIONS 54,56Fe,SS,OONi,lZOSn,ZOSpb(polarized n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 54, 56Fe,56,6ONi,~ZOSn,ZOSpb l e v e l d e d u c e d s p i n - o r b i t to C o u l o m b d e f o r m a t i o n parameter ratio. Coupled-channels a n a l y s i s . P R V C A 25 2 8 5 4 . NUCLEAR REACTIONS n ~ S n ( a , n ) , E = 1 6 , 1 8 , 2 0 MeV; n9Sn(c~,n),E=18 MeV; n 4 S n ( a , 2 n ) , E = 2 2 , 2 4 MeV; n6Sn(a,2n),E=22 MeV; l ° 6 P d ( 1 2 C , 2 n ) , E = 5 8 MeV; u ° P d ( l ~ C , 3 n ) , E = 4 0 , 4 5 , 4 9 , 5 2 MeV; l~°Cd(l~C,3n), E=52 MeV; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) , c r ( E T ) . ~16,118,1e°,~Z~Te,la°Xe d e d u c e d l e v e l s , J , ~ . E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 25 813. NUCLEAR REACTIONS n 6 , n e S n ( c ~ , 2 n ) , E = 2 2 - 3 3 MeV; m e a s u r e d E%IT,77(0),a(E7,0),I(ce),linear polarization. *ls,la°Te deduced levels,JJT,7-branching,& Enriched targets,Ge(Li),Si-Li detectors. Interacting boson approximation,broken p a i r m o d e l . N U P A B 380 125. NUCLEAR REACTIONS n~Sn(~,n),E=16,18,20 MeV; ngsn(~x,n),E=18 MeV; n 4 S n ( a , 2 n ) , E = 2 2 , 2 4 MeV; U ~ S n ( ~ x , 2 n ) , E = 2 2 MeV; l ° 6 P d ( l ~ C , 2 n ) , E = 5 8 MeV; n o p d ( l ~ C , 3 n ) , E = 4 0 , 4 5 , 4 9 , 5 2 MeV; ~l°Cd(13C,3n), E=52 MeV; m e a s u r e d 77-coin,7(0),a(E7). n6,~*8,1e°,laaTe,la°Xe d e d u c e d l e v e l s , J , T r . E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 25 813.

A '2lAg

AND

=

122

NUCLEAR REACTIONS 112,114,115,116,nT,us,ug,lzo,122,124Sn(p,d),E_20_ MeV; m e a s u r e d a(Ep),a(0). 112,114,116,118,12°,122,124Sn d e d u c e d occupation probabilities. 111 113,114 115 116 117 118,119,121, 123Sn d e d u c e d l e v e l s , J j r , S . F i n i t e - r a n g e DWBA a n a l y s i s . C J P H A 60 428. NUCLEAR REACTIONS n T S n ( a , n ) , E = 1 6 , 1 8 , 2 9 MeV; n g S n ( a , n ) , E = 1 8 MeV; n4Sn(cx,2n),E=22,24 MeV; U 6 S n ( a , 2 n ) , E = 2 2 MeV; l ° 6 P d ( 1 2 C , 2 n ) , E = 5 8 MeV; n O p d ( 1 3 C , 3 n ) , E = 4 0 , 4 5 , 4 9 , 5 2 MeV; ll°Cd(13C,3n), E=52 MeV; m e a s u r e d 77-coin,7(0),a(ET). l16,118,l~°,122Te,laOXe d e d u c e d l e v e l s , J , T r . E n r i c h e d £ a r g e t s , G e ( L i ) d e t e c t o r s . P R V C A 25 813. NUCLEAR REACTIONS 122124 , , 126Te( 3 H e , 3 n ) , E = 2 0 - 2 7 MeV; m e a s u r e d ET,IT,I(ce),7(0),~(ET) v s E, 77-coin. 122,124,126Xe d e d u c e d levels,J,Tr,ICC,6,7-branching,band structure, lZ6Xe d e d u c e d i s o m e r J j T , T , / 2 . PHSTB 26 205.

56

KEY

NUMBERS

A

123Sn

123Te

R 82F102:

R 81Io05: 82Ga18:

1231

R 82Ca10: 82Sh20:

123Xe

D 82No03:

R

82DjO4

82F102

124 I

R 82Bu12 82Ca10

~24Xe

R 82Ha44

D 82Co05 R 82Ma04

~25Te

D 82Br16

82Mu02

1251

D 82Br16

R

82Sh20

R 82Ha44

MeV; m e a s u r e d

a(Ep),cr(0).

111,113,114,115,116,117,118119,121,

=

124

NUCLEAR REACTIONS 51V,5S,6°,62Ni,SSZn,9°,o2,94,SSZr,O2,sa,v6,os,l°°Mo,12°,124Sn,t4°Ce(p,p'),E=200 MeV; m e a s u r e d a t 0 ) . 51V,5S,66,62Ni,SSZn,9°,sa,94,96Zr,92,sa,96,98,1°°Mo,12°,124Sn,146Ce d e d u c e d resonances,F,T,M1 character. NUPAB 388 1. NUCLEAR REACTIONS 112,114,115,11s,llT,11e,lls,la°,122,124Sn(p,d),E=20 MeV; m e a s u r e d a(Ep),cr(O). 112,114,116,118,12°,122,124Sn deduced occupation probabilities. 111113114,I15116,117,118,119121, 123Sn d e d u c e d l e v e l s , J , y r , S . F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS 124Te(p,n),E=3.9-6 MeV; m e a s u r e d E?,I%-y?-coin,?3,(t),I?(0). 124I d e d u c e d levels,J,lr,?,T1/2,?-multipolarity. E n r i c h e d t a r g e t . NUPAB 385 29. NUCLEAR REACTIONS I S T A u , 1 2 1 S b ( a , n ) , ( a , 2 n ) , E = l l . 5 - 2 7 MeV; m e a s u r e d or(E). 2°6,199T1,~24,123I deduced level density,average ?-strength. NUPAB 383 251. NUCLEAR REACTIONS 122,12%126Te(3He,3n),E=20-27 MeV; m e a s u r e d E%I?,l(ce),'y(0),cr(E?) v s E, ??-coin. 122,124,126Xe d e d u c e d l e v e l s , J , ~ r , I C C , 6 , ? - b r a n e h i n g , b a n d structure. 126Xe d e d u c e d i s o m e r J,Tr,T1/2. PHSTB 36 205.

=

125

R A D I O A C T I V I T Y 125Sb,154,155Eu; m e a s u r e d E?,I?,E(X-ray),l(X-ray); deduced photon,X-ray emission rates. Separated,mixed s o u r c e s . NUIMA 193 1. NUCLEAR REACTIONS 28Si,54Fe,SSNi(3He,3He),(3He,d),E=90 MeV; 9°Zr(3He,3He),(3He,d),E=89.3 MeV; 124Sn(3He,3He),(3He,d),E=89.8 MeV; m e a s u r e d or(0); d e d u c e d o p t i c a l p o t e n t i a l s . 29p,55Co, 59Cu,91Nb,125Sb l e v e l s d e d u c e d spectroscopic f a c t o r s . DWBA a n a l y s e s . E n r i c h e d , n a t u r a l t a r g e t s . NUPAB 373 377. R A D I O A C T I V I T Y IzSI(EC) [ f r o m 124Xe(n,?)125Xe(decay)]; measured I(ce). 125Te t r a n s i t i o n d e d u c e d I C C , s u b s h e l l r a t i o s , & I r o n y o k e rr s q u a r e r o o t 2 m a g n e t i c s p e c t r o m e t e r . ZPAAD 306 347. RADIOACTIVITY 125mTe E f r o m 125Sb d e c a y ] ; m e a s u r e d E%I?,E(K X - r a y ) , I ( K X - r a y ) . lZ5Te t r a n s i t i o n s d e d u c e d ICC. C h e m i c a l s e p a r a t i o n , G e ( L i ) d e t e c t o r , X - , ? - r a y s u m s p e c t r a . PRVCA 25 2120. R A D I O A C T I V I T Y 125I(EC) [ f r o m 124Xe(n,~)lZSXe(decay)3; m e a s u r e d I(ce). 125Te t r a n s i t i o n d e d u c e d I C C , s u b s h e l l r a t i o s , & I r o n y o k e ~r s q u a r e r o o t 2 m a g n e t i c s p e c t r o m e t e r . ZPAAD 306 347. NUCLEAR REACTIONS 12°,122,124Sn(SLi,3n),E=32-34 MeV; m e a s u r e d E ? , I % 7 ? - c o i n , I ? ( E , 0 , t ) . 123, 125,127I d e d u c e d l e v e l s , J J r , i s o m e r T l / 2 , ? - b r a n c h i n g r a t i o , ~ ( E 2 / M 1 ) , b a n d s t r u c t u r e . PRVCA 26 1089.

A

126Xe

123

123Sn d e d u c e d l e v e l s , J J r , S . F i n i t e - r a n g e DWBA a n a l y s i s . CJPHA 60 428. NUCLEAR REACTIONS 1 2 ° S n ( a , n ) , E = 2 5 MeV; 123Sb(d,2n),E=12.5 MeV; m e a s u r e d ?(t),?(0,H,t). 123Te d e d u c e d i s o m e r , T 1 / a , J , T r , t t . RRPQA 26 239. NUCLEAR REACTIONS 124,12°Te(3He,a),E=70 MeV; m e a s u r e d a(Ea,0). 12a,124,130Te(pd), ,E-42- MeV; measured (7(0). 121,123,129Te d e d u c e d levels,L,J,Tr,C2S. Enriched targets,magnetic spectrometer. DWBA,inner-shell a n a l y s i s . NUPAB 381 173. NUCLEAR REACTIONS 197Au,121Sb(a,n),(a,2n),E=ll.5-27 MeV; m e a s u r e d or(E). 266,100Tl,124,1e31 deduced level density,average ?-strength. NUPAB 383 251. NUCLEAR REACTIONS 12°,122,124Sn(SLi,3n),E=32-34 MeV; m e a s u r e d E ? , I ? , ? ? - c o i n , I ? ( E , e , t ) . 123 125,127I d e d u c e d l e v e l s , J , r r , i s o m e r T 1 / 2 , ~ / - b r a n c h i n g r a t i o , 6 ( E 2 / M l ) , b a n d s t r u c t u r e . PRVCA 26 1089. R A D I O A C T I V I T Y 123Xe [ f r o m Xe(%n),E=40 MeV b r e m s s t r a h l u n g ] ; m e a s u r e d E%I7; d e d u c e d 123I y i e l d . L i q u i d x e n o n t a r g e t , G e ( L i ) d e t e c t o r . I J A R A 33 183.

A

125Sb

=

KEYWORDS

NUCLEAR REACTIONS 112,114,115,116,117,11s,lls,120,122,124Sn(p,d),E-20_ 112,114,116,118,12°,122,124Sn deduced occupation probabilities.

A

124Sn

AND

=

126

NUCLEAR REACTIONS 122,124,1ZSTe(3He,3n),E=20-27 MeV; m e a s u r e d ??-coin. lz2,124,12SXe d e d u c e d l e v e l s , J , r r , l C C , d , ? - b r a n c h i n g , b a n d i s o m e r J,Tr,TI/2. PHSTB 26 205.

57

E%I%I(ce),~/(0),cr(E?) v s E, structure. 126Xe d e d u c e d

KEY

NUMBERS

A 1271

R 83Sh20:

127La

D

83No03:

82A110:

R

81Bu22:

138Cs

D 82La15

128Ba

D

82La15

=

=

D 82HuO9

129Sb

D

82HuO9

129Te

D

82Hu09

R 82Ga18

1291

R

81De35:

iag~ a

D

82La15

D

82Ur01

J

82Gr14

130La

D 82Ur01:

t3OCe

D

82No02:

D 82Pr01:

129

=

130

RADIOACTIVITY 13°La [ f r o m 13°Ba(p,n),E=10 MeV]; m e a s u r e d E v , I ? , v V - c o i n ; d e d u c e d log ft. 13°Ba d e d u c e d levels,J,zr,B(E2) r a t i o s , i n t r i n s i c quadrupole moment. Enriched target,Ge(Li) d e t e c t o r s . ZPAAD 305 335. NUCLEAR MOMENTS 135,137Ba; m e a s u r e d isotope shifts,hfs; deduced electric quadrupole moments. 137,136,135,134,13°Ba d e d u c e d c h a r g e r m s r a d i i c h a n g e r e l a t i v e to ~3SBa. H i g h resolution laser fluoresence spectroscopy. Self-consistent f i e l d c a l c u l a t i o n s . ZPAAD 306 195. RADIOACTIVITY i3°La [ f r o m 13°Ba(p,n),E=10 MeV3; m e a s u r e d E v , I v , v T - c o i n ; d e d u c e d log ft. la°Ba d e d u c e d l e v e l s , J j r , B ( E 2 ) r a t i o s , i n t r i n s i c quadrupole moment. Enriched target,Ge(Li) d e t e c t o r s . ZPAAD 305 335. RADIOACTIVITY 127La,la°,131Ce [ f r o m liSIn,US,nT,nSsn(lnO,X),(lSO,X),E=75-85 MeVS; m e a s u r e d ??-coin. 13°,131Ce d e d u c e d yrast levels,J,Tr,backbending,hn/2 proton alignment. 127La d e d u c e d l e v e l s , J , w . E n r i c h e d I n , S n t a r g e t s . PYLBB 108 269.

A lalSb

138

RADIOACTIVITY lagsn(fl-),lagSb(fl-) [ f r o m 2 3 5 U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d E T , I T , 7 7 - c o i n , T l / 2 . 129Sb,tagTe d e d u c e d l e v e l s , 7 - b r a n c h i n g . Ge(Li) d e t e c t o r s , o n - l i n e m a s s s e p a r a t i o n . PRVCA 26 621. RADIOACTIVITY lagSn(fl-),t29Sb(fl-) [ f r o m 2 3 5 U ( n , F ) , E = t h e r m a l S ; m e a s u r e d E T , l % 7 7 - c o i n , T w a . 129Sb,129Te d e d u c e d l e v e l s , v - b r a n c h i n g . Ge(Li) d e t e c t o r s , o n - l i n e m a s s s e p a r a t i o n . PRVCA 26 621. RADIOACTIVITY taaSn(fl-),tagSb(fl-) [ f r o m a a 5 U ( n , F ) , E = t h e r m a l 3 ; m e a s u r e d E % I T , 7 7 - c o i n , T t / 2 . lagSb,tagTe d e d u c e d l e v e l s , ? b r a n c h i n g . Ge(Li) d e t e c t o r s , o n - l i n e m a s s s e p a r a t i o n . PRVCA 26 621. NUCLEAR REACTIONS 124,130Te(aHe,a),E=70 MeV; m e a s u r e d a(Ea,0), la2,124,13°Te(p,d),E=42 MeV; measured o(0). lat,laa,129Te deduced levels,L,J,Tr,C2S. Enriched targets,magnetic spectrometer. DWBA,inner-shell a n a l y s i s . NUPAB 381 173. NUCLEAR REACTIONS 129I(7,7'),E=27.8 keV; m e a s u r e d M o s s b a u e r s p e c t r a . 129I levels d e d u c e d g ratio hyperfine anomaly. Shell model,configuration admixtures. PYLBB 106 457. RADIOACTIVITY 1 2 8 B a ( E C ) , l a 9 m B a ( E C ) , ( f l + ) , t 2 9 B a ( E C ) , ( f l + ) , 1 3 I B a ( E C ) [ f r o m laaCs(p,xnyp), E = 3 6 . 4 - 6 7 MeV3; 12SCs [ f r o m 12SBa d e c a y ] ; m e a s u r e d E7,I7. CsC1 t a r g e t , e l u t i o n teehique. I J A R A 33 619.

A 13OBa

137

RADIOACTIVITY laSl [ f r o m n e u t r o n i r r a d i a t i o n of 12713; m e a s u r e d E v , I v , v V - c o i n ; d e d u c e d levels,J,Tr,v-multipolarity,v-branching. IANFA 46 53. NUCLEAR REACTIONS * 2 S T e ( p , n ) , E = 2 . 8 - 5 MeV; m e a s u r e d Ev,Iv,vV-coiin,vT(t),I?(0). 128I deduced levels,JJr,v-multipolarity,7-branching,eonfigurations. Enriched t a r g e t . NUPAB 351 238. RADIOACTIVITY 1 2 8 B a ( E C ) , l a g m B a ( E C ) , ( f l + ) , ~ a a B a ( E C ) , ( f l + ) , l a l B a ( E C ) [ f r o m 133Cs(p,xnyp), E = 3 6 . 4 - 6 7 MeVS; 122Cs [ f r o m ~28Ba d e c a y 3 ; m e a s u r e d E7,17. CsC1 t a r g e t , e l u t i o n techique. I J A R A 33 619. RADIOACTIVITY 1 2 8 B a ( E C ) , l z g m B a ( E C ) , ( f l + ) , I a g B a ( E C ) , ( f l + ) , I 3 1 B a ( E C ) [ f r o m 133Cs(p,xnyp), E = 3 6 . 4 - 6 7 MeVS; *ZSCs [ f r o m laSBa d e c a y 3 ; m e a s u r e d E7,I7. CsCI t a r g e t , e l u t i o n techique. I J A R A 33 619.

A = 129Sn

KEYWORDS

NUCLEAR REACTIONS ta°,laa,ia4Sn(SLi,3n),E=33-34 MeV; m e a s u r e d E v , I T , v T - c o i n , 1 7 ( E , 0 , t ). taa 125,127I d e d u c e d l e v e l s , J , T r , i s o m e r T l / 2 , v - b r a n e h i n g r a t i o , 6 ( E 2 / M t ) , b a n d s t r u c t u r e . PRVCA 26 1089. RADIOACTIVITY ta?La,la°,i31Ce [ f r o m n S I n , U S , n ? , n S S n ( l S O , X ) , ( l S o , x ) , E = 7 5 - 8 5 MeVS; m e a s u r e d 7V-coin. 13°,131Ce d e d u c e d yrast levels,J,~r,backbending,hu/2 proton alignment, la?La d e d u c e d l e v e l s , J j r . E n r i c h e d I n , S n t a r g e t s . PYLBB 108 269.

A D

AND

=

131

RADIOACTIVITY 9°rny,lalmSb [ f r o m ZaSU(?,F),E=50 MeV b r e m s s t r a h l u n g 3 ; m e a s u r e d ET,I%T1/z. electron beam,rotating a38U t a r g e t , G e ( L i ) s p e c t r o m e t e r . NUIMA 192 447.

Pulsed

58

KEY

NUMBERS

A i311

D 82Gi02

8~Ha37 131Xe

D

83Gi03

82Ha37 131Cs

D 78Ba81 831s04

~31Ba

D 82La15

131Co

R

8BBu07

D

8BNo03

D 82Bj02

132Sn

D

83Bj03

82Ka35 ~3eLa

R

8~Bu07

R 82Wa14

t33Ba

R

82Bu07

D 83A101:

134Cs

D 80Ru03: R 81Bo42: 83Bu07:

continued

=

132

=

133

NUCLEAR REACTIONS 13°Te(a,n),E-10 53.5 MeV; m e a s u r e d a b s o l u t e or(E); d e d u c e d t h i c k t a r g e t yields,iaam,iaaxe saturation production r a t e s . 133Xe d e d u c e d ff(isomer)/cr(ground state). Activation technique. R R A L A 50 307. NUCLEAR REACTIONS 142~14~144~145~46~1~5~Nd~4iPr~14~Ce~39La~Ba(7r~xnyp)~38Pr/132La/~a?Ba/ i35Ba/laaBa/lalBa/laScs/la4Cs/135Xe/,E a t r e s t ; m e a s u r e d E,/,I,/; d e d u c e d r e a c t i o n m e c h a n i s m . 134m,135mCs d e d u c e d isomer,J,vr,Ti/2,cr(production) r a t i o . 137rn,135m,133m,131mBa,laamLa,137mCe, t38mpr deduced isomer,JJr. 133,131Ba d e d u c e d a ( i s o m e r ) / c r ( g r o u n d s t a t e ) . N U P A B 382 501.

A

134Sb

131

R A D I O A C T I V I T Y main [ f r o m U(p,X),E=600 MeVV; m e a s u r e d , / 7 - c o i n f o l l o w i n g B - d e c a y ; d e d u c e d log f t , f l - b r a n c h i n g , T 1 / 2 , G a m o w - T e l l e r transition, la2Sn d e d u c e d levels,J,rr,7-branching, B(E]),configuration,shell c l o s u r e . Z P A A D 306 95. R A D I O A C T I V I T Y main [ f r o m U(p,X),E=600 MeV]; m e a s u r e d 7 , / - c o i n f o l l o w i n g B - d e c a y ; d e d u c e d log f t , f l - b r a n c h i n g , T t / a , G a m o w - T e l l e r transition. 132Sn d e d u c e d levels,J,vr,,/-branching, B(EV),configuration,shell c l o s u r e . Z P A A D 306 95. R A D I O A C T I V I T Y 13aSn(fl-) [ f r o m f i s s i o n p r o d u c t s e p a r a t i o n ] ; m e a s u r e d `//`/-coin. ~3aSn l e v e l s d e d u c e d T l / 2 , B O , ) , s h e l l c l o s u r e e f f e c t s . Z P A A D 308 33. NUCLEAR REACTIONS 14~43~44~45~46~48~5~Nd~141Pr~4~Ce~9La~1a~Ba(7r~nyp)13~Pr/~zLa/~7Ba/ 135B a / 133B a / 131B a / 135C s / 134 C s / 135X e / , E a t r e s t ; m e a s u r e d Ev,1,/; d e d u c e d r e a c t i o n m e c h a n i s m . 134rn,135rncs d e d u c e d i s o m e r , J , v r , T l / a , c r ( p r o d u c t i o n ) r a t i o . 137m,135m,133m,131mBa,132mLa,13?mCe, 138mpr d e d u c e d i s o m e r , J j r . 133,131Ba d e d u c e d ~ r ( i s o m e r ) / c r ( g r o u n d s t a t e ) . NUPAB 382 501.

A 133Xe

=

KEYWORDS

R A D I O A C T I V I T Y is'I; m e a s u r e d 7(O,~),linear polarization,oriented n u c l e i . 131Xe t r a n s i t i o n d e d u c e d E2,M1 m u l t i p o l a r i t y relative phase,time reversal invariance. Ion implantation in Fe,dilution refrigerator c o o l i n g . P R V C A 35 1567. R A D I O A C T I V I T Y 1311,75Se; m e a s u r e d E%l,/,V,/-coin. lSlXe,VSAs l e v e l s d e d u c e d ` / - b r a n c h i n g . S u m coincidence spectometer. NUIMA 198 305. R A D I O A C T I V I T Y 1311; m e a s u r e d ,/(0,~),linear polarization,oriented n u c l e i , lalXe t r a n s i t i o n d e d u c e d E2,M1 m u l t i p o l a r i t y relative phase,time reversal invariance. Ion implantation in Fe,dilution refrigerator c o o l i n g . P R V C A 25 1567. R A D I O A C T I V I T Y m~I,7%e; m e a s u r e d E % l v , , / 7 - c o i n . 13~Xe,?SAs l e v e l s d e d u c e d 7 - b r a n c h i n g . S u m coincidence spectometer. NUIMA t 9 8 305. R A D I O A C T I V I T Y la~Cs; m e a s u r e d Auger spectra. Magnetic beta-spectrometer. PIFLD 8 36. R A D I O A C T I V I T Y 131Cs [ f r o m 13°Ba(n,7)lalBa(EC)decay]; measured (K X - r a y ) ( K X-ray)-, ,/(X-ray)-coin; deduced double K-hole creation probability,hypersateilite energy shift,IB photon intensity,K X-ray intensity r a t i o . P R V C A 25 3078. R A D I O A C T I V I T Y teSBa(EC),iagmBa(EC),(fl+),~agBa(EC),(fl+),laiBa(EC) [ f r o m laaCs(p,xnyp), E = 3 6 . 4 - 6 7 M e V ] ; 1SaCs [ f r o m ~ZSBa d e c a y S ; m e a s u r e d E,/,1,/. CsCI t a r g e t , e l u t i o n techique. I J A R A 33 619. NUCLEAR REACTIONS i42~43~1~4~45~i4s~148~5~Nd~4~Pr~4~e~39La~i3~Ba(7r~xnyp)138~r/1~La/i~7Ba/ 135Ba/IaaBa/131Ba/135Cs/134Cs/135Xe/,E a t r e s t ; m e a s u r e d E,/,I,/; d e d u c e d r e a c t i o n m e c h a n i s m . 134m,135mcs d e d u c e d i s o m e r , J j r , T l / a , c r ( p r o d u c t i o n ) r a t i o . 137m 135m,133m,131mBa,132mLa 137mCe ' ~38mpr d e d u c e d i s o m e r , J j r . i3a,i31Ba d e d u c e d a ( i s o m e r ) / c r ( g r o u n d s t a t e ) . N U P A B 382 501. R A D I O A C T I V I T Y leVLa,i3o,131Ce [ f r o m n 5 1 n , n 6 , n 7 , n S S n ( 1 6 0 , X ) , ( ~ 8 0 , X ) , E = 7 5 - 8 5 MeVV; m e a s u r e d ` / ` / - c o i n . 13°,lanCe d e d u c e d yrast levels,J,rr,backbending,hn/a proton alignment, la?La deduced levels,J,rr. Enriched I n , S n t a r g e t s . PYLBB 108 269.

A 1321n

AND

=

134

RADIOACTIVITY 86,87,88,89BF,89,91,9a,93K F,89,91,92,93,94 R b,93,94,95Sr,94,95,96 y,134S b,136,137,138 139I, 137,138,139,140,141Xe,138,139,140,141,142Cs; m e a s u r e d average Eft. F i s s i o n products,B-strength functions input,Si-Li detector s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 134Cs(fl-); ll0rnAg(/?-); m e a s u r e d ,/,/(e),oriented n u c l e i . 134Ba,ll°Cd l e v e l d e d u c e d 6 ( E 2 / M 1 ) . NUIMA 173 4 8 9 . NUCLEAR REACTIONS 1 3 3 C s ( n , 7 ) , E = t h e r m a l ; m e a s u r e d E,/,I,/,I(ce),,/,/ coin. 13¢Cs d e d u c e d l e v e l s , J,w,configuration,,/-transition multipolarity. F Z K A A 13 40. NUCLEAR REACTIONS ~4a~43,~44~45~4s~i48~5~Nd~4~P~4~Ce~39La~38Ba(~.-~nyp)~3~Pr/~3~La/~37Ba/ iaSBa/iaaBa/lalBa/135Cs/la4Cs/laSXe/,E at rest; measured E,/,I,/; d e d u c e d r e a c t i o n m e c h a n i s m . 134m,135mCs d e d u c e d i s o m e r , J j r , T l / a , c T ( p r o d u c t i o n ) ratio. 137rn,I35m,133m,131mBa,132mLa,137mCe, 13Smpr d e d u c e d i s o m e r , J , r r , laa,lalBa d e d u c e d c r ( i s o m e r ) / ~ ( g r o u n d s t a t e ) . N U P A B 382 501.

59

KEY

NUMBERS

A 134Cs

R 82Ma33:

134Ba

D 80Ru03: J

83Gr14:

82Sh05:

134Ce

R 8~Ze04:

R 82Bu07:

135Ba

J

82Gr14:

B2Grl5:

83Ri03: 8ZSh05:

=

134

KEYWORDS

continued

NUCLEAR REACTIONS 133Cs(n,3"),E=~.66-600 keV; m e a s u r e d a ( c a p t u r e ) v s E. 134Cs d e d u c e d resonances,F3",resonanee parameters. NSENA 81 418. RADIOACTIVITY 134Cs(/~-); l l ° m A g ( f l - ) ; m e a s u r e d 77(0),oriented n u c l e i . 134Ba,u°Cd l e v e l d e d u c e d 6 ( E 2 / M I ) . NUIMA 173 489. NUCLEAR MOMENTS 135,137Ba; m e a s u r e d isotope shifts,hfs; deduced electric quadrupole moments. 137,13s,135,134,13°Ba d e d u c e d c h a r g e r m s r a d i i c h a n g e r e l a t i v e to 13eBa. H i g h resolution laser fluoresence spectroscopy. Self-consistent f i e l d c a l c u l a t i o n s . ZPAAD 306 195. NUCLEAR MOMENTS 13~,135,ms,137,13SBa; m e a s u r e d m u o n i c X - r a y s ; d e d u c e d c h a r g e d i s t r i b u t i o n s , isotope shifts. Droplet model,interacting boson approximation calculations. PYLBB 112 124. NUCLEAR REACTIONS *ZaSn(~60,4n),E=75,80 MeV; m e a s u r e d I3"(E),~(t),3"3"-coin,reeoil,T(0), o r i e n t e d n u c l e i . 134Ce d e d u c e d l e v e l s , J j r , O , T i / ~ , g . Fe,Gd h o s t s . NUPAB 383 165.

A

135Cs

AND

=

135

NUCLEAR REACTIONS i42~i43~144~145~i4s~i4~i5~Nd~4lPr~i4~e~i39La~13sBa(1r~xnyp)i3~Pr/13~La/137Ba/ 135Ba/133Ba/131Ba/135Cs/134Cs/135Xe/,E a t r e s t ; m e a s u r e d E%I7; d e d u c e d r e a c t i o n m e c h a n i s m . 134m,135mCs d e d u c e d i s o m e r , J , T r , T 1 / a , a ( p r o d u c t i o n ) r a t i o . 137m 135m 133m 131mBa,13gmLa 137raCe ' 13erupt d e d u c e d i s o m e r , J , ~ r . 133,i31Ba d e d u c e d c r ( i s o m e r ) / c r ( g r o u n d s t a t e ) . NUPAB 382 501. NUCLEAR MOMENTS 135,137Ba; m e a s u r e d isotope shifts,hfs; deduced electric quadrupole moments. 137,136,135,134,13°Ba d e d u c e d c h a r g e r m s r a d i i c h a n g e r e l a t i v e to 13SBa. H i g h resolution laser fluoresence spectroscopy. Self-consistent f i e l d c a l c u l a t i o n s . ZPAAD 306 195. NUCLEAR MOMENTS 135,13s,lsT,13~Ba; m e a s u r e d h f s . 135,13B,137Ba d e d u c e d i s o t o p e s h i f t r e l a t i v e to 13SBa. H i g h r e s o l u t i o n l a s e r s p e c t r o s c o p y . ZPAAD 306 281. NUCLEAR MOMENTS 135,137,138Ba; m e a s u r e d o p t i c a l i s o t o p e s h i f t s . ZPAAD 306 11. NUCLEAR MOMENTS 134,135,136,137,13aBa; m e a s u r e d m u o n i c X - r a y s ; d e d u c e d c h a r g e d i s t r i b u t i o n s , isotope shifts. Droplet model,interacting boson approximation calculations. PYLBB 112

124. R

135Ce

R

82Bu07:

82Ze01:

NUCLEAR REACTIONS •4a•143••44••45••46••48••5•Nd••4•P••14•Ce••39La••38Ba(Tf-••nyp)•3•P•/•32La/•37Ba/ 135Ba/133Ba/131Ba/135Cs/134Cs/135Xe/,E a t r e s t ; m e a s u r e d E7,I3"; d e d u c e d

reaction mechanism. 134m,135mCs d e d u c e d i s o m e r , J , T r , T ~ / 2 , a ( p r o d u c t i o n ) r a t i o . 137m,135m,133m,131m~a,132mLa,I37mCe, 13Smpr d e d u c e d i s o m e r , J , T r . 133,13'Ba d e d u c e d a ( i s o m e r ) / a ( g r o u n d s t a t e ) . NUPAB 382 501. NUCLEAR REACTIONS lZaSn(160,3n),E=6~ MeV; m e a s u r e d E%I3",3"(t),recoil,3"(0,H). 135Ce l e v e l d e d u c e d g , e o n f i g u r a t i o n , T 1 / 2 . ZPAAD 304 269.

A 1361

D

82A101:

t3SBa

J

8ZGrt4:

83Gr15: 82Sh05:

R 78Bo41: 82Ch14:

t36pm

D

136Sm

D 82A107:

8~AI07:

=

136

RADIOACTIVITY 86,87,88,89Br,89,91,9~,93K r,B9,91,92,93,94Rh,93,94,s5SF,94,95,96 y,134S b,136,t37,138,139I, 137,138,139,14°,141Xe,138,139,14°,141,14gCs; measured average Eft. F i s s i o n p r o d u e t s , f l - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. NUCLEAR MOMENTS 135,137Ba; m e a s u r e d isotope shifts,hfs; deduced electric quadrupole moments. 137,136,135,134,13°Ba d e d u c e d c h a r g e r m s r a d i i c h a n g e r e l a t i v e to ~3SBa. H i g h resolution laser fluoresence spectroscopy. Self-consistent f i e l d c a l c u l a t i o n s . ZPAAD 306 195. NUCLEAR MOMENTS 135,13s,13?,138Ba; m e a s u r e d h f s . 135,13s,13?Ba d e d u c e d i s o t o p e s h i f t r e l a t i v e to 13SBa. H i g h r e s o l u t i o n l a s e r s p e c t r o s c o p y . ZPAAD 306 281. NUCLEAR MOMENTS 134,~35,13s,13?,13SBa; m e a s u r e d m u o n i c X - r a y s ; d e d u c e d c h a r g e d i s t r i b u t i o n s , isotope shifts. Droplet model,interacting boson approximation calculations. PYLBB 113 124. NUCLEAR REACTIONS 135,~37Ba(polarized n , 3 " ) , E = t h e r m a l ; m e a s u r e d 3' CP. 136,13eBa r e s o n a n c e s deduced JJr,3"-multipolarity. E n r i c h e d t a r g e t s , N a I ( T 1 ) d e t e c t o r s . PIFLD 8 93. NUCLEAR REACTIONS m?Ba(n,2n),E=14.4 MeV; m e a s u r e d p r o d u c t i o n a f o r *3SmBa. 13SBa d e d u c e d cr(isomer)/a(ground state). Activation technique,natural t a r g e t , a ° T m p b m o n i t o r . RRALA 51 391. R A D I O A C T I V I T Y 136Sm,145Dy [ - f r o m W , T a ( p , X ) , o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d E ( X - r a y ) , I(X-ray),ET,I%Ti/~. 136Pm [ - f r o m 136Sm d e c a y ] ; m e a s u r e d TI/2, 145Tb,i36pm d e d u c e d l e v e l s . High purity G e , l a r g e v o l u m e G e ( L i ) , S i - L i d e t e c t o r s . ZPAAD 305 185. RADIOACTIVITY 136Sm,*45Dy [ - f r o m W , T a ( p , X ) , o n - l i n e m a s s s e p a r a t i o n ' ] ; m e a s u r e d E ( X - r a y ) , I(X-ray),ET,13",Tl/e. 136pm [ f r o m 13eSm d e c a y ] ; m e a s u r e d T1/z. 145Tb,136pm d e d u c e d l e v e l s . High purity G e , l a r g e v o l u m e G e ( L i ) , S i - L i d e t e c t o r s . ZPAAD 305 185.

60

KEY

NUMBERS

A 13'71

13.TXe

137Ba

D 82A101:

D

J

82AI01

82Gr14

82Gr15 82Ri03 82Sh05

R 82Bu07

AND

=

KEYWORDS

137

R A D I O A C T I V I T Y •••87••••89B••89•9••92•93Kr••9•9••93•93•94Rb•93•94•95S••94•95•96Y,•34Sb•t36••3.7••38••39I• 137,138,139,14°,141Xe,138,139,14°,141,14ZCs; m e a s u r e d average Eft. F i s s i o n

products,f-strength

functions input,Si-Li detector system. N S E N A 80 7 4 . R A D I O A C T I V I T Y 86,8.7,88,89B F,89,91,Sa,93KF,89,91,92,93,94 R D,93,94,95SF,94,95,96

V,134Sb,136,i 37,138,1391,

137,138,139,14°,141Xe,138,139,14°,141,142Cs;

products,f-strength

measured

average

Eft.

Fission

f u n c t i o n s i n p u t , S i - L i d e t e c t o r s y s t e m . NSENA 8 0 74. NUCLEAR MOMENTS 135,137Ba; m e a s u r e d isotope s h i f t s , h f s ; deduced e l e c t r i c q u a d r u p o l e

moments.

13.7,136,135,134,13°Ba

deduced

resolution 195. NUCLEAR

laser

spectroscopy.

fluoresence

MOMENTS

135,136,i3.7,13SBa;

charge

radii

change

Self-consistent

rms

field

measured

hfs.

135,136,137Ba

relative

to

calculations.

deduced

isotope

138Ba. ZPAAD

shift

High 306

relative

t o 138Ba. H i g h r e s o l u t i o n laser spectroscopy. Z P A A D 3 0 6 281. N U C L E A R M O M E N T S 135,i3.7,13BBa; m e a s u r e d optical isotope shifts. Z P A A D 3 0 6 11. N U C L E A R MOMENTS ~34,135,136,137,138Ba; m e a s u r e d muonic X-rays; deduced charge distributions, isotope shifts. Droplet model,interacting boson approximation calculations. PYLBB I12

124. NUCLEAR

REACTIONS

i42~143~i44~145~i46~j4~15~Nd~4~Pr,i4~Ce~l99La~38Ba(~r~xnyp)~3~Pr/13aLa/1~.7Ba/ at rest; measured EV,I'/; deduced reaction mechanism. 134m,135mCS deduced isomer,J,~r,T1/2,cr(production) ratio. I37m,isSm,133m,131mBa,132mLa,13.TmCe, 13arnpr deduced isomer,Jjr, t33,131Ba deduced ff(isomer)/ff(ground state). NUPAB 382 501. RADIOACTIVITY 137raCe [from 137Ba(SHe,3n)]; measured Ev,I'y,7-f-coin. 137La deduced levels. NUPAB 376 i. NUCLEAR REACTIONS ~3aBa(p,2n),E=17.1-20.3 MeV; measured ET,17(E),Iv(0),I(ce),~/V-coin, pT(t). ~37La deduced levels,J,~r,Twa,ICC,B(X ). Enriched targets. NUPAB 376 I.

13SBa/laSBa/131Ba/135Cs/i34Cs/t35Xe/,E 137La

D

82Ko05

R 82Ko05 137Ce

D

8~Ko05

RADIOACTIVITY 137raCe NUPAB

R 82Bu07

376

[from

laTBa(3He,3n)]; measured

E%l%~7-eoin.

13.TLa d e d u c e d

levels.

1.

NUCLEAR REACTIONS ~ 4 z ~ 1 4 3 ~ 4 4 ~ 5 ~ I 4 6 ~ 4 8 ~ t 5 ~ N d ~ t 4 ~ r ~ 4 ~ C e ~ t 3 9 L a ~ i 3 ~ B a ( r r ~ x n y p ) ~ 3 8 ~ r / 1 3 e L a / ~ 7 B a / at rest; measured E%17; d e d u c e d reaction mechanism. isomer,J,rr,Tt/a,cr(produetion) ratio. 13~m,t35m,~33m,13~rnBa,t3amLa,13.TmCe,

135Ba/~33Ba/iSlBa/tSaCs/'34Cs/~35Xe/,E

i34m,laSmCs i3Bmpr

deduced

deduced

isomer,Jjr.

133,tSlBa

A 1381

D 82AI0t:

138Xe

D

13aCs

D 82AI01:

t38Ba

J

8~AIOI:

82Gr15: 82Ri03: 82Sh05:

R 78Bo41: 13SLa

D 81Sa42:

13apr

R 82Bu07:

D 81De38:

138pm

D 81De38:

cr(isomer)/cr(ground

state).

NUPAB

38£

501.

138

R A D I O A C T I V I T Y s6 , B7 , B0 , 89 B r . B9. 91 . . 9z 93 K r . s9. 91 . . 9a . 93 94 R b , 93 , 94 , 95 S r , 9¢ , 95 , 96 Y , 134 S b . 136 . .i37. 13a 139 I , 137 . 138 139 140 141 Xe . 138 139 140 141 142 Cs; m e a s u r e d . . . . . . . average Eft. F i s s i o n products,f-strength functions input,Si-Li detector system. N S E N A 80 7 4 . R A D I O A C T I V I T Y s6 87 88 89 B r . 89. .91. 92 93 K r . 89. 91 . . 92 . 93 94 R b , 93 , 94 , 95 S r , 94 , 95 , 96 Y , 134 S b . 136 . .137 . 138 139 I , 137 . 138 139 140 141 Xe . 138 139 140 141 142 Cs; m e a s u r e d . . . . . . . average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector system. N S E N A 80 7 4 . R A D I O A C T I V I T Y 86 , 87 , 88 , 89 B r . 89. .91. 92 93 K r . 89. 91 . . 92 . 93 94 R b , 93 , 94 , 95 S r , 94 , 95 , 96 Y , 134 S b . 136 . 137 . . 138 139 I , /37 . 138 139 140 141 X e . 138 139 140 141 142 Cs; m e a s u r e d . . . . . . . average Eft. F i s s i o n products,fl-strength functions input,Si-Li detector system. NSENA 80 74. N U C L E A R M O M E N T S 135,136,137,138Ba; m e a s u r e d h f s . 135,136,137Ba d e d u c e d isotope shift relative to laSBa. H i g h r e s o l u t i o n laser spectroscopy. Z P A A D 3 0 6 281. N U C L E A R M O M E N T S 135,137,13BBa; m e a s u r e d optical isotope shifts. Z P A A D 3 0 6 i1. N U C L E A R M O M E N T S 134,135,136,137,13SBa; m e a s u r e d muonic X-rays; deduced charge distributions, isotope shifts. Droplet model,interacting bosun approximation calculations. PYLBB i12 124. NUCLEAR REACTIONS la5,137Ba(polarized n,~/),E=thermal; measured 7 CP. 136,13SBa r e s o n a n c e s deduced J,Tr,~/-multipolarity, Enriched targets,NaI(T1) detectors. P I F L D 8 93. RADIOACTIVITY IaaLa(EC),(f-); measured TI/z,TI/2(EC)/TI/z(f). Gamma spectroscopy,different La c o m p o u n d s . RRALA 46 145. N U C L E A R R E A C T I O N S i4a~14~j44~i4~i~6~14~1~Nd~i4iPr~4~Ce~1~9La~1~Ba(~r-~nyp)i3~Pr/i~zLa/t~.7Ba/ 135 B a / 139 B a / 131B a / I35 C s / 134 C s / 135 X e / , E a t r e s t ; m e a s u r e d E7,17; d e d u c e d reaction mechanism. •

134m,135mCS d e d u c e d t3SNd

=

deduced

,

isomer,J,wr,T1/z,~(production

)

ratio.

13.Tm,135rn,133m,131mBa,132mLa,13.TmCe,

t38mpr deduced isomer,J,Tr. 133,t31Ba d e d u c e d a(isomer)/a(ground state). NUPAB 382 50t. R A D I O A C T I V I T Y 13SPin [ f r o m 1 4 a N d ( p , 5 n ) , E = 6 0 MeV; 1 4 4 S m ( p , 3 n a ) ] ; m e a s u r e d ET,I%I(ce),TT- , fV-coin; deduced Q ( E C ) , l o g f t . 13aNd d e d u c e d levels,ICC,J,Tr,v-branehing,v-muttipolarity. Z P A A D 3 0 3 151. R A D I O A C T I V I T Y 13SPin [ f r o m 1 4 ~ N d ( p , 5 n ) , E = 6 0 MeV; 1 4 4 S m ( p , 3 n a ) ] ; m e a s u r e d EV,IT,I(ce),77-, fT-coin; deduced Q ( E C ) , l o g f t . taSNd d e d u c e d levels,ICC,J,Tr,7-branching,v-multipolarity. Z P A A D 3 0 3 151.

61

KEY

A 13g I

D 82A101:

139Xe

D 82A101:

139Cs

D 82A101:

139La

J

~39pm

D 82De06:

139Sm

D 82De06:

82Ho02:

D 82A101:

=

KEYWORDS

139

R A D I O A C T I V I T Y 86,87,88,89Br,89,91,92,93Kr,89,91,92,93,94 R b,93,94,95Sr,94,95,g6y,134Sb,136,137,138,139I, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average YD. F i s s i o n products,fl-strength functions input,Si-Li detector s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 86,87,88,89Br,SS,g*,sa,93K r,Sg,ot ,s~,93,84R b,S3,s4,SSSr,94,95,96y,134Sb,t 36,137,138,t39I, 137,138,139,148,14tXe,138,J39,14°,141,14aCs; m e a s u r e d average ED. F i s s i o n products,fl-strength functions lnput,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 86,87,88,89Br,89,91,92,93Kr,89,91,9a,93,94 Rb,93,94,95Sr,94,95,96y,134Sb,136,137,138,139[, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average Eft. F i s s i o n products,fl-strength functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. NUCLEAR MOMENTS 139La; m e a s u r e d h f s c o n s t a n t s a,b. High r e s o l u t i o n s p e c t r o s c o p y , e o l l i n e a r l a s e r i o n b e a m s . Z P A A D 3 0 4 279. R A D I O A C T I V I T Y '39Sm [ f r o m *44Sm(p,5np),*~¢Sm(p,6n)139Eu(fl++EC)decay]; m e a s u r e d ET,17,I(ce), Efl+,flT-,77-eoin,T,/z; d e d u c e d Q(EC),log f t . *3SPin d e d u c e d l e v e l s , J , ~ r , I C C , 7 - m u l t i p o l a r i t y . Enriched targets,Ge(Li),Si(Li),intrinsic Ge d e t e c t o r s , m a g n e t i c spectrometers. P R V C A 25 504. R A D I O A C T I V I T Y 139Sin [ f r o m ~44Sm(p,5np),t44Sm(p,6n)i38Eu(fl++EC)decay3; m e a s u r e d gT,IT,I(ce), Efl+,flT-,77-coin,T,/a; d e d u c e d Q(EC),log f t . 139Pro d e d u c e d l e v e l s , J j r , I C C , 7 - m u l t i p o l a r i t y . Enriched targets,Ge(Li),Si(Li),intrinsic Ge d e t e c t o r s , m a g n e t i c spectrometers. PRVCA 25 504.

A 14OXe

AND

NUMBERS

=

140

RADIOACTIVITY 86,87,88,89Br,89,91,g2,93KF,89,91,92,93,94R b,93,94,O5SF,94,95,g6y,134Sb,136,137,138,139I, 137,138,139,140,141Xe,I38,I39,t40,141,142Cs; m e a s u r e d average functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74.

14OCs

D 82A101:

14OBa

D 82Ad02:

14OLa

D 82Ad02:

82Mi03: R 82A121:

82Ve07:

14OCe

D 82Ad02:

82Mi03: R 82Ce01: 82Dj04:

82Na06:

~4Opr

D 82Ad02:

14ONd

D 8~Ad02:

Eft.

Fission

products,fl-strength

RADIOACTIVITY 86,87,88,89Br,89,91,Q2,93Kr,89,91,92,93,94R b,93,94,95Sr,Q4,Qs,96y,134Sb,136,137,138,1391, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; m e a s u r e d average Eft. F i s s i o n products,fl-strength

functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 14°Ba; m e a s u r e d E T , I T , I ( c e ) , c e 7 - c o i n , 7 7 ( O ) ; d e d u c e d log ft,Ifl. 14°La d e d u c e d levels,T,/2,configuration,7-branehing. 14eLa [ f r o m 14°Ba d e c a y ] ; m e a s u r e d E?,I?,T7-coin, 7 7 ( 0 ) ; 14°Pr [ f r o m 14°Nd d e c a y ] ; m e a s u r e d E7,I?,E(X-ray),I(X-ray); deduced log ft,Ifl. 14°Nd; m e a s u r e d E(K X - r a y ) , l ( K X - r a y ) . 14°Ce d e d u c e d l e v e l s , T - b r a n c h i n g , J J r . IANFA 46 2. R A D I O A C T I V I T Y 14°Ba; m e a s u r e d E T , I T , I ( c e ) , c e T - c o i n , T 7 ( O ) ; d e d u c e d log ft,Ifl. 14°La d e d u c e d levels,T1/a,configuration,7-branching. 14°La [ f r o m '4°Ba decay]; measured ET,I7,77-coin, 77(0); '4°pr [from 14ONd d e c a y ] ; m e a s u r e d E7,IT,E(X-ray),I(X-ray); deduced log f t , I f l . 14°Nd; m e a s u r e d E(K X - r a y ) , I ( K X - r a y ) . t4OCe d e d u c e d l e v e l s , 7 - b r a n c h i n g , J , T r . IANFA 46 2. RADIOACTIVITY i4°La; m e a s u r e d 7 7 ( 0 ) . 14aCe d e d u c e d J,~r,6. J P H G B 8 581. NUCLEAR REACTIONS 1 3 9 L a ( p o l a r i z e d n , X ) , E = 0 . 7 5 eV; m e a s u r e d transmission; . A v e r a g e a-width a n a l y s i s . CZYPA 32 117. NUCLEAR REACTIONS 51v,5S,6°,6ZNi,6aZn,9°,92,9%96Zr,92,94,96,ss,i°°Mo,iZ°,124Sn,14°Ce(p,p'),E=200 MeV; m e a s u r e d (7(0). 51V,58,6°,6aNi,68Zn,9°,92,94,96Zr,9a,94,sa,98,1°°Mo,la°,la4Sn,14°Ce d e d u c e d resonances,F,T,Ml character. N U P A B 388 1. NUCLEAR REACTIONS 68Zn,9°,sa,94Zr,94,9~,se,l°OMo,t24Te,t38Ba,14aCe,146Nd,iS°Sm,Z32Th(p,t),E=52 MeV; m e a s u r e d ~;(Et,0). 6%n,9°,9ZZr,9a,9%96Mo,14°Ce,144Nd,14aSm,238Th d e d u c e d d e e p t w o - h o l e states. Enriched t a r g e t s . N U P A B 376 513. R A D I O A C T I V I T Y 14OBa; m e a s u r e d E 7 , I T , I ( c e ) , e e T - e o i n , 7 7 ( 0 ) ; d e d u c e d log ft,Ifl. ~4°La d e d u c e d levels,Tj/a,configuration,7-branching. 14°La [ f r o m 14°Ba d e c a y ] ; m e a s u r e d [7,17,77-coin, 77(0); 14°pr [from 14°Nd d e c a y ] ; m e a s u r e d ET,17,E(X-ray),l(X-ray); deduced log f t , I f l . 14°Nd; m e a s u r e d E(K X ~ r a y ) , I ( K X - r a y ) . ~4°Ce d e d u c e d l e v e l s , 7 - b r a n c h i n g , J j r . IANFA 4 6 2. R A D I O A C T I V I T Y 14°Ba; m e a s u r e d E T , l T , I ( c e ) , c e T - c o i n , T T ( 0 ) ; d e d u c e d log ft,Ifl. ~4°La d e d u c e d levels,T1/a,configuration,7-branching. 14°La [ f r o m 14OBa d e c a y ] ; m e a s u r e d ET,]7,77-coin, 77(0); ~4°pr [from 14°Nd decay]; m e a s u r e d ET,I7,E(X-ray),I(X-ray); d e d u c e d log f t , I f l . 148Nd; m e a s u r e d E(K X - r a y ) , I ( K X - r a y ) . 14°Ce d e d u c e d l e v e l s , 7 - b r a n c h i n g , J j r . IANFA 46 2.

62

KEY

NUMBERS

AND

A 141Xe

D 82A101

14iCs

D 82A101

82Ya04

~4~Ba

D 82Ya04

14iCe 141pr

D 82Gu01 J 83Ma31

D 82A101

14ZLa

D 82Mi01

t42Ce

D 82Mi01

14Zpr

R 82A103

D 82Ge03

143pr

D 82Ge03

14aNd

R 821s05

D 82Ch22

144La

D 82Ch22

82Mi01: 144Ce

D 81Yu02: 82Mi01:

144pr

D 81Yu02:

t44Nd

R 82Is05:

82Na06:

142

=

143

R A D I O A C T I V I T Y ~43Ce [ f r o m n e u t r o n i r r a d i a t i o n of 142Ce]; m e a s u r e d f l 7 - c o i n , E v , 1 7 . 143pF levels deduced 7-emission probabilities,relative I7. I J A R A 33 355. RADIOACTIVITY 14ace [ f r o m n e u t r o n i r r a d i a t i o n of 14aCeS; m e a s u r e d flV-coin,Ev,17. ~43Pr levels deduced v-emission probabilities,relative 17. I J A R A 33 355. NUCLEAR REACTIONS 14a,143,145Nd,155,157Gd,*m,isa,164Dy,lSaHo,174,173yb(n,7),E=thermal; m e a s u r e d EV. t43,144,146Nd,tSs,158Gd,lS2,163,164,165Dy,le6Ho,175,174yb d e d u c e d n e u t r o n separation energy. PRVCA 35 3184.

A t44Ba

=

RADIOACTIVITY 8~7~88~89B~89~9~2~93Kr~8~9~9~9:3~94Rb~9~94~95Sr~94~5~96Y~134~b~136~7~i~8~39~ 137,138,139,t40,141Xe,138,139,140,14t,142Cs; measured average EB. F i s s i o n p r o d u c t s , B - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y i4a,144La [ f r o m f i s s i o n p r o d u c t Cs d e c a y ] ; m e a s u r e d E7,Iv,77(O),oriented nuclei,77-eoin; d e d u c e d Qfl. 14a,144Ce d e d u c e d l e v e l s , J j r , d . Ge(Li) d e t e c t o r s . JPHGB 8 l l l . R A D I O A C T I V I T Y 14z,144La [ f r o m f i s s i o n p r o d u c t Cs d e c a y S ; m e a s u r e d E v , I v , 7 7 ( 0 ) , o r i e n t e d nuclei,77-coin; d e d u c e d Qfl. 142,144Ce d e d u c e d l e v e l s , J j r , d . Oe(Li) d e t e c t o r s , JPHGB 8 111. NUCLEAR REACTIONS ~4'pr,tSaTb,165Ho,le7Er,169Tm(polarized n,X),E=0.001-100 keV; m e a s u r e d transmission; d e d u c e d (~ s p i n d e p e n d e n c e , s t r e n g t h f u n c t i o n s . 14aPr,16°Tb,~66Ho,t68Er?65Tm r e s o n a n c e s d e d u c e d J. P o l a r i z e d n a t u r a l targets,liquid scintillation d e t e c t o r . NUPAB 376 229.

A t43Ce

141

R A D I O A C T I V I T Y 86,87,88,89Br,eS,91,92,SaKr,89,91,92,93,94R b,93,94,95Sr,94,95,96y,134Sb,136,137,138,i39I, 137,la8,139,14°,141Xe,la8,139,146,141,142Cs; measured average Eft. F i s s i o n p r o d u c t s , B - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y 86,87,88,89Br,e9,91,9a,93KF,89,91,92,93,a4Rb,ga,94,95SF,94,95,96y,I34sb,la6,137138,139I, 137,138,139,14°,141Xe,138,139,14°,141,142Cs; measured average Eft. F i s s i o n p r o d u c t s , B - s t r e n g t h functions input,Si-Li d e t e c t o r s y s t e m . NSENA 80 74. R A D I O A C T I V I T Y ~4~Cs [ f r o m a S S U ( n , F ) , E = t h e r m a l S ; m e a s u r e d E v , 1 7 , 7 7 - c o i n , 7 7 ( t ) , E ( X - r a y ) , l(X-ray); deduced log f t . ~4~Ba d e d u c e d levels,J,w,ICC,fl-branching,d(E2/Ml). M a s s separated source, ttyperpure Ge,Ge(Li) d e t e c t o r s . PRVCA 26 1215. R A D I O A C T I V I T Y '¢~Cs [ f r o m a a 5 U ( n , F ) , E = t h e r m a l S ; m e a s u r e d E 7 , I 7 , 7 7 - c o i n , 7 7 ( t ) , E ( X - r a y ) , l(X-ray); deduced log f t . ~4~Ba d e d u c e d levels,J,vr,ICC,fl-branching,d(E2/Ml). M a s s separated source. Hyperpure Ge,Ge(Li) d e t e c t o r s . PRVCA E6 1215. R A D I O A C T I V I T Y ~4~Ce; m e a s u r e d IB f o l l o w i n g B - d e c a y . Magnetic d e f l e c t i o n . NUPAB 376 478. NUCLEAR MOMENTS ~4~pr; m e a s u r e d /x. Electronic IDa e x c i t a t i o n , d i r e c t m e a s u r e m e n t . PRLTA 49 636.

A ~4~Cs

=

KEYWORDS

=

i44

RADIOACTIVITY 144Ba [ f r o m Z a S U ( n , F ) , E = t h e r m a l S ; m e a s u r e d E v , I 7 , 7 7 - c o i n , 7 7 ( 0 ) , T 1 / a , 7 7 ( t ) , 7(t),I(K X-ray)/17; deduced log ft,Ifl. 144La d e d u c e d levels,J,rr,d,ICC. H y p e r p u r e Ge, Ge(Li) d e t e c t o r s , l o w e n e r g y p h o t o n s p e c t r o m e t e r . Mass s e p a r a t e d s o u r c e . PRVCA 26 1198. R A D I O A C T I V I T Y 144Ba [ f r o m a 3 a U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d E7,Iv,77-eoin,77(O),T1/e,77(t), 7(t),I(K X-ray)/I7; deduced log ft,Ifl, i44La d e d u c e d levels,Jjr,&ICC. Hyperpure Ge, Ge(Li) d e t e c t o r s , l o w e n e r g y p h o t o n s p e c t r o m e t e r . Mass s e p a r a t e d s o u r c e . PRVCA 26 1198. RADIOACTIVITY 14z,144La [ f r o m f i s s i o n p r o d u c t Cs d e c a y ] ; m e a s u r e d Ev,Iv,77(O),oriented nuclei,77-eoin; d e d u c e d Qfl. 14~,144Ce d e d u c e d l e v e l s , J j r , d . Ge(Li) d e t e c t o r s . JPHGB 8 111. RADIOACTIVITY 144Ce; m e a s u r e d E7,I7,E(X ray); deduced Ifl. ~44Pr l e v e l s d e d u c e d 7-branching. YTHLD 3 312. R A D I O A C T I V I T Y 142,144La [ f r o m f i s s i o n p r o d u c t Cs d e c a y S ; m e a s u r e d E7,I%vv(O),oriented nuelei,77-eoin; d e d u c e d Qfl. 142,144Ce d e d u c e d levels,J,~r,6. Ge(Li) d e t e c t o r s . JPHGB 8 111. R A D I O A C T I V I T Y 144Ce; m e a s u r e d Ev,I7,E(X-ray); deduced Ifl. 144pr l e v e l s d e d u c e d -/-branching. YTHLD 3 312. NUCLEAR REACTIONS 14e,143,145Nd,155,157Gd,161,16a,164Dy,165Ho,174,173yb(n,7),E=thermal;m e a s u r e d EV. 143,I44,146Nd,I56,158Gd,I62,I63,164,165Dy,t66Ho,175,I74yb d e d u c e d n e u t r o n s e p a r a t i o n e n e r g y . PRVCA 25 3184. NUCLEAR REACTIONS 68Zn,9°,sa,94Zr,94,96,98,l°°Mo,124Te,138Ba,14eCe,14~Nd,15°Sm,~3aTh(p,t),E=52 MeV; m e a s u r e d (7(Et,0). 6BZn,9°,SaZr,SZ,94,SdMo,t4°Ce,t44Nd,148Sm,23°Th d e d u c e d d e e p t w o - h o l e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513.

63

KEY

NUMBERS

A

144Sm

R 82C101:

82GaO2:

82Sa19:

82Ta17: 82YaO2:

144Gd

D 82No08:

R 82Ha22:

144Tb

D 82No08:

82So02:

D 82Ra13:

145Ba

D 82Ra13:

145Nd

R 82Ar13:

145Sm

D 82De26:

145Eu

D 82De26:

82Fi01

R 82Ga12

145Gd

D 81A123 82FiOl

82No08

82So02

=

144

KEYWORDS

continued

NUCLEAR REACTIONS 16,180,~4Mg,28Si,32S,SSAr,4°Ca,54Cr,144,152,154Sm,2°spb,232Th(polarized d,d), ( p o l a r i z e d d , d ' ) , E = 1 8 - 2 3 MeV; m e a s u r e d a(O),iTll(O ). ls,180,24M~,2Ssi,SaS,3°Ar,4OCa,S4Cr,144, lsz,154Sm,a°sPb,a3aTh l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o e t u p o l e t r a n s i t i o n s t r e n g t h . 154 152,144Sm,23aTh d e d u c e d neutron,proton deformation d i f f e r e n c e s . , Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082. NUCLEAR REACTIONS 9°Zr,~a°Sn,144Sm,Z°spb(p,p'),E=800 MeV; m e a s u r e d a(O). ~°Zr,~a°Sn,144Sm, Z°"pb,4°Ca,SSNi d e d u c e d d e f o r m a t i o n l e n g t h s , n e u t r o n , p r o t o n m a t r i x e l e m e n t r a t i o s . O p t i c a l m o d e l , D W B A a n a l y s e s . PRVCA 25 408. NUCLEAR REACTIONS 1~4Mg~sSi~4~Ar~4~4~4sCa~4~4s~T~54~sFe~58~s~a~s4Ni~8~Y~Z~1~M~ 144Sm,ZO8pb,aO~Bi(polarized p,p),E=65 MeV; m e a s u r e d a(0),A(0); d e d u c e d o p t i c a l m o d e l parameters. 160,~4 Mg,28Si,4°A r,4°,44,48Ca,46,48,5°Ti,S4,56Fe,58,s°,62,64 Ni,89Y,S°Zr,SS,l°°Mo,144Sm, 2°spb,a°sBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 9 4 4 . NUCLEAR REACTIONS I44,~56,15aSm(p,p),(p,p'),E=l.04 GeV; m e a s u r e d c~(0). 144Sm l e v e l s d e d u c e d t r a n s i t i o n s t r e n g t h s . M i c r o s c o p i c a n a l y s i s . E n r i c h e d t a r g e t s . NUPAB 386 552. NUCLEAR REACTIONS 1 4 4 S m ( a , a ' ) , E = 8 3 . 8 , 9 9 . 1 , 1 0 8 . 6 MeV; a ° s p b ( a , a ' ) , E = 8 3 . 8 , 8 9 , 1 1 8 . 7 MeV; m e a s u r e d a(0,E). 144Sm,a°aPb d e d u c e d g i a n t m o n o p o l e , q u a d r u p o l e r e s o n a n c e s , P , d e f o r m a t i o n parameters fl(L). Dipole p l u s t r i p l e t q u a d r u p o l e magnetic detection system,enriched t a r g e t . DWBA a n a l y s i s . NUPAB 381 277. RADIOACTIVITY 144,145,146Tb,l~'S,146Dy,147,148,15°Ho,148,15°Er,148,15°Tm [ f r o m 9°,91,~aZr,~SNb,°Z, ~4Mo(SSNi,xnyp),E=233-250 MeV]; m e a s u r e d "y'y-coin,EC/fl+,Ey,I%fl-decay Tl/~; d e d u c e d log ft, Ifl. ~5°Er d e d u c e d Q(EC). 144 ,45,~46Gd,147,~4e,150Dy,146Tb,148,,50Ho deduced levels,-~-branching. ZPAAD 306 223. NUCLEAR REACTIONS la°,1~4Sn(~SSi,xn),E=108-144 MeV; measured 17(0,H,t) vs T. 144,147,'4SGd levels deduced quadrupole moment,tentative J,deformation. Pulsed beam,Ge(Li) detectors, recoil implantation into Gd. NUPAB 379 ~87. RADIOACTIVITY 144,145,14~Tb,145,~4SDy,14v,148,~5°Ho,~48,15°Er,14s,15°Tm [from 9°,91,92Zr,93Nb,9~, 94Mo(SeNi,xnyp),E=233-250 MeV]; measured ~-coin,EC/fl+,Ey,l%fl-decay T1/a; deduced log ft, lfi. 15°Er deduced Q(EC). 144,145,146Gd,147,148,159Dy,14STb,148,15aHo deduced levels,y-branching. ZPAAD 306 223. RADIOACTIVITY 144,145Tb [from ~44Sm(I°B,X),E=96,125 MeV]; measured E%I%T1/~,7~-coin. '45Gd d e d u c e d ]evels,J,~. PRVCA 25 1Ol2.

A 145Cs

AND

=

145

RADIOACTIVITY 145Cs [ f r o m 2 3 5 U ( n , F ) , E = t h e r m a l , o n - l i n e s e p a r a t i o n ] ; m e a s u r e d E%I%I(ce) f o l l o w i n g g - d e c a y ; d e d u c e d log ft,Ifl. 145Ba d e d u c e d l e v e l s , 7 - m u l t i p o l a r i t y , p o s s i b l e J,Tr. ZPAAD 305 359. RADIOACTIVITY 145Cs [ f r o m 2 3 5 U ( n , F ) , E = t h e r m a l , o n - l i n e s e p a r a t i o n ] ; m e a s u r e d E%I%I(ce) f o l l o w i n g g - d e c a y ; d e d u c e d log ft,Ifl. 14SBa d e d u c e d l e v e l s , y - m u l t i p o l a r i t y , p o s s i b l e J,~r. ZPAAD 305 359. NUCLEAR REACTIONS 14°Nd(polarized d,t),E=16 MeV; m e a s u r e d a ( E t ) , a ( 0 ) , a n a l y z i n g p o w e r v s (0). 14SNd l e v e l s d e d u c e d J j r . DWBA a n a l y s i s . CJPHA 69 1534. RADIOACTIVITY 145Eu(EC),(fl+); m e a s u r e d 7 ( 0 ) , o r i e n t e d n u c l e i in Fe. 145Sm levels d e d u c e d J, 7r,6(E2/M1),6(M2/E1). Ge(Li) d e t e c t o r s , 3 H e - 4 H e d i l u t i o n refrigerator. Quasiparticle plus p h o n o n c a l c u l a t i o n s . IANFA 46 860. RADIOACTIVITY 145Eu(EC),(fl+); m e a s u r e d 7 ( 0 ) , o r i e n t e d n u c l e i in Fe. 14SSm levels d e d u c e d J, w,6(E2/M1),(~(M2/E1). Ge(Li) d e t e c t o r s , S H e - 4 H e d i l u t i o n r e f r i g e r a t o r . Q u a s i p a r t i c l e p l u s p h o n o n c a l c u l a t i o n s . IANFA 46 860. RADIOACTIVITY '4SGd [ f r o m 144Sm(SHe,2n),E=20 MeV; '44Sm(a,3n),E=42 MeV]; m e a s u r e d Ey,I%Efl, Q,T,/2,Ty-,fl~/-,(X-ray)y-coin; d e d u c e d ~/fl+ r a t i o s , l o g f t , f l - s t r e n g t h function,missing continuum d e c a y i n t e n s i t y . 145Eu d e d u c e d l e v e l s , J , w . PRVCA 25 527. NUCLEAR REACTIONS 144Sm(a,t),E=80 MeV; 144Sm(3He,d),E=240 MeV; m e a s u r e d a(0),a(Et),a(Ed). 14SEu d e d u c e d broad structures,P,L,J,Tr,C2S,hs/a,ij3/2 proton strength distribution. Z e r o - r a n g e DWBA a n a l y s i s . PRLTA 48 1593. RADIOACTIVITY 145Tb,146Dy [ f r o m m a s s s e p a r a t o r ] ; m e a s u r e d Ey,ly,TI/2. 145Gd d e d u c e d levels, J , T r , y - b r a n c h i n g . 146Tb deduced Tl/a. IANFA 45 1827. RADIOACTIVITY 14SGd [ f r o m 144Sm(3He,2n),E=20 MeV; 144Sm(a,3n),E=42 MeV]; m e a s u r e d E%Iy,Efl, Q,Tl/a,yT-,fly-,(X-ray)y-coin; d e d u c e d z/fl + r a t i o s , l o g f t , f l - s t r e n g t h function,missing continuum d e c a y i n t e n s i t y . 145Eu d e d u c e d l e v e l s , J d r . PRVCA 25 527. RADIOACTIVITY 144,145,146Tb,145,146Dy,147,14s,15°Ho,14s,lS°Er,148,150Tm [ f r o m 9°,91,92Zr,gaNb,g2, 94Mo(SSNi,xnyp),E=233-250 MeV3; measured yy-coin,EC/fl+,Ey,lY,fl-decay Tl/u; deduced log ft, Ifl. IS°Er deduced Q(EC). 144,145,14SGd,147,148,15°Dy,146Tb,14s,lS°Ho deduced levels,~/-branching. ZPAAD 306 223. RADIOACTIVITY 144,145Tb [from 144Sm(mB,X),E=96,125 MeV]; measured Ey,ly,Ti/2,yy-coin. 145Gd deduced levels,Jflr. PRVCA 25 1012.

64

KEY

NUMBERS

A 145Gd

R 82Pa04:

~45Tb

D 81A123: 82A107:

82No08:

8~8o02: 145Dy

D

82A107:

82No08:

R 821s05:

146Sm

R BERo05:

~46Gd

O 82No08:

R 82Ka22:

14~Tb

D 81A123: 82No08:

~46Dy

D

B1AI23: 82Gu07:

82No08:

R 82Gu07:

14~Ho

D 82Gu07:

D 80Ch38: 82Sa09:

145

continued

=

146

NUCLEAR REACTIONS 142,143,145Nd,155,157Gd,161,1sa,164Dy,165Ho,174,i73yb(n,y),E=thermal; m e a s u r e d EY. 143,t44,146Nd,156,15SGd,16e,163 164,165Dy,J66Ho,175,174yb deduced n e u t r o n separation energy. PRVCA 25 3184. NUCLEAR REACTIONS mgLa(UB,4n),E=54 MeV; measured Ey,ly,recoi]. 1~6Srn levels deduced TI/2, B(E2). Ge(Li) detectors,plunger technique. Cluster v i b r a t o r , i n t e r a c t i n g boson models. PRVCA 25 3000. R A D I O A C T I V I T Y t44 145 146Tb 145 14eDy 147 148 150HO 148 150Er t48 tSOTm [ f r o m 90 gl ~ZZr 9aNb 9z 94Mo(SeNi,xnyp),E=233-250 MeV]; m e a s u r e d 7 7 - c o i n , E C / f l + , E y I v f l - d e c a y T1/2; d e d u c e d log f t , IS. 15°Er d e d u c e d Q(EC). 144,145,146Gd,147,148,~5°Dy,146Tb,14s,15°Ho d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223. NUCLEAR REACTIONS 1 4 4 S r n ( 3 H e , n ) , E = 1 5 . 3 MeV; 6 2 N i , 9 2 Z r ( p , p ' ) , E ~ 7 . 0 8 MeV; m e a s u r e d I(ce), ( e e ) ( t ) . i46Gd,o2Zr l e v e l d e d u c e d T1/2. C e n t r o i d timing method,magnetic plus Si-Li combination electron spectrometer,composite Ni,Zr t a r g e t . NUIMA 200 253. R A D I O A C T I V I T Y 145Tb,J46Dy [ f r o m m a s s s e p a r a t o r ] ; m e a s u r e d Ey,Iy,TI/2. 145Gd d e d u c e d levels, Jflr,y-branehing. ~46Tb d e d u c e d TI/2. IANFA 4 5 1827. R A D I O A C T I V I T Y 144 145 146Tb 145 146Dy 147 148 150Ho 148 15OEr 148 15OTm [ f r o m 90 91 92Zr 93Nb 92 9 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d 7y-coin,EC/fl+,E%Ivfl-decay T1/2; d e d u c e d log f t IS. iS°Er d e d u c e d Q(EC). 144 145,146Gd 147 148,15ODy,l~6Tb,148,15OHo d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223. R A D I O A C T I V I T Y 145Tb,~46Dy [ f r o m m a s s s e p a r a t o r S ; m e a s u r e d E%I%T1/2. 145Gd d e d u c e d levels, J,rr,y-branehing. ~46Tb d e d u c e d T~/2. I A N F A 45 1827. R A D I O A C T I V I T Y 146H0 [ f r o m g°Zr(58Ni,np),E=250 MeV]; m e a s u r e d S - d e c a y T~/2; d e d u c e d Q(EC), log f t . 146Dy d e d u c e d levels,y-branching,IS. Z P A A D 305 297. R A D I O A C T I V I T Y 144 145 146Tb 145 146Dy ~47 14~ 150H0 148 150Er 14s 150Tin [ f r o m 90 gi 92Zr 93Nb 92 9 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d yy-eoin,EC/fl+,Ev,lyfl-decay Tt/2; d e d u c e d log f t Ifl. 15°Er d e d u c e d Q(EC). 144 145146Gd1471¢s,tSODy,14OTb,t4slSOHo d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223. NUCLEAR REACTIONS 9°,mZr(5~Ni,xnypza)14SHo/~4~Dy/145Dy/i45Tb/~44Tb/14aTb/~42Tb/~44Gd/~4aGd/, E = 2 3 3 , 2 5 0 MeV; m e a s u r e d Ey,Iv,~(Ev),Vy-,v(ce)-coin; d e d u c e d r e l a t i v e y i e l d s f o r 14SHo,~4s ~4SDy,~45,~44,14a,~4~Tb,~4%~aaGd. t4SDy d e d u c e d levels,ICC,y-branching,y-multipolarity,isome; J,~r,T~/2,B(), ). Z P A A D 305 297. R A D I O A C T I V I T Y 14Silo [ f r o m O°Zr(SSNi,np),E=250 MeV]; m e a s u r e d S - d e c a y T~/e; d e d u c e d Q(EC), log f t . ~4SDy d e d u c e d l e v e l s , 7 - b r a n c h i n g , l f l . Z P A A D 305 297.

A 147Nd

=

KEYWORDS

NUCLEAR REACTIONS 1 4 4 S m ( a H e , ~ n ) , E = 1 2 . 6 - g 7 MeV; m e a s u r e d Ev,Iy(E),iy(0),I(ce),yy-coin, 3He2e(t). *45Gd d e d u c e d l e v e l s , J , w , T l / 2 , I C C , B ( ) , ). E n r i c h e d t a r g e t s . NUPAB 373 237. R A D I O A C T I V I T Y 145Tb,146Dy [ f r o m m a s s s e p a r a t o r S ; m e a s u r e d Ey,IT,T~/e. 145Gd d e d u c e d levels, J,rr,y-branehing. 14STb d e d u c e d T~/2. I A N F A 45 1827. R A D I O A C T I V I T Y ~3~Sm,~45Dy [ f r o m W , T a ( p , X ) , o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d E ( X - r a y ) , I(X-ray),Ey,IT,T1/2. ta~pm [from ~36Sm d e c a y ] ; m e a s u r e d TI/2. 145Tb,~a6Pm d e d u c e d l e v e l s . High purity Ge,large volume C e ( L i ) , S i - L i d e t e c t o r s . Z P A A D 305 185. R A D I O A C T I V I T Y 144,~45,146Tb,~4~,14~Dy,147,~48,15°Ho,14s,~50Er,l~a,~SOTm [ f r o m 9°,gl,gaZr,93Nb,92, ~ 4 M o ( 5 ~ N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d yy-coin,EC/fl+,Ey,Iy,fl-decay Ti/2; d e d u c e d log f t , IS. 15°Er d e d u c e d Q(EC). 144,~45,t46Gd,~47,148,~5°Dy,*46Tb,148,~5°Ho d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223. R A D I O A C T I V I T Y 144,~45Tb [ f r o m ~44Sm(I~B,X),E=96,125 MeV]; m e a s u r e d E y , I y , T l / 2 , y y - c o i n . i45Gd deduced l e v e l s , J , r r . P R V C A 25 1012. R A D I O A C T I V I T Y laSsm,~45Dy [ f r o m W , T a ( p , X ) , o n - l i n e m a s s s e p a r a t i o n S ; m e a s u r e d E ( X - r a y ) , I(X-ray),Ey,ly,Ti/a. *a6pm 5from laSsm decayS; measured TI/2. 145Tb,~a~Pm d e d u c e d l e v e l s . High purity Ge,large volume G e ( L i ) , S i - L i d e t e c t o r s . Z P A A D 305 185. R A D I O A C T I V I T Y i44,145,14STb,145,146Dy,147,148,15°Ho,148,~5OEr,14s,t5OTm [ f r o m 9°,9~,geZr,9aNb, 92, ~ 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d 7y-coin,EC/fl+,Ev,I.y,fl-decay T1/a; d e d u c e d log f t , IS. ~5°Er d e d u c e d Q(EC). ~44,145,14~Gd,147,~48,15°Dy,146Tb,~4~,'S°Ho d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223.

A ~46Nd

AND

=

147

R A D I O A C T I V I T Y 147Nd; m e a s u r e d EV,Iv. 147prn d e d u c e d levels,v-branching. Ge(Li) spectrometers. YTHLD 2 382. R A D I O A C T I V I T Y '47Nd; m e a s u r e d y v - e o i n , v v ( t ) , v V ( 0 ) , o r i e n t e d n u c l e i . 147Pm d e d u c e d levels,T1/ 2,J,~r,6,B()~),M1 hindrance,E3 enhancement factors,v-branching. Sum coincidence spectrometer. NCIAA 67 267.

65

KEY

NUMBERS

AND

A =

147Nd

R 82Ja09:

147pm

D 80Ch38: 82Sa09:

147Sm

D 82De27:

147Eu

D 82De27:

147Gd

D 82K104:

R 82Ba46:

82Rr13: 82Ha22:

147Tb 147Dy

D D

82ToOl: 82No08:

147Ho

D

82No08:

82To01:

R 82No07:

D 82K103:

2it.

R A D I O A C T I V I T Y 147Tm [ f r o m 92Mo(SSNi,2np)]; measured direct proton decay Tl/a,Ep,lp, fl-delayed Ep,lp,Tl/~ lower limit. E-hE detector anticoincidence,sum spectra,evaporation residue mass separation. Z P A A D 305 125.

A 14aNd

b 82Be20:

t4SSm

R 82Do06

82Na06

148Gd

R 82Ha22

148Tb

D 81Sc21

148Dy

D 81Sc21

continued

NUCLEAR REACTIONS 1 4 S N d ( d , p ) , 1 4 S N d ( d , t ) , E = 1 2 . 1 MeV; m e a s u r e d a(Ep),a(Et),a(0). 147Nd deduced levels,L,Jjr,speetroscopic factors.Magnetic spectrograph. DWBA a n a l y s i s . APOBB 13 63. R A D I O A C T I V I T Y t47Nd; m e a s u r e d ET,I~. 1 4 7 p m d e d u c e d levels,y-branching. Ge(Li) spectrometers. YTHLD 2 382. R A D I O A C T I V I T Y 147Nd; m e a s u r e d - / ~ - c o i n , y T ( t ) , ~ 7 ( 0 ) , o r i e n t e d n u c l e i . 147pm d e d u c e d levels,T1/ 2,J,Tr,6,B(X),M1 hindrance,E2 enhancement factors,7-branching. Sum coincidence spectrometer. NCIAA 67 267. R A D I O A C T I V I T Y 147Eu(EC),(fl+) [ - f r o m Ta(p,X),E=660 MeV]; m e a s u r e d y ( 0 ) , o r i e n t e d n u c l e i i n Fe,Gd; d e d u c e d #. t47Sm levels deduced J,zr,~(E2/M1),6(M2/E1). Ge(Li) d e t e c t o r , a H e - 4 H e dilution refrigerator. Quasiparticle plus phonon m o d e l . I A N F A 46 867. R A D I O A C T I V I T Y 147Eu(EC),(fl +) [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d y ( 0 ) , o r i e n t e d n u c l e i i n Fe,Gd; d e d u c e d Iz. 147Sm l e v e l s d e d u c e d J , T r , 6 ( E 2 / M 1 ) , 6 ( M 2 / E 1 ) . Ge(Li) d e t e c t o r , 3 H e - 4 H e dilution refrigerator. Quasiparticle plus phonon m o d e l . I A N F A 46 867. R A D I O A C T I V I T Y 147Gd [ f r o m 1 4 7 S m ( 3 H e , 3 n ) , E = 2 2 , 2 7 MeV3; m e a s u r e d I(ce),ce(t). 147Gd l e v e l deduced Tl/a,y-branching ratio,B(E3),configuration. Si-Li,magnetic lens spectrometers. P R L T A 48 1457. NUCLEAR REACTIONS 135Ra(160,4n),E=77-84 MeV; m4Sn(2SSi,5n),E=128-140 MeV; m e a s u r e d y ~ - c o i n , IT(0),I(ce). 147Gd d e d u c e d levels,J,Tr,isomer Ta/2,reduced transition probabilities. Pulsed beam,Ge(Li),Si(Li) detectors,NaI(Tl) array,mini-orange spectrometer. N U P A B 389 93. NUCLEAR REACTIONS 14OCe(12C,Sn),E=96 MeV; 1 4 8 S m ( a , 5 n ) , E = 7 6 MeV; m e a s u r e d E ' y , I y , T y - c o i n , "y(0). 147Gd d e d u c e d i s o m e r d e c a y , l e v e l s , J , ~ , ' y - b r a n c h i n g , c o n f i g u r a t i o n . Z P A A D 305 281. NUCLEAR REACTIONS 12°,le4Sn(~SSi,xn),E=108-144 MeV; m e a s u r e d IT(0,H,t) v s T. 144,147,148Gd levels deduced quadrupole moment,tentative J,deformation. Pulsed beam,Ge(Li) detectors, recoil implantation i n t o Gd. N U P A B 379 287. R A D I O A C T I V I T Y 147Dy; m e a s u r e d E T , I T , 7 7 - c o i n . 147Tb d e d u c e d l e v e l s , J , ~ . PRVCA 25 667. R A D I O A C T I V I T Y 144,145,146Tb,145,146Dy,147,14~,15°Ho,148,la°Er,148,15°Tm [ f r o m 9°,91,92Zr,93Nb, 9~, 9 4 M o ( S a N i , x n y p ) , E = 2 3 3 - 2 5 0 MeVJ; m e a s u r e d "yy-eoin,EC/fl+,ET,I%fl-decay T~/2; d e d u c e d log f t , Ifl. tS°Er d e d u c e d Q(EC). 144,t45,146Gd,147,148,15°Dy,14STb,14s,15°Ho d e d u c e d l e v e l s , y - b r a n c h i n g . Z P A A D 306 223. R A D I O A C T I V I T Y laTDy; m e a s u r e d E T , I T , T T - e o i n . 147Tb d e d u c e d l e v e l s , J , r r . PRVCA 25 667. R A D I O A C T I V I T Y 144,145,146Tb,145,146Dy,147,148,15°Ho,148,15°Er,148,15°Tm [ f r o m 9°,gt,gZZr,93Nb, 9~, 9 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d ~ 7 - e o i n , E C / f l + , E % I y , f l - d e c a y T1/2; d e d u c e d log f t , lfl. 15°mr d e d u c e d Q(EC). 144,~45,14SGd,147,148,15°Dy,t4STb,14s,15°Ho d e d u c e d l e v e l s , ~ / - b r a n c h i n g . Z P A A D 306 223. NUCLEAR REACTIONS 9~94M~9~Nb(5~Ni~xnypz(x)/~4~Tm/~5~Tm/x47Er/14~Er/~4~Er/~5~Er/145H~/x49H~/~4~H~/ t46Ho/t47Ho/~44Dy/146Dy/~4SDy,E=233-250 MeV; 9 a M o ( S ° N i , x n y p z a ) , E = 2 4 0 - 2 5 9 MeV; m e a s u r e d ~r(E~/), 7y-coin,E~/,I-~,7(t),relative yields for residuals; deduced two proton evaporation dominance. 148,15°Er,147Ho d e d u c e d levels,J,Tr,Tt/~. B u n c h e d , p u l s e d b e a m t e c h n i q u e s . . ZPAAD 306

147Tm

147

KEYWORDS

=

148

R A D I O A C T I V I T Y Nd,Mo,Ge; m e a s u r e d E%I7; d e d u c e d n o e v i d e n e e f o r n e u t r i n o l e s s process, r i g h t h a n d e d c u r r e n t f r a c t i o n l i m i t s . 14s,15ONd,ga,l°°Mo d e d u c e d l i m i t o n d o u b l e f l - d e c a y T I / 2. 76Ge d e d u c e d l i m i t o n n e u t r i n o l e s s d o u b l e f l - d e c a y Tj/2. NCLTA 33 273. NUCLEAR REACTIONS 1 4 s , 1 5 2 S m ( e , e ' ) , E = 1 5 0 - 2 1 5 MeV; m e a s u r e d (r(0,E(e)). t48,tSZSm d e d u c e d giant multipole resonances,parameters,isovector GDR,isovector,isoscalar GQR s p l i t t i n g s , EWSR. P R V C A 25 2255. NUCLEAR REACTIONS 6SZn,9°,92,94Zr,ga,96,ga,J°°Mo,t24Te,a38Ba,14ZCe,146Nd,~5°SmfiaZTh(p,t),E = 5 2 MeV; m e a s u r e d (~(Et,0). 66Zn,9°,O2Zr,92,94,gSMo,X4°Ce,144Nd,148Sm,23°Th d e d u c e d d e e p t w o - h o l e states. Enriched t a r g e t s . N U P A B 376 513. NUCLEAR REACTIONS l a ° , l Z 4 S n ( Z S S i , x n ) , E = 1 0 8 - 1 4 4 MeV; m e a s u r e d I3~(0,H,t) v s T. 144 147,148Gd levels deduced quadrupole moment,tentative J,deformation. Pulsed beam,Ge(Li) detectors, recoil implantation i n t o Gd. N U P A B 379 287. R A D I O A C T I V I T Y 148Dy,JaSTb [ f r o m 14apr(laN,X),E=120 MeV3; m e a s u r e d 7 7 - , ( X - r a y ) 7 - e o i n , E % I T ; deduced Q(EC),end-point e n e r g y E f l + , m a s s e x c e s s . P R V C A 24 2695. R A D I O A C T I V I T Y 14SDy,148Tb [ f r o m 141pr(14N,X),E=120 MeV]; m e a s u r e d 7 ~ / - , ( X - r a y ) ~ - c o i n , E T , I ~ / ; deduced Q(EC),end-point e n e r g y E f l + , m a s s e x c e s s . P R V C A 24 2695.

66

KEY

NUMBERS

A 14aDy

D 82No08:

~4SHo

D

148Er

D 8gNo08:

8~No08:

R 82No07:

14aTm

D

83No08:

D 82Me10

1498m

D 8gMel0

R 82Ba15 149Eu

D 82Me10

149Tb

D 8~Bo04

D 82Be20

R 82Ja04 tS0Sm

R 8IWa31

15ODy

D 82Bo04

82Mo19

8gNo08

15OHo

D 82Mo19

continued

=

149

R A D I O A C T I V I T Y 149Eu(EC) [ f r o m S m ( p , x n ) , 1 4 % m ( a , 4 n ) l ~ 9 O d ( E C - d e c a y ) ] ; 149Pm(fl-) [ f r o m 14aNd(n, T)149Nd(fl-decay)3; measured E v , I v , v T - e o i n , I ( e e ). 149Sm d e d u c e d l e v e l s , I C C , v - m u l t i p o l a r i t y , band structure,configuration. Compton suppression,Ge(Li),Si d e t e c t o r s . J P H O B 8 1413. R A D I O A C T I V I T Y 149Eu(EC) [ f r o m Sm(p,xn),149Sm(a,4n)149Gd(EC-deeay)3; 149pm(fl-) [ f r o m 14aNd(n, T)14gNd(fl-deeay)3; measured E y , I v , y T - e o i n , I ( c e ) . 1498m d e d u c e d l e v e l s , I C C , 7 - m u l t i p o l a r i t y , band structure,configuration. Compton suppression,Ge(Li),Si d e t e c t o r s . J P H G B 8 1413. NUCLEAR REACTIONS ~4s,~5a,~54Sm(n,v),E=thermal; m e a s u r e d E%Iv. i49,~53,155Sm d e d u c e d levels. IANFA 46 63. R A D I O A C T I V I T Y t49Eu(EC) [ f r o m Sm(p,xn),t49Sm(a,4n)149Gd(EC-decay)?; 149Pm(fl-) [ f r o m ~4SNd(n, V)~4~Nd(fl-decay)?; measured E y , I v , v V - e o i n , I ( c e ) . i~SSm d e d u c e d l e v e l s , I C C , v - m u l t i p o l a r i t y , band structure,configuration. Compton suppression,Ge(Li),Si d e t e c t o r s . JPHGB 8 1413. R A D I O A C T I V I T Y ~ 5 ~ 5 ~ D y ~ 5 ~ i 5 i r n ~ 5 z ~ 5 ~ m H ~ i 5 ~ 5 ~ E r ~ 5 ~ 5 4 ~ 5 4 m T m ~ 7 9 ~ 7 s ~ 7 7 ~ 7 6 ~ t ~ 5 5 Y b ~ 9 ~ 197rn , ~9ampo,a3Fr,aaRa [from U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d Ea,Tt/z. 149Tb,aU,a~4,n5,ns,aVAt, a°~,al",a~SYr,~n,aUm,a~a,ns,al~Po,al~,a~Rn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV?; m e a s u r e d Ea. Helium jet recoil product separation. PRVCA ~5 941.

A 15ONd

148

=

KEYWORDS

R A D I O A C T I V I T Y 144,14514STb,145,14SDy,147,148,iS8Ho,148,15°Er,148,15°Tm [ f r o m 9°,si,9aZr,aaNb,Sa, 9 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV?; m e a s u r e d yy-coin,EC/B+,Ev,l%fl d e c a y %/~; d e d u c e d log f t , lfl. ~5°Er d e d u c e d Q(EC). 144,145,146Gd,147,148,15°Dy,14STb,148,150HOd e d u c e d l e v e l s , 7 - b r a n e h i n g . Z P A A D 306 ~23. R A D I O A C T I V I T Y ~4,1~s,~STb,~45,1~SDy,14~,l~s,~5~Ho,~4s,iS°Er,l*s,~5°Tm [ f r o m s°?l,SaZr,SaNb,Sa, 9 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d Ty-coin,EC/fl+,Ev,I%fl-decay TVa; d e d u c e d log f t , Ifl. ~S°Er d e d u c e d Q(EC). 144,145,146Gd,147,148,15°Dy,146Tb,14s,15°Ho d e d u c e d l e v e l s , T - b r a n c h i n g . Z P A A D 306 223. RADIOACTIVITY 144,145,146Tb,145,14SDy,147,148,15°Ho,14s,lS°Er,148,lS°Tm [ f r o m 9°,91,gaZr,gaNb,ga, ~ 4 M o ( S S N i , x n y p ) , E = 2 3 3 - 3 5 0 MeV]; m e a s u r e d 7T-coin,EC/fl+,Ev,Iv,fl-decay T1/a; d e d u c e d log f t , Ifl. 1SeEr d e d u c e d Q(EC). 144,145,14SGd,147,148,15°Dy,14STb,14s,15°Ho d e d u c e d l e v e l s , v - b r a n c h i n g . Z P A A D 306 3a3. NUCLEAR REACTIONS 9a,94Mo,SaNb(S~Ni,xnypza)/l~STm/~S°Tm/~4~Er/14~Er/~49Er/~S%r/14SHo/149Ho/~4SHo/ 146Ho/14~Ho/144Dy/146Dy/~4SDy,E=233 250 MeV; 9 a M o ( 6 ° N i , x n y p z a ) , E = 2 4 0 - 3 5 9 MeV; m e a s u r e d a(Ev), Ty-eoin,Ev,I%y(t),relative yields far residuals; deduced two proton evaporation dominance. 14a,~5°Er,147Ho d e d u c e d levels,J,~r,%/2. B u n c h e d , p u l s e d beam techniques. ZPAAD 306 ~11, R A D I O A C T I V I T Y ~44,~5746Tb,145,~4SDy,14v,14~,lS°Ho,14a,15°Er,14~,i5°Tm [ f r o m 9e,gi,gaZr,93Nb? e, ~ 4 M o ( 5 8 N i , x n y p ) , E = 2 3 3 - 2 5 0 MeV]; m e a s u r e d 7 T - c o i n , E C / f l + , E % I % f l - d e e a y Ti/2; d e d u c e d log f t , lfl. iS°Er d e d u c e d Q(EC). ~44,~4574SGd,i47,~48,15°Dy,~4STb,148,15°Ho d e d u c e d l e v e l s , v - b r a n c h i n g . ZPAAD 306 223.

A

t49pm

AND

=

150

R A D I O A C T I V I T Y Nd,Mo,Ge; m e a s u r e d EV,I% d e d u c e d n o e v i d e n c e f o r n e u t r i n o l e s s process, r i g h t b a n d e d c u r r e n t f r a c t i o n l i m i t s . 148,15°Nd,92,1°QMo d e d u c e d l i m i t o n d o u b l e f l - d e c a y T~/ 2. 76Ge d e d u c e d l i m i t o n n e u t r i n o l e s s d o u b l e f l - d e c a y T1/z. NCLTA 33 a73. NUCLEAR REACTIONS 154Sm(d?Li),E=33 MeV; m e a s u r e d G(E(6Li)),a(0). 15°Nd d e d u c e d l e v e l s , S a , a-reduced widths,rotational b a n d s . DWBA. P R V C A 26 405, NUCLEAR REACTIONS 1 5 a G d ( n , a ) , 5 ° V ( n , p ) , E = t h e r m a l ; m e a s u r e d cr(Ea),a(Ep); d e d u c e d Q. 15aGd d e d u c e d m a s s . 5°v,s°Ti,15aGd,15°Sm d e d u c e d m a s s d i f f e r e n c e , eaSTh d e d u c e d m a s s . A n a l y z e d (n, a ) d a t a , a a a U m a s s i n p u t . NUIMA 190 167. R A D I O A C T I V I T Y i5~i51Dy~i5i~i5im~i5a~i5~mH~i5~i5~Er~i5a~i54~154mTm~i79~178~i77~176~t~1~5Yb~9~ Is~m, t99mpo,alaFr,aaRa [from U,Th,Au,Ta(p,X),E=5 GeVS; m e a s u r e d Ea,Tj/a. 1 4 9 T b , a U , a 4 , ~ l s , a s , a 7 A t , ao4,as,eiaFr,eU,eUm,ala,ata,n4po,atv,ataRn I - f r o m U,Th,Au,Ta(p,X),E=5 GeV?; m e a s u r e d Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 15°Er(B +) [ f r o m 144Sm(ZeC,xnyp),E=124 MeV?; '5°Ho(B+),(EC) [ f r o m 15°Er d e c a y ? ; measured E%Iv,vv-,v(K X-ray)-coin. 15°Er l e v e l d e d u c e d TI/a. 15°Ho,iS°Dy d e d u c e d l e v e l s , J , Jr. P R V C A 26 1316. R A D I O A C T I V I T Y ~44,t4s,146Tb,145,14SDy,~4v,14s,l~°Ho,14B,15°Er,14B,i5°Tm [ f r o m 9°,sl,SaZr,9~Nb,Sa, 9 4 M o ( 5 S N i , x n y p ) , E = 3 3 3 - 3 5 0 MeVS; m e a s u r e d VV-coin,EC/fl+,EV,I%fl-deeay T1/a; d e d u c e d log f t , lfl. 15°Er d e d u c e d Q(EC). 144,145,14SGd,147,148,15°Dy,146Tb,148,15°Ho d e d u c e d l e v e l s , v - b r a n c h i n g . Z P A A D 306 333. R A D I O A C T I V I T Y 15°Er(fl+) [ f r o m 144Sm(12C,xnyp),E=124 M e V t 15°Ho(fl+),(EC) [ f r o m lS°Er d e c a y ] ; measured E % I v , v V ,T(K X - r a y ) - c o i n . 150Er l e v e l d e d u c e d Ti/a. 15°Ho,15°Dy d e d u c e d l e v e l s , J , Jr. P R V C A 26 1316.

67

KEY

NUMBERS

A i50Ho

D 82No08:

i50Er

D 82Mo19

82No08

82To14

AND

=

150

KEYWORDS

continued

RADIOACTIVITY 144,145,146Tb,145,146Dy,147,148,15°Ho,148,15°Er,148,150Tm [ f r o m 9°,91,gazr,93Nb, 92, 94Mo(58Ni,xnyp),E=233-250 MeV]; m e a s u r e d 77-coin,EC/fl+,ET,IT,fl-decay Tt/a; d e d u c e d log f t , Ifl. ~59Er deduced Q(EC). 144,145,146Gd,147,t48,15°Dy,146Tb,148,15°I~o deduced I e v e ] s , 7 - b r a n c h i n g . ZPAAD 306 223. RADIOACTIVITY ~5°Er(fl+) [ f r o m /44Sm(/eC,xnyp),E=124 MeV]; ~S°Ho(fl+),(EC) [ f r o m 15°Er decay]; m e a s u r e d E % I % 7 7 - , 7 ( K X - r a y ) - c o i n . ~5°Er l e v e l d e d u c e d T]/~. 15°Ho,15°Dy d e d u c e d l e v e l s , J , ~r. PRVCA 26 1316. RADIOACTIVITY 144,145,146Tb,145,146Dy,147,148,15°Ho,148,15°Er,148,150Tm [ f r o m 9°,91,9~Zr,93Nb,92, 94Mo(SaNi,xnyp),E=R33-250 MeV]; m e a s u r e d 77-coin,EC/fl+,ET,IT,fl-decay Tt/z; d e d u c e d log ft, Ifl. t5°Er d e d u c e d Q(EC). 144,145,14SGd,t4~,~4e,~S°Dy,t46Tb,148,tS°Ho deduced levels,7-branching. ZPAAD 306 223. RADIOACTIVITY i5°Er(EC),(fl+),la~Er(EC),(fl+),154Er(EC),(fl+)[from ~4%~47Sm(~ZC,xn)J,~5~yb(EC),

(fl+) [from ~44}47Sm(~80,xn)]; measured Ti/z,E%I%7~-coin,Ea. ~5~Tm,~52,~S~Ho deduced isomer T~/z,a-branching,predominant level systematics prolate configuration. PYLBB 117 It. R 82He08

82No07

*50Tm

D 82No08

NUCLEAR REACTIONS 92,94Zr,93Nb,9a,94,95Mo(SaNi,X),(62Ni,X),E~225-285 MeV; m e a s u r e d a(E~),~7-, ~(X-ray)-coin. ~5°Er,151Tm d e d u c e d l e v e l s , - y - b r a n c h i n g , J , v r , i s o m e r Tt/z,B(~),configuration. PYLBB 115 l l . NUCLEAR REACTIONS 9z,94Mo,SUNb(SeNi,xnypza)/i48Tm/lS°Tm/i47Er/14SEr/t4%r/tSOEr/'4~Ho/149Ho/t4aHo/ '46Ho/~47Ho/i44Dy/t4SDy/14SDy,E=233-E50 MeV; 9UMo(S°Ni,xnypz~),E=240-259 MeV; m e a s u r e d a(E~), 77-coin,ET,I~,7(t),relative yields for residuals; deduced two proton evaporation d o m i n a n c e . ~4s,]5°Er,~aTHo d e d u c e d levels,J,Tr,Tt/z. Bunched,pulsed b e a m t e c h n i q u e s . ZPAAD 306 211. RADIOACTIVITY 144,145,146Tb,145,146Dy,147,148,15°Ho,148,15°Er,148,15OTm [ f r o m 9°,sl,92Zr,93Nb,92, 94Mo(SaNi,xnyp),E=233-250 MeV]; m e a s u r e d 7 7 - c o i n , E C / f l * , E T , l T , f l - d e c a y Tl/e; d e d u c e d log ft, Ifl. tS°Er d e d u c e d Q(EC). ~44,145,t46Gd,t47,148,159Dy,laaTb,14a,~5°Ho d e d u c e d l e v e l s , ~ - b r a n c h i n g . ZPAAD 306 223.

A ~5~Sm

D 81Un02

'S~Eu

J 82Kr02 R 82Bo07:

151Gd

D 82Ba51:

~5~Tb

D 82Ba51:

*SiDy

D 82Bo04:

82Dell:

R 82Tr01:

ISiHo

D 82Bo04:

82Dell:

15~Tm

R 82He08:

15fLu

D 82Ho04:

=

151

RADIOACTIVITY 151Sin; m e a s u r e d I(K X - r a y ) / 1 7 , I ( L X - r a y ) / I T , E ( L X - r a y ) ; d e d u c e d i n t e r n a l s u b s h e l ] i o n i z a t i o n p r o b a b i l i t i e s . JPHGB 7 1683. NUCLEAR MOMENTS 151,153Eu; r n e a s u r e d o p t i c a l h f s ; d e d u c e d i s o t o p e s h i f t s . PHBCD 112 138. NUCLEAR REACTIONS t 5 ~ E u ( n , n ' 7 ) , E = f a s t ; m e a s u r e d ET,I7(E),I7(0). 15'Eu d e d u c e d levels,J,Tr, r o t a t i o n a l b a n d s , N i l s s o n c o n f i g u r a t i o n s . E n r i c h e d t a r g e t , G e ( L i ) d e t e c t o r . ZPAAD 304 257. RADIOACTIVITY 151Tb(EC),(fl +) [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d E T , I T , I ( c e ) , 7 ( c e ) - c o i n ; d e d u c e d log f t . ~SlGd d e d u c e d l e v e l s , J , ~ r , 7 - m u l t i p o l a r i t y . Toroidal beta-spectrometer, G e ( L i ) , S i - L i d e t e c t o r s , c h e m i c a l , i o n s e p a r a t i o n m e t h o d s . APOBB 13 89. RADIOACTIVITY 151Tb(EC),(fl +) [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d g T , I T , I ( c e ) , 7 ( c e ) - c o i n ; d e d u c e d log f t . ~SlGd d e d u c e d l e v e l s , J D r , 7 - m u l t i p o l a r i t y . Toroidal beta-spectrometer, G e ( L i ) , S i - L i d e t e c t o r s , c h e m i c a l , i o n s e p a r a t i o n m e t h o d s . APOBB 13 89. RADIOACTIVITY ~5~5~Dy~5~5~n~5~152mH~52~53Er~53~54~54mTm~79~7~77~76Pt~55Yb~98~97m~ l°9mpo,2'3Fr,ZlaRa [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d E~,Ti/2. 149Tb,Zn,214,zls,21s,217At, ~o4,ais,219Fr,211,anm,e'2,ala,a14po,alT,zleRn [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941. RADIOACTIVITY 162,163,164W,166,167,16B,169Re,167,168,169,17°Os,168,169,17°,171,17a,1731 r,175,176pt, 151Dy,151 m,lSl,152Ho,ISa,153Er,lSS,154Tm,154 Y b [ f r o m l°7,1°SAg,l°8,11°Cd,J~31n,ll~,J1°Sn(S3Cu,X), E = 2 4 5 - 3 0 0 MeVS; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149. NUCLEAR REACTIONS 13°Te,t24Sn(3aS,xn),E=150 MeV; measured ET,17,1inear p o l a r i z a t i o n , 7 ( ~ ) . t56,158Er,15i,15eDy d e d u c e d 7 - m u l t i p o l a r i t y , c o l l e c t i v e 7 - r a y c o n t i n u u m . P u l s e d beam,NaI(Tl), Ge(Li) d e t e c t o r s , t h r e e - G e ( L i ) p o l a r i m e t e r , N a I ( T ] ) a r r a y . NUPAB 378 141. RADIOACTIVITY ~5~5~Dy~5~,~5~m~52~52mH~5~53Er~53~54~54rnTm~79~78~77~76Pt~55Yb~9~97m~ 199mpo,alSFr,212Ra [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d Ec(,Tt/2. i49Tb,211,214,als,21s,2~TAt, ~°4,als,219Fr,211,211r~,212,21s,214po,217,21BRn [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeVS; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941. RADIOACTIVITY ~ 2 ~ 3 ~ 4 W ~ 6 6 ~ 7 ~ 8 ~ 9 R e ~ 6 7 ~ 6 8 ~ 6 9 ~ 7 ~ 8 ~ 6 ~ 7 ~ 7 ~ 7 e ~ 7 3 ~ 5 ~ 7 6 P t ~ 151Dy, 151 m,151,152H 0,15a,153Er,153,154Tm,154 Y b [ f r o m l°7,1°SAg,l°8,11°cd,l13In,lla,l16Sn(63Cu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149. NUCLEAR REACTIONS 92,94Zr,93Nb,92,94,95Mo(5SNi,X),(SaNi,X),E=225-285 MeV; m e a s u r e d a(ET),~7-, 7(X-ray)-eoin. 15°Er,iSlTm d e d u c e d l e v e l s , 7 - b r a n c h i n g , J , ~ r , i s o m e r T ~ / a , B ( ) , ) , c o n f i g u r a t i o n . PYLBB 115 11. RADIOACTIVITY 15tLu [ f r o m 9SRu(SSNi,2np),E=261 MeVS; m e a s u r e d Ep,Ip,direct p r o t o n decay T~/ 2,Q(p). C o i n c i d e n c e t e c h n i q u e s , e n r i c h e d R u t a r g e t . ZPAAD 305 111.

68

KEY

NUMBERS

A ~52Sm

D 81Is12: 811s14: R 78De42: 82An10:

82CI01:

82C103:

82Do06

82Ko03

~52Eu

D 81Is12 811s14

tSeGd

D 811s12 R 82Jo04

~SaDy

R 82Lu03

8~Sc07

82Tr01

~SaHo

D 81Ga36 82Bo04

82Deii

82To14

15ZEr

D 82Bo04

82Dell

AND

=

KEYWORDS

152

R A D I O A C T I V I T Y 152Eu; m e a s u r e d E % l % T v - c o i n . 15aSm,15eGd d e d u c e d l e v e l s , v - b r a n c h i n g , J , T r , K , rotational band,band structure. Ge(Li),hyperpure G e , N a I ( T I ) d e t e c t o r s . A P A H A 50 391. R A D I O A C T I V I T Y t6°Tb(fl-),tSaEu(EC),(fl+) [ f r o m Tb,Eu n e u t r o n i r r a d i a t i o n ] ; m e a s u r e d V T - c o i n . 16°Dy,152Sm d e d u c e d 2 + l e v e l TI/z,B(E2) r a t i o s . F a s t , s l o w c o i n c i d e n c e s y s t e m . RRPQA 26 461. NUCLEAR REACTIONS 152,~S4Sm(n,n'~/),E=fast; m e a s u r e d E%Iv. ~ae,154Sm d e d u c e d l e v e l s , J , r r , -/-branching,configurations. Enriched t a r g e t s . PIFLD 8 113. NUCLEAR REACTIONS 152,154Sm,Gd,15SGd,Dy,169Tm,174yb(dUCu,SSCu'),E=154,230 MeV; 15a,lS4Sm,Gd, 156Gd,Dy,169Tm,174yb(79Br,79Br'),(SlBr,81Br'),E=200,240 MeV; m e a s u r e d ( d a c u ) - / - , ( 7 9 B r ) 7 - c o i n , "/(0,H); d e d u c e d transient field ealibration,Z,velocity dependence. ~52,154Sm l e v e l s deduced g. N a t u r a l , e n r i c h e d targets,Ge(Li) detectors,transient f i e l d IMPAC t e c h n i q u e . N U P A B 383 509. NUCLEAR REACTIONS 16,1aO,e4Mg,ZSsi,a2s,adAr,4°Ca,S4Cr,144,15a,lS4Sm,a°sPb,a32Th(polarized d,d), (polarized d,d'),E=lS-23 MeV; m e a s u r e d a(O),iTH(O). 16,1eO,24Mg,aaSi,32S,SeAr,4°Ca,S4Cr,144, 152,154Sm,2°spb,ua2Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition strength. ~s4 152,144Sm,232Th d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . P R L T A 48 1083. NUCLEAR REACTIONS 160,4°,48Ca,S°Zr,144,~52,154Sm,a°dPb,e32Th(polarized d , d ) , ( p o l a r i z e d d,d'), E = 2 0 MeV; m e a s u r e d ¢r(O),iTll(O). 152,154Sm,aaeTh l e v e l s d e d u c e d s t a t i c m a s s q u a d r u p o l e moments. Coupled-channels a n a l y s i s . PYLBB 116 109. NUCLEAR REACTIONS 1 4 s , l a 2 S m ( e , e ' ) , E = 1 5 0 - 2 1 5 MeV; m e a s u r e d ff(0,E(e)). 148,ISZSm d e d u c e d giant multipole resonances,parameters,isovector GDR,isoveetor,isosealar GQR s p l i t t i n g s , EWSR. P R V C A 25 2255. NUCLEAR REACTIONS 15°Nd(a,2n-/),E=21-26 MeV; m e a s u r e d Ev,I%I(ce),v(0),~/(t),7~/(t),linear polarization. 152Sm d e d u c e d levels,J,~r,ICC,T1/2,7-branching. E n r i c h e d t a r g e t s , G e ( L i ) , G e , Si-Li detectors,mini-orange electron spectrometer. Interacting boson model calculations. N U P A B 373 397. R A D I O A C T I V I T Y 15aEu; m e a s u r e d ET,I%v-y-coin. 152Sm,152Gd d e d u c e d levels,~-branching,J,~r,K, rotational band,band structure. Ge(Li),hyperpure Ge,NaI(T1) d e t e c t o r s . A P A H A 50 391. R A D I O A C T I V I T Y 16°Tb(fl-),lS2Eu(EC),(fl +) [ f r o m Tb,Eu n e u t r o n i r r a d i a t i o n S ; m e a s u r e d ~/V-coin. l°°Dy,~SaSm d e d u c e d 2 + l e v e l T~/e,B(E2) r a t i o s . F a s t , s l o w c o i n c i d e n c e s y s t e m . RRPQA 26 461. R A D I O A C T I V I T Y ~5eEu; m e a s u r e d E T , I v , v ' y - c o i n . ~5~Sm,15~Gd d e d u c e d levels,~/-branching,J,Tr,K, rotational band,band structure. Ge(Li),hyperpure Ge,NaI(T1) d e t e c t o r s . A P A H A 50 391. NUCLEAR REACTIONS 15~Gd(4°Ar,4°Ar'),E=147.2 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , D S A , r e e o i l . ~5aGd l e v e l s d e d u c e d T~/e,B(E2). P R V C A 26 1004. NUCLEAR REACTIONS 154,155,~5~,~S°Gd(~,xn),E=40-110 MeV; m e a s u r e d E%Iv(0). ~46,~5°Nd (taC,xn), E = 8 0 - l l 0 MeV; m e a s u r e d E%l~/(O),ff f o r x = 4 - 8 . 15°Nd(~C,xnc~),E=80-110 MeV; m e a s u r e d cr f o r x = 4 - 6 . ~s2,~SSDy d e d u c e d l e v e l s , ~ / - m u l t i p l i c i t y , c e n t r o i d entry regions. Enriched targets, Ge(Li) d e t e c t o r , N a I multiplicity filter. Statistical m o d e l . N U P A B 379 125. NUCLEAR REACTIONS ~e3Sn(SZS,xn),E=160 MeV; m e a s u r e d 7"~(0) ratio,'~V(E). ~5~Dy d e d u c e d h i g h spin collective effects,superdeformed configuration parameters,moments of inertia. Rotating Woods-Saxon potential. P R L T A 48 1534. NUCLEAR REACTIONS i3°Te,~24Sn(3ZS,xn),E=150 MeV; m e a s u r e d E%I%linear polarization,v(0). ~56,~56Er,~5~,~SeDy d e d u c e d - ~ - m u l t i p o l a r i t y , e o l l e c t i v e */-ray continuum. Pulsed beam,NaI(T1), Ge(Li) d e t e c t o r s , t h r e e - G e ( L i ) polarimeter,NaI(Tl) a r r a y . N U P A B 378 141. R A D I O A C T I V I T Y ~SZHo,~5~Tm,l~°Lu; m e a s u r e d Ev,I%Ea,a-decay T t / ~ , a - b r a n c h i n g ; d e d u c e d Qa. I A N F A 4 5 2107. R A D I O A C T I V I T Y 150,151Dy,151,151 m,lS2,152m H0,152,153Er,153,154,154 mTm,179,178,177,176pt,i55y b,198,197m, 199mpo,~Fr,Z~Ra [from U , T h , A u , T a ( p , X ) , E = 5 GeV~; m e a s u r e d E~,T~/~. ~49Tb,Z~,~4,u~5,u~u,Z~VAt, e°%e~s,z~OFr,Z~,aHm,a~e,z~a,a~¢Po,a~,e~aRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 162,163,164w,iSd,167,168,169Re,167,168,169,17°Os,168,ids,176,171,17~,1731r,175,176p t, ~5~Dy,15~m,~51,~52Ho,15e,~SUEr,~53,~SaTm,i54yb [ f r o m ~°7,~°9Ag,~°a,ll°Cd,~aIn,l~z,~l~Sn(daCu,X), E ~ 2 4 5 - 3 0 0 MeVS; m e a s u r e d E~. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149. R A D I O A C T I V I T Y ~5°Er(EC),(fl+),~SaEr(EC),(fl+),i54Er(EC),(fl+)[ f r o m ~44,~4~Sm(~eC,xn)J,~5~yb(EC), (fl+) [ f r o m ~ 4 , ~ S m ( l e 0 , x n ) 3 ; m e a s u r e d T ~ / z , E % I % T v - c o i n , E ~ . ~5~Tm,~5a,~5~Ho d e d u c e d i s o m e r T~/z,~-branching,predominant l e v e l s y s t e m a t i c s p r o l a t e c o n f i g u r a t i o n . PYLBB 117 11. RADIOACTIVITY ~ 5 ~ 1 5 ~ D y ~ 5 ~ m ~ 5 ~ 5 e m H ~ 5 ~ 5 ~ E ~ 5 ~ 5 4 ~ 5 4 r n T m ~ i 7 ~ t ~ e ~ 7 7 ~ 7 6 P t ~ i 5 5 Y b ~ 1 ~ 8 ~ 197m, t99mpo,el~Fr,elaRa [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d E~,T~/e. 149Tb,Zlt,z14,eis,als,atTAt, zo~ ~ 8 , e t g F r , e H , e ~ m , e ~ z , z ~ a , a l 4 p o , a ~ 7 , ~ S R n [from U,Th,Au,Ta(p,X),E=5 GeVS; m e a s u r e d E~. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 162,163,164W,166,167,168,1S9Re,167,168,169,i760s,lSS,169,170,171,172,173I r,175,iTSpt, ~5~Dy,~5~rn,~5~,~SeHo,~52,153Er,~Sa,~S~Tm,tS4yb [ f r o m ~°7,~°~Ag,~°8,HoCd,~aln,~l~,H~Sn(~aCu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. Enriched targets,precision measurement,He-jet transport. A N P H A 7 149.

69

KEY

NUMBERS

A

ISZEr

D 83To14:

R 83Ba15

153Eu

J 83Kr03 D 83A134

153Gd

R 81Wa31

153Tb

D 83A134

~53Er

D 82Bo04

83Dell:

R 82Ca09

82Fo06

~53Tm

D 83Bo04

82Dell

R 78De42 82An10

82C101

83C103

154Eu

D 83Co05:

154Gd

R 82Da12:

152

continued

=

153

NUCLEAR REACTIONS 14e,~52,154Sm(n,v),E=thermal; m e a s u r e d E%Iv. x49,153,155Sm d e d u c e d levels. I A N F A 4 6 63. NUCLEAR MOMENTS isl,153Eu; m e a s u r e d o p t i c a l h f s ; d e d u c e d i s o t o p e s h i f t s . PHBCD 113 138. R A D I O A C T I V I T Y 153Tb [ f r o m Ta(p,X)3; measured (ce)-/-coin,v~(0),(ce)v(t),(ce)(ce)(t),vV(0, H); d e d u c e d log f t . 153Gd d e d u c e d levels,J,Tr,T1/2,g,6,B(:~ ). N a t u r a l Ta t a r g e t , i s o t o p e , mass-separated s o u r c e s . N U P A B 383 333. NUCLEAR REACTIONS ~ 5 3 G d ( n , ~ ) , S ° V ( n , p ) , E = t h e r m a l ; m e a s u r e d cr(Ea),a(Ep); d e d u c e d Q. 153Gd d e d u c e d m a s s . 5°V,5°Ti,~53Gd,15°Sm d e d u c e d m a s s d i f f e r e n c e . 235Th d e d u c e d m a s s . A n a l y z e d (n, ~) d a t a , Z 3 e U m a s s i n p u t . NUIMA 190 167. R A D I O A C T I V I T Y ~53Tb [ f r o m Ta(p,X)3; measured (ce)v-coin,vv(0),(ce)v(t),(ce)(ce)(t),TV(0, H); d e d u c e d log f t . '53Gd d e d u c e d levels,Jjr,Ta/~,g,5,B(~). Natural Ta t a r g e t , i s o t o p e , mass-separated s o u r c e s . N U P A B 383 333. R A D I O A C T I V I T Y 15°,151Dy,151,15im,152,152m Ho,15~,153Er,153,154,154mTm,179,178,177,176pt,155y b,198,197m, ~99mpo,Z~3Fr,2~eRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV3; m e a s u r e d Ea,T~/~. a49Tb,~U,2~4,215,~6,217At, ~°4,~s,2~gFr,2~,Z~lm,Zl2,el3,Z~4po,2~,z~SRn [ f r o m U,Th,Au,Ta(p,X),]~3=5 G e V ] ; m e a s u r e d E~. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 162,163,164 W,166,167,168,169Re,167,168,169,17°0s,168,169,17°,171,17~,173I r,175,176P t, 151Dy,151rn,151,152Ho,15~,153Er,153,154Tm,154yb [ f r o m l°7,1°gAg,i°8,118cd,l13In,l12,1iSSn(63Cu,X), E = 3 4 5 - 3 0 0 MeV3; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149. NUCLEAR REACTIONS ~ 4 4 S m ( ~ e C , 3 n ) , E = 5 3 - 6 5 MeV; m e a s u r e d EV,Iv(E),IT(t),IT(0),-/-ray multiplicity mean values,standard deviations,l(ce). 153Er d e d u c e d levels,J,~r,T,/2. Enriched targets,Ge(Li),Ge,NaI(T1) detectors,Compton suppression,mini-orange electron spectrometer w i t h S i - L i d e t e c t o r . NUPAB 381 155. NUCLEAR REACTIONS 14~Sm(~ZC,3n),E ~ 76 MeV; m e a s u r e d ' E v , I % v ( 0 ) , a ( E v ) , V V - c o i n , c e ( t ) , v T ( t ) . lS3Er d e d u c e d l e v e l s , v - b r a n c h i n g , i s o m e r s , T 1 / 2 , J , T r , I C C , c o n f i g u r a t i o n s . Shell model. ZPAAD 305 81. R A D I O A C T I V I T Y i5~51Dy~5~5~m~52~52mH~5~53Er~53~54~54mTm~79~78~77~76Pt~55Yb~98~i97m~ ~99mpo,Z'3Fr,Z12Ra [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV2; m e a s u r e d Ea,T~/~. a49Tb,ZU,za4,~15,~6,e~TAt, 29%zls,~lgFr,eU,Znm,~12,~3,Z14po,~XT,~lSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 16~,163,164 W,166,167,168,169Re,167,168,169,17°0s,168,169,17°,171,172,173I r,175,176p t, ~SlDy,~5~rn,~5',15eHo,iS~,'53Er,153,154Tm,154yb [ f r o m ~°7,~°9Ag,a°8,n°Cd,ll3In,ll2,nSSn(6~Cu,X), E=245-306 MeV]; measured Ea. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149.

A 154Sm

=

KEYWORDS

R A D I O A C T I V I T Y ~5°Er(EC),(fl+),152Er(EC),(fl+),154Er(EC),(fl+) [ f r o m ~44,147Sm(~ZC,xn)3,156yb(EC), (fl+) [ f r o m 14~,~4~Sm(aSO,xn)]; m e a s u r e d T , / 2 , E % l % ~ / 7 - c o i n , E ~ . ~56Tm,152,~SaHo d e d u c e d i s o m e r T~/~,a-branching,predominant level systematics prolate configuration. PYLBB 117 11.

A 153Sm

AND

=

154

NUCLEAR REACTIONS 1 5 2 , 1 5 4 S m ( n , n ' v ) , E = f a s t ; m e a s u r e d E'y,I~. ls2,154Sm d e d u c e d levels,J,~r, v-branching,configurations. Enriched t a r g e t s . PIFLD 8 113. NUCLEAR REACTIONS 152,154Sm,Gd,156Gd,Dy,169Tm,17~yb(63Cu,~3Cu'),E=154,230 MeV; 15e,154Sm,Gd, 1 5 6 G d , D y , ' 6 9 T m , ' 7 4 y b ( 7 9 B r , 7 9 B r ' ) , ( S l B r , S a B r ' ) , E = 2 0 0 , 2 4 0 MeV; m e a s u r e d (63Cu)v-,(79Br)*y-coin, V(0,H); d e d u c e d transient field calibration,Z,veloeity dependence. 152,154Sm l e v e l s deduced g. N a t u r a l , e n r i c h e d targets,Ge(Li) detectors,transient f i e l d IMPAC t e c h n i q u e . N U P A B 383 509. NUCLEAR REACTIONS 16,1SO,e4Mg,28Si,32S,SSAr,4°Ca,54Cr,144,152,i54Sm,Z°sPb,e3ZTh(polarized d,d), (polarized d,d'),E=18-33 MeV; m e a s u r e d a(0),iT11(0). 16,180,24Mg,eSSi,3eS,3°Ar,4°Ca,54Cr,144, 152,154Sm,2°sPb,232Th l e v e l s d e d u c e d i s o s e a l a r q u a d r u p o l e , o c t u p o l e transition strength. 154, 'se,144Sm,232Th deduced neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . P R L T A 48 1083. NUCLEAR REACTIONS 160,4°,48Ca,9°Zr,144,15z,154Sm,~°sPb,232Th(polarized d , d ) , ( p o l a r i z e d d,d'), E=20 MeV; m e a s u r e d ~ ( 0 ) , i T u ( 0 ) . 15z,154Sm,23ZTh l e v e l s d e d u c e d s t a t i c m a s s q u a d r u p o l e moments. Coupled-channels a n a l y s i s . PYLBB 116 109. R A D I O A C T I V I T Y 125Sb,154,155Eu; m e a s u r e d E%I%E(X-ray),I(X-ray); deduced photon,X-ray emission rates. Separated,mixed s o u r c e s . NUIMA 193 1. NUCLEAR REACTIONS 152Sm(~,2n),E=19.5 MeV; m e a s u r e d E % I % l i n e a r p o l a r i z a t i o n v s 0. 154Gd deduced levels,J,Tr,vibrational band characteristics,v-multipolarity,6. Fast counting Ge(Li) p o l a r i m e t e r , i n - p l a n e , o u t - o f - p l a n e sum,difference s p e c t r a . NUIMA 193 6 4 7 .

70

KEY

NUMBERS

A ~54Tb

R 8~Be46

~54Dy

R 82Le16 83PalO

154Ho

D 83To14

~5~Er

D 83To14

~54Tm

D 8~Bo04

8EDell

~54yb

D

82Dell

~55Sm

D 82Gr13 R 82Ba15 8~SeO3

155Eu

D 83Co05

~55Gd

J

82Ta01

R 81Be57 ~55Tb

R 82Be46

lasYb

D 8~Bo04

=

D 81Bu34

156Gd

D 81Bu24: R 82Ba28:

83Ha13:

continued

targets,precision

measurement,He-jet

transport.

155

RADIOACTIVITY 155Pro [ f r o m 25aCf(SF),chemical separation]: measured ET,17,TI/a. 155Sm deduced levels,7-branehing. RAACA 30 57. RADIOACTIVITY l a 5 p m [ f r o m aSaCf(SF),chemical separation3: measured E~/,IT,Tt/a. 155Sm deduced levels,7-branehing. RAACA 30 57. NUCLEAR REACTIONS 148,152)54Sm(n,3,),E=thermal; m e a s u r e d E7,I% 14a,lsa,155Sm d e d u c e d levels. IANFA 46 63. NUCLEAR REACTIONS ~ 5 4 S m ( n , 7 ) , E = t h e r m a l , - > 10O eV,2,24 keV; m e a s u r e d E-/,!7; 154Sm(n,e), E=thermal; measured I(ce). 155Sm d e d u c e d levels,neutron binding energy,transitions, "y-multipolarity,J,~r,ICC. Curved crystal,magnetic conversion electron,Ge(Li) pair spectrometers,enriched t a r g e t . N i l s s o n m o d e l , C o r i o l i s , A N = 2 c o u p l i n g s . NUPAB 376 149. RADIOACTIVITY lasSb,la4,15SEu; m e a s u r e d E%I%E(X-ray),I(X-ray); deduced photon,X-ray emission rates. Separated,mixed s o u r c e s . NUIMA 193 1. NUCLEAR MOMENTS 155,157Gd; m e a s u r e d m u o n i c X - r a y s , h y p e r f i n e splittings; deduced q u a d r u p o l e moments. PYLBB 108 8. NUCLEAR REACTIONS 154Gd(n,~/),E=thermal; m e a s u r e d E?/,I% lSSGd d e d u c e d l e v e l s , J j r , n e u t r o n reduced width,r7 correlation. Quasiparticle-phonon m o d e l . YAFIA 34 1158. NUCLEAR REACTIONS 148,1SONd(nB,xn),E=50-68 MeV; m e a s u r e d E-y,I%cr(ET,07,E),77(t),llBT(t). 154,155,tSSTb d e d u c e d levels,JJr,T~/a,eonfiguration,band systematies. Enriched targets. NUPAB 389 158. R A D I O A C T I V I T Y 15~l51Dy~l~1,151m,152~152mH~,1~15~Er~t~3~1~4,l54mTm,1~9,178,177,176~t,j5~Yb,198~197m, 199mpo,alaFr,a12Ra [ f r o m U,Th,Au,Ta(p,X),E=5 GeV3; m e a s u r e d Ea,TI/2. i49Tb,ell,214,215,alo,alTAt, a°4,218,alaFr,all,a~lm,2~a,a~3,a~4Po,a~v,a~SRn [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV3; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941.

A 156Eu

154

Ea. E n r i c h e d

A D 83Gr13

=

KEYWORDS

NUCLEAR REACTIONS ~48,~5°Nd(UB,xn),E=50-68 MeV; m e a s u r e d E'LI%cr(E~/,0%E),'~(t),~B'~(t). 154,155,156Tb deduced levels,J,rr,T~/a,eonfiguration,band systematies. Enriched targets. NUPAB 389 158. NUCLEAR REACTIONS ~ S H o , ~ 8 ~ T a ( r r - , x n ) , E a t r e s t ; m e a s u r e d 7n-coin. ~e,~s°,~ss,~56,154Dy deduced neutron energy for given multiplicity. PYLBB 114 427. NUCLEAR REACTIONS 124Sn(S4S,4n),E=145-165 MeV; m e a s u r e d 7-~-coin,3,(0),cr(E-/),recoil. ~54Dy d e d u c e d levels,J,Tr,-~-branching,T~/a,yrast level i n t r i n s i c q u a d r u p o l e m o m e n t s , b a c k b e n d i n g , s h a p e c h a n g e . PRLTA 48 1530. RADIOACTIVITY ~5°Er(EC),(fl+),~SaEr(EC),(fl+),~5~Er(EC),(fl +) [ f r o m t44,~4~Sm(~aC,xn)],~5eyb(EC), (fl+) [ f r o m ~44,~47Sm(~60,xn)]; m e a s u r e d Ti/2,E~,13,,~/'y-coin,Ea. t56Tm,t52,~SaHo d e d u c e d i s o m e r T~/a,a-branehing,predominant l e v e l s y s t e m a t i c s p r o l a t e c o n f i g u r a t i o n . PYLBB 117 11. RADIOACTIVITY ~5°Er(EC),(fi+),ISZEr(EC),(fl+),~54Er(EC),(fl+)[ f r o m t44,~47Sm(~aC,xn)],lsSyb(EC), (fl+) [ f r o m 144,147Sm(tS0,xn)3; m e a s u r e d T~/a,E%I3,j/-y-coin,Ec~. ~5STm,~52,~54Ho d e d u c e d i s o m e r T~/a,c~-branching,predominant level systematics prolate configuration. PYLBB 117 11. RADIOACTIVITY ~5~5~Dy'~5~'~5~m'~52~52mH~5a'~53Er'~5~4~54mTm~79~78~77~7~pt~55Yb~9~97m~ ~9~rnpo,al3Fr,a~aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d E~,T~/a. t49Tb,aU,214,215,a~6,a~TAt, a°4,a~8,atgFr,al~,a~rn,~ta,ala,a~4Po,e~7,e~aRn [from U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941. R A D I O A C T I V I T Y 162,163,164 w,l S6,167,168,169Re,167,168,169,1780s,lSS,169,17°,171,17~,1731 r,175,176pt, ~5~Dy,i5~m,tSt,~SaHo,~Sa,~aaEr,~Sa,i54Tm,i54yb [ f r o m 167,~°gAg,l°a,~°Cd,H3In,~a,l~SSn(SSCu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149. RADIOACTIVITY •6a••63••64W••66•••7••6•••69Re••67••6•••69••7••s••••••69••7•••7•••7a••7•I•••75••76•t• 151Dy,151m,151,152Ho,152,153Er,lSa,154Tm,154 Yb [ f r o m l°7,1°gAg,l°8,11°Cd,l13In,lla,llSSn(63Cu,X), E = a 4 5 - 3 0 0 MeV3; m e a s u r e d ANPHA 7 149.

~55pm

AND

156

RADIOACTIVITY 156Eu,166Ho; m e a s u r e d l(ce). 15SGd,166Er t r a n s i t i o n s deduced s u b s h e l l ICC ratios. IANFA 45 2133. RADIOACTIVITY ~SSEu,166Ho; m e a s u r e d I(ce). I56Gd,166Er t r a n s i t i o n s deduced s u b s h e l l ICC ratios. IANFA 45 2133. NUCLEAR REACTIONS 155Gd(n,'y),E=thermal,resonance; m e a s u r e d E%Iv,l(ce). 156Gd deduced Ievels,J,~r,lCC,B(X),neutron b i n d i n g energy. Ge(Li) d e t e c t o r s , c u r v e d - c r y s t a l s p e c t r o m e t e r , m a g n e t i c e l e c t r o n - s p e c t r o m e t e r s , e n r i c h e d targets. NUPAB 380 189. NUCLEAR REACTIONS i°°Mo(TLi,2np),(TLi,nd),(TLi,t),i54Sm(TLi,4np),(VLi,3nd),(7Li,2nt),E=48 MeV; m e a s u r e d E3',Iv,vV , 7 ( p a r t i c l e ) - c o i n . 1°4Ru,156Gd deduced levels. PRVCA 25 1699.

71

KEY

NUMBERS

A I5OGd

R 831s05

,56Tb

R 82Be46

'SSDy

J

82C104

R 82De13

82Le16 82Lu03:

83Ro07: I56Ho

R 82Lo05:

'5SEr

D 82EIOI: R 82Ri02:

82TrOl:

ISSTm

D

81Ga36: 82To14:

J

15?Dy

R 82De13:

157Ho

R 82Ha27:

157Er

D 82EIOI:

82TaOl:

R 82Hu03:

R 821s05:

~58Dy

J

82C104:

156

continued

=

157

NUCLEAR MOMENTS 155,157Gd; m e a s u r e d m u o n i c X - r a y s , h y p e r f i n e splittings; deduced q u a d r u p o l e moments. PYLBB 108 8. NUCLEAR REACTIONS 158Gd(a,xn7),E=70 MeV; m e a s u r e d a ( E n ) , a ( 0 n ) , I 7 , E 7 f o r x=4,5,6. 156,157 t58Dy d e d u c e d 7 m u l t i p l i c i t i e s , t o t a l 7-ray energy,neutron energy,angular momentum release. Enriched lSaGd t a r g e t . Ge(Li),Nal(T1) d e t e c t o r s , N E 213 l i q u i d scintillator,Tof. NUPAB 379 160. NUCLEAR REACTIONS i46Nd(*SN,4n),E=74 MeV; m e a s u r e d 17(0),77-coin. 157Ho d e d u c e d levels,Jjr, d,branching ratios,(g(k)-g(R)),shape c h a n g e . PRVCA 25 3224. RADIOACTIVITY 156,157,158Er [ f r o m 1 2 2 S n ( 4 ° A r , x n ) , E = 1 8 5 MeV]; m e a s u r e d 77(E); d e d u c e d noneollective alignment e f f e c t s a t h i g h s p i n . PRLTA 48 870. NUCLEAR REACTIONS 28Si('agXe,xn),E=730 MeV; 28Si(13°Xe,xn),E=740 MeV; m e a s u r e d DSA,ET,I 7. 164,*STEr d e d u c e d c o n t i n u u m transition Ti/2,B(E2),fle,quadrupole moment. Ge(Li),NaI(Tl) d e t e c t o r s . ZPAAD 304 225.

A 158Gd

=

KEYW0RDS

NUCLEAR REACTIONS '42,143,14SNd,'55,'STGd,161,16a,164Dy,'SSHo,lV4,173yb(n,7),E=thermal; m e a s u r e d E~. 143,144,146Nd,156,*58Gd,162,163,164,185Dy,166Ho,175,174yb deduced neutron separation energy. PRVCA 25 3184. NUCLEAR REACTIONS 14a,*SONd(nB,xn),E=50-68 MeV; m e a s u r e d E T , I T , g ( E 7 , 0 7 , E ) , 7 7 ( t ) , l ' B T ( t ) . 154,155,156Tb deduced levels,J,vr,T,/a,eonfiguration,band systematics. Enriched targets. NUPAB 389 158. NUCLEAR MOMENTS '56,158,16°,*61,'62,163,t°4Dy; measured hfs,optical isotope shifts; deduced rms charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 26 1638. NUCLEAR REACTIONS *SaGd(a,xn7),E=70 MeV; m e a s u r e d c;(En),a(On),I7,E7 f o r x=4,5,6. 156*57 'SSDy d e d u c e d 7 m u l t i p l i c i t i e s , t o t a l 7-ray energy,neutron energy,angular momentum release. Enriched lSSGd t a r g e t . G e ( L i ) , N a l ( T l ) d e t e c t o r s , N E 213 l i q u i d scintillator,Tof. NUPAB 379 160. NUCLEAR REACTIONS 165Ho,t81Ta(w-,xn),E a t r e s t ; m e a s u r e d 7n-coin. *sa,ls°,/s8,~56,'S4Dy deduced neutron energy for given multiplicity. PYLBB 114 427. NUCLEAR REACTIONS 154,15s,16a,laOGd(a,xn),E=40-llO MeV; m e a s u r e d E7,I7(0). 14s,iS°Nd (laC,xn), E=80-11O MeV; m e a s u r e d ET,I7(0),a f o r x = 4 - 8 , lS°Nd(12C,xna),E=80-110 MeV; m e a s u r e d a f o r x = 4 - 6 . 152,15°Dy d e d u c e d l e v e l s , 7 - m u l t i p l i c i t y , c e n t r o i d entry regions. Enriched targets, Ge(Li) d e t e c t o r , N a l m u l t i p l i c i t y f i l t e r . S t a t i s t i c a l m o d e l . NUPAB 379 125. NUCLEAR REACTIONS 16s,lSSDy,'Sa,'64Er,168yb(a,a'),E=12-16 MeV; m e a s u r e d a. 1ss,158Dy,16a,'~4Er, l s s y b l e v e l s d e d u c e d B(),). E n r i c h e d t a r g e t s . PRVCA 28 97. NUCLEAR REACTIONS 146Nd(14N,4n),E=72 MeV; m e a s u r e d 77-coin. 156Ho d e d u c e d l e v e l s , 7-branching,rotational b a n d s . PHSTB 25 459. RADIOACTIVITY *56,tsT,~SSEr [ f r o m l a a S n ( 4 ° A r , x n ) , E = 1 8 5 MeVS; m e a s u r e d 77(E); d e d u c e d noncollective alignment e f f e c t s a t h i g h s p i n . PRLTA 48 670. NUCLEAR REACTIONS n a S n , ~ S 4 S m , 1 9 7 A u ( ~ O A r , p F ) , ( 4 ° A r , d F ) , ( 4 ° A r , t F ) , ( 4 O A r , a F ) , E = 3 3 3 MeV; measured (fragment)p-,(fragment)d-,(fragment)t-,(fragment)a-coin,a(fragment 0,0p,Ep), a(fragment 0,0a,Ea); deduced reaction mechanism. 237Bk,ia4Hg,156Er d e d u c e d e m i s s i o n barriers,level density parameters,fins(J). Evaporation,statistical m o d e l s . PRVCA 25 2430. NUCLEAR REACTIONS '3°Te,ia~Sn(3aS,xn),E=150 MeV; m e a s u r e d E T , I T , l i n e a r p o l a r i z a t i o n , 7 ( 0 ) . ~ss,lSSEr,~5t,lSaDy d e d u c e d 7 - m u l t i p o l a r i t y , c o l l e c t i v e 7-ray continuum. P u l s e d beam,NaI(T1), Ge(Li) d e t e c t o r s , t h r e e - G e ( L i ) p o l a r i m e t e r , N a I ( T 1 ) a r r a y . NUPAB 378 141. RADIOACTIVITY 'SaHo,'56Tm,l°°Lu; m e a s u r e d E T , I T , E a , a - d e c a y T 1 / a , a - b r a n c h i n g ; d e d u c e d Qa. IANFA 45 2187. RADIOACTIVITY 15°Er(EC),(fl+),~SZEr(EC),(fl+),~54Er(EC),(fl+) [ f r o m 144,'47Sm(laC,xn)],~s~yb(EC), (fl+) [ f r o m '4~,147Sm(160,xn)3; m e a s u r e d T i / z , E T , I T , 7 7 - c o i n , E a . 156Tm,15a,lS4Ho d e d u c e d i s o m e r Tl/a,a-branching,predominant level systematics prolate configuration. PYLBB 117 11.

A 157Gd

AND

=

158

NUCLEAR REACTIONS 142,143,'45Nd,lSs,tS7Gd,tSl,lsz,164Dy,165Ho,174,173yb(n,7),E=thermal; m e a s u r e d E7. 143,t44,146Nd,lSs,lSSGd,taa,la3,164,165Dy,lS6Ho,175,174Yb d e d u c e d n e u t r o n separation energy. PRVCA 25 3184. NUCLEAR MOMENTS lss,lss,la°,iai,16a,i63,1S4Dy; m e a s u r e d hfs,optical isotope shifts; deduced rms charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 36 1636.

72

KEY

NUMBERS

A ~58Dy

R 83De13

82Le16 82Ro07 158Er

D 82E101 R 8iYal0:

82Tr01:

D 82Vy02:

159He

D 82Vy02: R 82Ha17:

=

158

=

D 81Is14: 82Kr04: R 82A103:

160Dy

D 81Is14: 83Kr04 J

81Ah05 82C104

R 82Le16 ls0yb

R 82Ja08

t6OLu

D 81Ga36

J

82C104

159

160

RADIOACTIVITY 16°Tb(fl-),IS2Eu(EC),(fl +) [from Tb,Eu neutron irradiation]; measured T~-coin. IS°Dy,152Sm deduced 2+ level TI/a,B(E2) ratios. Fast,slow coincidence system. RRPQA 26 461. RADIOACTIVITY ISeTb Efrom Tb(n,T)]; measured IT(0),oriented nuclei; deduced hyperfine interaction parameters. 16°Dy deduced E2/MI,M2/EI,E3/EI mixing ratios 6. NUPAB 377 176. NUCLEAR REACTIONS 141Pr,lSSTb,lS5Ho,167Er,lSSTm(polarized n,X),E=0.001-100 keV; measured transmission; d e d u c e d (~ spin dependence,strength functions, i42pr,16°Tb,16SHo,lSSEr,lSSTm resonances deduced J. Polarized n a t u r a l targets,liquid scintillation detector. NUPAB 376 229. RADIOACTIVITY 'S°Tb(fl-),i5aEu(EC),(fl +) [ f r o m Tb,Eu neutron irradiation]; measured TT-eoin. IS°Dy,iSaSm deduced 2+ level TI/2,B(E3) ratios. Fast,slow coincidence system. RRPQA 26 461. RADIOACTIVITY IS°Tb [ f r o m Tb(n,T)]; measured I~/(0),oriented nuclei; deduced hyperfine interaction parameters, iSODy deduced E2/MI,M2/EI,E3/EI mixing ratios 6. NUPAB 377 176. NUCLEAR MOMENTS Is4,'SODy; measured optical isotope shifts. Enriched isotopes,Fabry-Perot spectrometer. IJOPA 19 1183. NUCLEAR MOMENTS Iss,15s,ls°,ISl,lSa,lsa,lS4Dy; measured hfs,optical isotope shifts; deduced r m s charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser spectroscopy. PRVCA 36 1636. NUCLEAR REACTIONS ISSHo,lSITa(Tr-,xn),E at rest; measured -/n-coin. Is2,1s°,'ss,lss,154Dy deduced n e u t r o n energy for given m u l t i p l i c i t y . PYLBB 114 427. NUCLEAR REACTIONS '4SNd(2°Ne,6n),E=136,149 MeV; measured ~/-multiplicity. i~°Yb deduced e n t r y state population,decay properties,shape change. Spin spectrometer. PRLTA 49 1387. RADIOACTIVITY i52Ho,lSSTm,lS°Lu; measured E%IT,Ea,~-decay Ti/2,~-branching; deduced Qa. IANFA 45 2107.

A i61Dy

continued

RADIOACTIVITY t59Ho; measured Efl+,lfl+/I(K X-ray),E%I%I(ce); deduced fl-strength function. i59Dy deduced levels,ICC,T-multipolarity,6. IANFA 46 16. RADIOACTIVITY i59Ho; measured Efl+,Ifl+/I(K X-ray),ET,IT,I(ce); deduced fl-strength function. iSSDy deduced levels,ICCjT-multipolarity,d. IANFA 46 16. NUCLEAR REACTIONS l s a , i S 4 E r ( p , ~ ) , E = 1 7 MeV; m e a s u r e d cr(Ec~),cr(0), lSiHo l e v e l s d e d u c e d normalization f a c t o r s . 159Ho d e d u c e d l e v e l s , J , ~ r , S , r o t a t i o n a l b a n d s , N i l s s o n a s s i g n m e n t s . Enriched targets. Triton cluster transfer D W B A , C o r i o l i s m i x i n g c a l c u l a t i o n s . ZPAAD 305 143.

A =

ISOTb

KEYWORDS

NUCLEAR REACTIONS 158Gd(~,xnT),E=70 MeV; m e a s u r e d cr(En),~(0n),I3',E~/ f o r x=4,5,6. 15s,157, 15SDy d e d u c e d T m u l t i p l i c i t i e s , t o t a l v-ray energy,neutron energy,angular momentum release. Enriched 15SGd t a r g e t . Ge(Li),Nal(T1) d e t e c t o r s , N E 213 l i q u i d scintillator,Tof. NUPAB 379 160. NUCLEAR REACTIONS lS5Ho,iSlTa(Tr-,xn),E a t r e s t ; m e a s u r e d Tn-coin. 162,~s°,15s,15s,lS*Dy deduced neutron energy for given multiplicity. PYLBB 114 437. NUCLEAR REACTIONS 156,158Dy?Sa,iS4Er,iSSyb(a,(x'),E=12-16 MeV; m e a s u r e d c~. 156,iSSDy,laa,lS4Er, l s s Y b l e v e l s d e d u c e d B(X). E n r i c h e d t a r g e t s . PRVCA 26 97. R A D I O A C T I V I T Y ~5s,'sT,15SEr [ f r o m 1 2 2 S n ( t ° A r , x n ) , E = 1 8 5 MeV]; m e a s u r e d T~/(E); d e d u c e d noncollective alignment e f f e c t s a t h i g h s p i n . PRLTA 48 670. NUCLEAR REACTIONS '54Sm(14N,xnp),(~4N,xnd),(~4N,xnt),E=167 MeV; m e a s u r e d T ( p a r t i c l e ) - c o i n , ~-multiplicity,cr(evaporation residue); deduced entrance channel localized fusion L w i n d o w . 15SEr d e d u c e d y r a s t t r a n s i t i o n v - m u l t i p l i c i t y . M a s s i v e t r a n s f e r m o d e l . PRVCA 24 2565. NUCLEAR REACTIONS ~3°Te,ia4Sn(aaS,xn),E=lSO MeV; m e a s u r e d E'y,I3,,linear p o l a r i z a t i o n , T ( 0 ) . 156,~SSEr,'5~,~SaDy d e d u c e d T - m u l t i p o l a r i t y , c o l l e c t i v e v-ray continuum. P u l s e d beam,NaI(T1), Ge(Li) d e t e c t o r s , t h r e e - G e ( L i ) p o l a r i m e t e r , N a I ( T 1 ) a r r a y . NUPAB 378 141.

A t59Dy

AND

=

161

NUCLEAR MOMENTS 15s,lss,16°,Is1,1s2,163,iS4Dy; measured hfs,optical isotope shifts; deduced r m s charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 26 1636.

73

KEY

NUMBERS

A 161Ho

R 82Ha17

J

82C104

R 82Fi15

82IsO5

82Le16

IS~Er

R 83Ro07

i6~Lu

D 82Sc15

tsaHf

D 82Sc15

162 W

D 82Dell

82C104:

R 821s05:

163Ho

D

163Lu

D 82Sc15:

163Hf

D 82Sc15:

ts3 w

D 82Dell:

81Be56:

J

81Ah05: 82C104:

continued

162

=

targets,precision

measurement,He-jet

transport.

163

NUCLEAR MOMENTS 15s,158,ls°,161,ts2,is3,164Dy; m e a s u r e d h f s , o p t i c a l i s o t o p e s h i f t s ; d e d u c e d rms charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 26 1636. NUCLEAR REACTIONS 14a,143,145Nd,155,157Gd,iSl,ls2,164Dy,lS5Ho,l~4,173yb(n,v),E=thermal; m e a s u r e d EV. 143,144,146Nd,156,158Gd,lS2,163,164,I65Dy,166Ho,175,174yb d e d u c e d n e u t r o n s e p a r a t i o n e n e r g y . PRVCA 25 3184. RADIOACTIVITY 163Ho [ f r o m ~62Er(n,-y)lSaEr(fl-decay)]; m e a s u r e d E ( X - r a y ) , l ( X - r a y ) ; d e d u c e d Q(EC) l o w e r l i m i t . PYLBB 167 19. RADIOACTIVITY tsa,lS3Hf [ f r o m 142Nd(24Mg,xn),E=105-133 MeVJ; m e a s u r e d ET,l%Ea,Ia,TV-coin, T1/a. laaHf d e d u c e d r e d u c e d a - w i d t h , Q a , a - b r a n c h i n g , m a s s e x c e s s , a63Lu d e d u c e d l e v e l s , v-branching,-y-multipolarity, i62Lu d e d u c e d l e v e l s , v - b r a n c h i n g . Helium jet,hyperpure Ge, Ge(Li),Si s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 25 3091. RADIOACTIVITY 162,163Hf [ f r o m 142Nd(24Mg,xn),E=105-133 MeVJ; m e a s u r e d E % l % E a , I a , 7 7 - c o i n , T1/2. 16aHf d e d u c e d r e d u c e d a - w i d t h , Q a , a - b r a n c h i n g , m a s s e x c e s s . 163Lu d e d u c e d l e v e l s , v-branching,v-multipolarity. 162Lu d e d u c e d l e v e l s , 7 - b r a n c h i n g . Helium jet,hyperpure Ge, Ge(Li),Si s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 25 3091. RADIOACTIVITY i62,163,164W,166,167,168,169R e,167,16S,lSg,176Os,lSS,169,17°,lTl,17a,1731r,175,176pt, 151Dy,151m,/51,152Ho,i52,153Er,153,154 Tin,154 Y b [ f r o m l°7,1°9Ag,l°S,l l°Cd,113I n,11g,IISSn(63Cu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149.

A 164Dy

=

Ea. E n r i c h e d

A J

161

NUCLEAR MOMENTS 15s,lss,16°,lSl,tSa,ls3,tS4Dy; m e a s u r e d h f s , o p t i c a l i s o t o p e s h i f t s ; d e d u c e d rms charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 26 1636. NUCLEAR REACTIONS lSOGd(a,2n),E=24,28 MeV; m e a s u r e d E(-y),I(-/)(E,t,0),T-Y-coin,ICC. i62Dy deduced levels,K,J,zr. Enriched targets,Ge(Li),hyperpure Ge d e t e c t o r s , m i n i - o r a n g e spectrometer. Two-quasiparticle p l u s r o t o r a n a l y s i s . NUPAB 389 218. NUCLEAR R E A C T I O N S 14a,143,145Nd,lSs,tSTGd,i6i,ls2,164Dy,16SHo,174,t~3yb(n,~,),E=thermal;m e a s u r e d EV. 143,t44,146Nd,lSs,lSSGd,tSa,ls3,164,165Dy,lSSHo,tTs,174Ybd e d u c e d n e u t r o n separation energy. P R V C A 25 3184. NUCLEAR REACTIONS 165Ho,lSiTa(~-,xn),E at r e s t ; m e a s u r e d vn-coin. 16a,lS6,lSS,156,154Dy deduced neutron energy for given multiplicity. PYLBB 114 427. NUCLEAR REACTIONS lss,tSSDy,lS2,tS4Er,lSayb(a,a'),E=12-16 MeV; m e a s u r e d a. zss,iSSDy,lSa,la4Er, 16sYb l e v e l s d e d u c e d B(X). E n r i c h e d t a r g e t s . PRVCA 26 97. RADIOACTIVITY lsz,lS3Hf [ f r o m 142Nd(a4Mg,xn),E=105-133 MeV]; m e a s u r e d Ev,I%Ea,ta,v-y-coin, Tl/2. 16aHf d e d u c e d r e d u c e d a - w i d t h , Q a , a - b r a n c h i n g , m a s s e x c e s s . 163Lu d e d u c e d l e v e l s , 7-branching,v-multipolarity. iSaLu d e d u c e d l e v e l s , v - b r a n c h i n g . Helium jet,hyperpure Ge, Ge(Li),Si s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 25 3091. RADIOACTIVITY lsa,iS3Hf [ f r o m t4~Nd(~4Mg,xn),E=105-133 MeV]; m e a s u r e d E % I % E a , l a , v V - c o i n , Tl/~. 16aHf d e d u c e d r e d u c e d a - w i d t h , Q a , a - b r a n c h i n g , m a s s e x c e s s , lSSLu d e d u c e d l e v e l s , v-branching,v-multipolarity. 16aLu d e d u c e d l e v e l s , v - b r a n c h i n g . Helium jet,hyperpure Ge, Ge(Li),Si s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 35 3091. RADIOACTIVITY 16a,163,164 w,lSS,167,16S,lSgRe,167,168,169,17°Os,lSe,lso,/7°,171,17a,i731r,175,176pt, 151Dy,t51m,iSt,152Ho,152,153Er,153,/54Tm,t54yb [from l°?,l°9Ag,i°8,1 l ° c d , l 13I n,112,116Sn(63C u , X ) , E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d ANPHA 7 149.

163Dy

=

KEYW0RDS

NUCLEAR REACTIONS x s a , t S 4 E r ( p , a ) , E = 1 7 MeV; m e a s u r e d a ( E a ) , a ( 0 ) , i6lHo l e v e l s d e d u c e d normalization f a c t o r s , t59Ho d e d u c e d l e v e l s , J , T r , S , r o t a t i o n a l b a n d s , N i l s s o n a s s i g n m e n t s . Enriched targets. Triton cluster transfer D W B A , C o r i o l i s m i x i n g c a l c u l a t i o n s . ZPAAD 305 143.

A

XSaDy

AND

=

164

NUCLEAR MOMENTS ts4,1S°Dy; m e a s u r e d o p t i c a l i s o t o p e s h i f t s . E n r i c h e d i s o t o p e s , F a b r y - P e r o t spectrometer. I J O P A 19 1183. NUCLEAR MOMENTS 156,15s,16°,161,162,163,1S4Dy; m e a s u r e d h f s , o p t i c a l i s o t o p e s h i f t s ; d e d u c e d rms charge radii differences,hyperfine anomaly,hyperfine constants. Atomic beams,laser s p e c t r o s c o p y . PRVCA 26 1636.

74

KEY

NUMBERS

A ~64Dy

R 821s05

lS4Er

R 81Bo40 82FiO6 82HuO3

82Ro07 164Lu

D 81Br30

164Hf

D 81Br30

164 W

D 82Dell

R 82Is05

=

164

KEYWORDS

continued

NUCLEAR REACTIONS 14a,143,~45Nd,~S5,157Gd,lS~,~sa,lS4Dy,~S5HoJ74,173yb(n,v),E=thermal; measured EV. i43,t44,14SNd,15s,tSSGd,16~,~sa,~s4,1SSDy,~SHo,175,t74Yb deduced neutron separation energy. PRVCA 25 3184. NUCLEAR REACTIONS Is4,~ss,16s,17°Er(n,n'v),E=reactor spectrum; measured EV,Iv. l~4,~7°Er deduced levels,Jjr. IANFA 45 2141. NUCLEAR REACTIONS ISaDy(a,2n),E=24 MeV; measured E%Iv(0,t),~/V-coin. ~S~Er deduced levels, Jjr,K,configurations,band structure. Band mixing analysis. PRVCA 26 290. NUCLEAR REACTIONS 28Si(129Xe,xn),E=720 MeV; 28Si(13SXe,xn),E=740 MeV; measured DSA,E%I V. is4,iSTEr deduced continuum transition T~/a,B(E2),fla,quadrupole moment. Ge(Li),NaI(TI) detectors. ZPAAD 304 335. NUCLEAR REACTIONS Iss,158Dy,lSa,lS4Er,lSsYb(a,a'),E=12-16 MeV; measured a. Is6,15SDy,lSa,lS4Er, i~sYb levels deduced B(;~). Enriched targets. PRVCA 26 97. RADIOACTIVITY is4,16SHf [from 147Sm(aaNe,xn),E=llO,136 MeV3; measured T~/a. 164,1SSLu deduced levels,I V . Chemical separation. RRALA 48 391. RADIOACTIVITY Is4,1SSHf [from t47Sm(aaNe,xn),E=l10,136 MeV]; measured Ti/a. is4,1SSLu deduced levels,I% Chemical separation. R R A L A 48 391. R A D I O A C T I V I T Y 16a,laa,t64 W,l~6,1s7,168,:tSgRe,lS7,168,169,1760s,lSS,169,17°,lTl,172,17a I r,175,t 76p t, 151Dy,151m,t51,152Ho,152,153Er,t 53,154Tm,154 Y b [ f r o m 1°7,1°9A g,l°8,11°Cd,ll3I n,112,116Sn(63C u , X ), E = 2 4 5 - 3 0 0 MeV3; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149.

A

I65Dy

AND

=

165

NUCLEAR REACTIONS 14z,143,t45Nd,155,157Gd,lSl,ls2,164Dy,165Ho,~4,1~3Yb(n,T),E=thermal;

ET. 14a,144,146Nd,15s,~SeGd,lea,163,la4,1S~Dy,lSSHo,175,174yb

~SHo

J

82Bu13

R 82ZuO1

ISSEr

D 82Va20 82Vy03

165Tm

D 82Vy03

R 82AI03

tssyb

D 82Ra19

R 82Ro08

~65Lu

D 81Br30 82Ra19:

~65Hf

D

81Br3O: 82Br15:

~SSTa

D 82Br15:

neutron

separation

measured

energy. PRVCA 25 3184. NUCLEAR MOMENTS ~65Ho; measured hfs; deduced nuclear electric quadrupole moment. ABMR,dye laser. ZPAAD 307 193. NUCLEAR REACTIONS a38U(v,T),E=2.75-6.5 MeV; measured a(O),total G(absorption) vs E; ISITa(v,v),E=3--6.75 MeV; t65Ho(v,v),E=3.5-6.75 MeV; measured total o(absorption) vs E. 23SU, lalTa,'65Ho deduced average y-branching ratio,El transition strength distribution, nonstatistical d e v i a t i o n s f r o m GDR L o r e n t z i a n . N u c l e a r r e s o n a n c e f l u o r e s c e n c e . PYLBB 114 99. R A D I O A C T I V I T Y 'S'W(EC)J~SEr(EC); m e a s u r e d (X-ray)(X-ray)-coin; deduced double K-shell vacancy production. P L R A A 26 2 7 4 9 . R A D I O A C T I V I T Y 165Tm(EC),(fl +) [ f r o m Ta(p,xnyp),E=660 MeV3; m e a s u r e d Efl+,Ifl+,Ev,Iv, (ce)v-eoin; deduced Qfl+,log f t . 16SEr d e d u c e d levels,ICC,J,Tr,v-multipolarity. IANFA 46 834. R A D I O A C T I V I T Y iSSTm(EC),(fl+) [ f r o m Ta(p,xnyp),E=660 MeV]; measured Efl+,tfl+,Ev,Iv, (ee)v-coin; deduced Qfl+,log f t . laSEr d e d u c e d levels,ICC,J,Tr,v-multipolarity. IANFA 46 834. NUCLEAR REACTIONS 141pr,159TbJ6SHo,i67Er,lS9Tm(polarized n,X),E=9.901-100 keV; measured transmission; deduced (7 spin dependence,strength functions. 142pr,lS°Tb,lSSHo,lSeEr,165Tm resonances deduced J. Polarized natural targets,liquid scintillation detector. NUPAB 376 229. R A D I O A C T I V I T Y 165Lu(EC),(fl+) [ f r o m lS~Gd(14N,4n),E=9.6 g e V / n u e l e o n ] ; m e a s u r e d EV,IT,XT-,VV- , ~ + T - c o i n . 165Lu l e v e l d e d u c e d J J r , c o n f i g u r a t i o n . 165yb d e d u c e d l e v e l s , J J r . E n r i c h e d t a r g e t , Ge(LI) d e t e c t o r s . J P H G B 8 1301. NUCLEAR REACTIONS l S a , 1 5 4 S m ( ~ 7 0 , x n ) , ( l S O , x n ) , E = 8 0 - 8 4 MeV; m e a s u r e d VV-coin,v(0),ICC f o l l o w i n g 4,5 n e u t r o n e m i s s i o n . Is5,1s7yb d e d u c e d l e v e l s , J , ~ r , B ( M 1 ) , o n e - , t h r e e - q u a s i n e u t r o n alignments. Enriched targets,Ge(Li) detectors,Nal(T1) array,Compton-suppressed Ge(Li) coincidence,mini-orange spectrometer,Si-Li d e t e c t o r . N U P A B 382 125. R A D I O A C T I V I T Y 164,165Hf [ f r o m 147Sm(aSNe,xn),E=l10,136 MeV3; m e a s u r e d T1/z. 164,165Lu d e d u c e d l e v e l s , I V. C h e m i c a l s e p a r a t i o n . R R A L A 48 391. R A D I O A C T I V I T Y 165Lu(EC),(fl+) [ f r o m lSSGd(14N,4n),E=9.6 M e V / n u c l e o n 3 ; m e a s u r e d EV,I%Xv-,VV-, f l + V - c o i n . 16SLu l e v e l d e d u c e d J , T r , e o n f i g u r a t i o n . l s S y b d e d u c e d l e v e l s , J , ~ . E n r i c h e d t a r g e t , Ge(Li) d e t e c t o r s . J P H G B 8 1301. R A D I O A C T I V I T Y 164,J65Hf [ f r o m 147Sm(aaNe,xn),E=l10,136 MeV]; m e a s u r e d Tl/2. i64,165Lu d e d u c e d l e v e l s , I V. C h e m i c a l s e p a r a t i o n . R R A L A 48 391. R A D I O A C T I V I T Y ~5Ta [ f r o m 151Eu(a°Ne,6n),E=154,164 MeV3; m e a s u r e d ET,IT,TI/~. lSSHf d e d u c e d l e v e l s . R R A L A 51 319. R A D I O A C T I V I T Y tS5Ta [ f r o m 151Eu(a°Ne,6n),E=154,164 MeV3; m e a s u r e d E%Iv,T~/a. 165Hf d e d u c e d l e v e l s . R R A L A 51 319.

75

deduced

KEY

NUMBERS

A

ISSHo

D 81Bu24: 81La37: R 83AI03:

8~De37:

821s05:

16SEr

D 81Bu24: 81La27: J

81Ho31:

~SSTm

R 82E102:

IS~Re

D 82De11:

J

81Ho31:

~67Tm

R 81Io06:

167yb

R 82Ro08:

167Hf

R 81De36: 81Jall:

167Re

D 82Dell:

16VOs

D 83Dell:

82EnO3:

D 82Ge04:

ISeHo

D 82Ge04:

166

=

167

NUCLEAR MOMENTS laSEr; m e a s u r e d Mossbauer effect in ErFe2,ErZn,ErAl 2. 167Er; m e a s u r e d NMR i n E r F e 2 , E r Z n , E r A 1 2 . lSSEr l e v e l d e d u c e d /~. HYIND 11 29. NUCLEAR REACTIONS tSSHo(a,2n),E=26.5 MeV; m e a s u r e d -/(0); d e d u c e d global G a u s s i a n s u b s t a t e population model inadequacy,direct discrete yrast transition f e e d i n g , lSTTm l e v e l s d e d u c e d J. NUIMA 190 19. NUCLEAR REACTIONS 1 2 2 , 1 5 4 S m ( 1 7 0 , x n ) , ( l S O , x n ) , E = 8 0 - 8 4 MeV; m e a s u r e d "YT-coin,T(0),ICC f o l l o w i n g 4,5 n e u t r o n e m i s s i o n . Is5,167yb d e d u c e d l e v e l s , J , ~ r , B ( M 1 ) , o n e - , t h r e e - q u a s i n e u t r o n alignments. Enriched targets,Ge(Li) detectors,Nal(Tl) array,Compton-suppressed Ge(Li) coincidence,mini-orange spectrometer,Si-Li d e t e c t o r . NUPAB 382 125. NUCLEAR REACTIONS 159Tb(14N,5n),(14N,6n),E=95 MeV; m e a s u r e d T T - e n e r g y c o r r e l a t i o n , lsT,lSSHf deduced collective,single particle motion,band c r o s s i n g e f f e c t s . PYLBB 106 480. NUCLEAR REACTIONS i59Tb(I~N,5n),(14N,6n),E=95 MeV; m e a s u r e d "yv(t),T(0). lsv,iSSHf d e d u c e d levels,~-multipolarity,J,zr,yrast,favored,unfavored bands,backbending,band crossing. Compton-suppression spectrometer. PYLBB 106 475. R A D I O A C T I V I T Y 12a i s 3 ts4w,tss,167,t68,lSgRe,tS7,168,169,1700s,lss,169,17o,171,172,173ir,175,176pt ' 121Dy,121m,121,152Ho,12a,123Er,123,124Tm,124yb [from 1°?,1°gAg,i°s,11°Cd,1131n,1Ia,llSSn(SaCu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. Enriched targets,precision m e a s u r e m e n t , H e - j e t transport. ANPHA 7 t49. RADIOACTIVITY 162,163,164w,lSS,lST,lSg,lsgRe,lST,168,169,17°os,lSS,lSS,17°,171,172,1731r,175,176pt, 151Dy,121m,121,122Ho,I52,123Er,lS3,124Tm,154 Y b [ f r o m l°?,l°gAg,l°8,11°Cd,l13I n,l12,116Sn(63Cu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149. RADIOACTIVITY 171,172,173,174pt [ f r o m ~44Sm(32S,xn),E=139.5-201 MeV]; 167,1ss,169,17°Os [ f r o m 171,172,173,174pt a - d e c a y ] ; measured Ea,Ia,Tl/a. 17Opt; m e a s u r e d Ea. 16"y,168,169,17°0s d e d u c e d a-branching. Recoil m a s s s e l e c t o r , t h i n gas A E , s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 25 1830.

A

ISSDy

=

KEYWORDS

RADIOACTIVITY 15SEu,16SHo; m e a s u r e d I(ce). ISSGd,la6Er transitions d e d u c e d subshell ICC ratios. I A N F A 45 2133. RADIOACTIVITY ISaHo; m e a s u r e d ~/~(0),oriented nuclei. IS6Er d e d u c e d T-branching,6,J,vr. Z P A A D 303 331. NUCLEAR R E A C T I O N S 141Pr,lSgTb,165Ho,lSTEr,lSgTm(polarized n,X),E=0.001-100 keV; m e a s u r e d transmission; d e d u c e d a spin dependence,strength functions. 142pr,18°Tb,lS6Ho,lSSEr,lSSTm resonances d e d u c e d J. Polarized natural targets,liquid scintillation detector. N U P A B 376 229. NUCLEAR R E A C T I O N S 16~Er(t,a),E=17 MeV; m e a s u r e d a(e),a(Ea); d e d u c e d optical m o d e l parameters. IS6Ho d e d u c e d levels,L,J,Tr,K,rotational band,Nilsson configurations. D W B A analysis. Z P A A D 397 351. NUCLEAR REACTIONS 142,14a,142Nd,lS2,127Gd,iSi,is2,164Dy,185Ho,174,173Yb(n,T),E=thermal; m e a s u r e d E-y. 143,144,146Nd,156,15BGd,16a,163,lS¢,lSSDy,lSSHo,175,174yb d e d u c e d n e u t r o n separation energy. PRVCA 25 3184. RADIOACTIVITY 15SEu,iSaHo; m e a s u r e d I(ce). 15SGd,lS6Er t r a n s i t i o n s d e d u c e d s u b s h e l l ICC r a t i o s . IANFA 45 2133. RADIOACTIVITY lSSHo; m e a s u r e d T T ( 0 ) , o r i e n t e d n u c l e i . 166Er d e d u c e d T - b r a n c h i n g , 6 , J J r . ZPAAD 303 321. NUCLEAR MOMENTS 16SEr; m e a s u r e d Mossbauer e f f e c t in ErFe2,ErZn,ErA12. l~TEr; m e a s u r e d NMR i n E r F e a , E r Z n , E r A l 2. lSSEr l e v e l d e d u c e d /z. HYIND 11 29. NUCLEAR REACTIONS lS5Ho(a,3n),E ~ 3 4 - 4 6 MeV; m e a s u r e d cr(ET),TT(0),T'F(t),Ev,IT. 16STm deduced levels,~-branching,rotational b a n d s . ZPAAD 305 87. RADIOACTIVITY i~2 1S3 184W,ISS,lST,168,i69Re,lST,Jss,169,1700s,168,lsg,17s,17i,tT~,173ir,175,176pt ' 151DxrJ, 151m ,151 ,152Ho ,122 ,153E~,, 153 ,124rP_m, 154yh_~ [ f r o m 1°7,1°9Ag,1°8,1 l ° c d , l 13I n,112,116Sn(63C u , X ) , E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149.

A 167Er

AND

=

168

RADIOACTIVITY lSaDy [ f r o m aSaCf(SF)]; m e a s u r e d T1/u,ET,IT; d e d u c e d v - e m i s s i o n p r o b a b i l i t y for transition, lSSHo l e v e l s d e d u c e d r e l a t i v e IT. Helium jet rapid chemical separation. ZPAAD 306 363. R A D I O A C T I V I T Y 16aDy [ f r o m aS2cf(SF)]; m e a s u r e d T1/2,ET,I2'; d e d u c e d v - e m i s s i o n p r o b a b i l i t y for transition. 168Ho l e v e l s d e d u c e d r e l a t i v e IT. Helium jet rapid chemical separation. ZPAAD 306 363.

76

KEY

NUMBERS

A ,SeEr

D 81IT04

R 82AI03

168Tm 158yb

D 82Se07 R 82Ro07 82Wa19

16sHf

R 81De36 81Jall

82PelO

:68Re

D 82Dell

,5 50s

D 82Dell

82EnO3

:581r

D 82Dell

169Re

D 82Dell

D 82De11:

82En03:

159ir

D 82Dell:

Ea . E n r i c h e d

R 81Bo40:

170Tin

R 82Ma33:

=

targets,precision

measurement,He-jet

transport.

169

Ea . E n r i c h e d

targets,precision

measurement,He-jet

transport.

RADIOACTIVITY :62,153, 1 5 4 W . 166. 167 . 155 . 169 Re . 157. 165 . 159 . 170 ON . 158. 169. 175 . 171 . 172 . 173 It, : 7 8 , 1 7 5 P t , :5'Dy,'Slm,tS',152Ho,15a,'53Er,'Sa,'54Tm,iS4yb [from l°7,1°SAg,'°s,'l°Cd,l19In,'12,1:SSn(SaCu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea . E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149. R A D I O A C T I V I T Y 17',172,173,174pt [ f r o m 1 4 * s m ( a 2 S , x n ) , E = 1 3 9 . 5 - 2 0 1 MeV3; '67,158,:59,17°0s E f r o m 17,,t72 ,73,174pt a - d e c a y ] ; measured E a , I a , T t / 2 . 170pt; m e a s u r e d E m 157,168,159,17°05 d e d u c e d a-branching. Recoil mass selector,thin gas &E,surface barrier d e t e c t o r s . PRVCA 25 1830. R A D I O A C T I V I T Y 1 6 2 . 1 6 .3 1. 6 4 .W . 1 6 6. 1.6 7 . 1 6.8 1. 6 9 ]. ~ o. 1 6. 7 .1 6 8 1 5 0 1 7 0 ~u s . 1 6 8. 1 6. 9 .1 7 0 . 171. 1.7 2 1 7 3 ] r . 1 7. 5 . l T. S.p f : 5 1 D y , 1 5 1 m , 151 , 1 5 2 Ho, 1 5 2 , 1 5 3 E r , : 5 3 , 1 5 4 T i n , 1 5 4 Y b [from l°7,l°9Ag,l°S,ll°cd,llSIn,l12,116Sn(53Cu,X), E = 2 4 5 - 3 0 0 MeVS; m e a s u r e d Ea . E n r i c h e d targets,precision measurement,He-jet transport. A N P H A 7 149.

A 170Er

continued

NUCLEAR REACTIONS l e ° G d ( 1 6 0 , 4 n ) , ( 1 6 0 , 5 n ) , E = 8 0 , 9 0 MeV; l S ° G d ( l s O , S n ) , ( l s 0 , 7 n ) , E = l 1 0 - 1 3 4 MeV; 1 6 ° G d ( 1 6 0 , 8 n ) , E = 1 2 0 , 1 2 9 , 1 3 4 MeV; m e a s u r e d E 7 , I 7 . 17z,171,17°,:69,168Hf t r a n s i t i o n s deduced average v-multiplicity,width distribution. I A N F A 46 1431. R A D I O A C T I V I T Y 162 . 1 6 3. : 6 4. w . , s s. 167 . ,65 15eRe . ,57. 165 . . 155 17005 . 155. 1 .5 9 :.7 5 . 171. ,7z , 7 3 i r , : 7 5 , 1 7 5 p t , 15,Dy 151m ,51 152Ho 152 , S e E r ,53 154Tin l s 4 y b [from l°7,'09Ag,l°S,lioCd,i13In,l:2,116Sn(63Cu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d A N P H A 7 149.

:5905

168

E = 2 4 5 - 3 0 0 MeVJ; m e a s u r e d Ea . E n r i c h e d targets,precision measurement,He-jet transport. ANPHA 7 149. R A D I O A C T I V I T Y 171,172,173,174pt I f t o r n 1 4 4 S m ( a Z S , x n ) , E = 1 3 9 . 5 - 2 0 1 MeV]; 1 6 7 , : 5 5 , 1 6 9 , 1 7 5 0 S [ f r o m 171 172 1 7 3 , 1 7 4 p t a - d e c a y ] ; measured E a , l a , T 1 / 2 . 17~Pt; m e a s u r e d Ea. 157,165,169,17805 d e d u c e d a-branching. Recoil mass selector,thin gas AE,surface barrier d e t e c t o r s . PRVCA 25 1830. R A D I O A C T I V I T Y ••2•:63•••4W•••6••67••••••••Re•••7••68•••9••7•••'•6••••9••••••7•••72••7••r••7•••7•Pt• 151Dy,lSlm,tS',lS2Ho,'S2,153Er,lSa,i54Tm,:Sdyb [from 157,t°SAg,taa,ttaCd,:taln,tt2,:tSSn(SUCu,X),

A R 82Pe10

=

KEYWORDS

R A D I O A C T I V I T Y laSEr [ f r o m 158Tm e l e c t r o n c a p t u r e d e c a y 9 ; m e a s u r e d Y T ( 0 ) , y y ( 0 , t ) , o r i e n t e d n u c l e i . 'SeEr t r a n s i t i o n s deduced d,transition probability. J U P S A 50 3191. NUCLEAR REACTIONS 1 4 1 p r , ' 5 9 T b , i 5 5 H o , l S T E r , i 6 9 T m ( p o l a r i z e d n , X ) , E = 0 . 9 0 1 - I 0 0 k e V ; m e a s u r e d transmission; deduced a spin dependence,strength functions. 142pr,16°Tb,165Ho,'65Er,155Tm resonances d e d u c e d J. P o l a r i z e d n a t u r a l targets,liquid scintillation d e t e c t o r . NUPAB 376 229. R A D I O A C T I V I T Y 168Tm(EC); m e a s u r e d E % I T , E ( X - r a y ) , l ( X - r a y ) ; d e d u c e d Q(EC). IANFA 46 944. NUCLEAR REACTIONS '56,'55Dy,i82,154Er,iSsyb(a,a'),E=12-16 MeV; m e a s u r e d (7. 155,:58Dy,182,'54Er, 168yb l e v e l s d e d u c e d B(X). E n r i c h e d t a r g e t s . PRVCA 26 97. NUCLEAR REACTIONS ' 5 5 E r ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) . 168Yb d e d u c e d l e v e l s , J , r r , 7-branching,(g(k)-g(R)),band structure. PYLBB 116 393. NUCLEAR REACTIONS 159Tb(14N,5n),(14N,Sn),E=95 MeV; m e a s u r e d 7 7 - e n e r g y c o r r e l a t i o n . 157,-'58Hf deduced collective,single particle motion,band c r o s s i n g e f f e c t s . PYLBB 106 4 8 0 . NUCLEAR REACTIONS 159Tb(:aN,5n),(i4N,6n),E=95 MeV; m e a s u r e d 7 7 ( t ) , y ( 0 ) . 157,'58Hf d e d u c e d levels,7-multipolarity,J,rr,yrast,favored,unfavored bands,backbending,band crossing. Compton-suppression spectrometer. PYLBB 106 475. NUCLEAR REACTIONS ' 5 5 G d ( i 5 0 , 4 n ) , ( : 8 0 , 5 n ) , E = 8 0 , 9 0 MeV; t S O G d ( i e 0 , 6 n ) , ( l s O , T n ) , E = l 1 0 - 1 3 4 MeV; 1 8 ° G d ( 1 5 0 , 8 n ) , E = 1 2 0 , 1 2 9 , 1 3 4 MeV; m e a s u r e d E % I y . 172,i71,178,169,168Hf transitions deduced average 7-multiplicity,width distribution. I A N F A 46 1431. R A D I O A C T I V I T Y 152: 63 164W 166,157,165,169Re,167,158,169,1760s,168 169,179,:71,172,173Ir,:TS,175pt ' :5:Dy,lSlm,15','S2Ho,lSa,153Er,'53,'54Tm,154yb [from :57,'99Ag,lOs,:toCd,l19In,1'a,'lSSn(63Cu,X), E = 2 4 5 - 3 0 0 MeV9; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet -transport. A N P H A 7 149. R A D I O A C T I V I T Y ,52 153 ~54 w 155 157 too ,69R e ,67 1 6 8 : 5 9 1700¢ ,68 , 5 9 : 7 0 171 172 1731~ 175 176D÷ 151Dy,/Slrn,15:,lS2Ho,152,lSaEr,153,154Tm,154 Yb [ f r o m l°7,:09Ag,l°8,liOcd,llaln,tla,ilSSn(63Cu,X),

E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d A N P H A 7 149.

169Hf

AND

=

170

NUCLEAR REACTIONS 1 6 4 , I s s , 1 6 8 , 1 7 ° E r ( n , n ' ~ / ) , E = r e a c t o r s p e c t r u m ; measured E 7 , I 7 . le4,~V°Er deduced l e v e l s , J , T r . I A N F A 4 5 2141. NUCLEAR REACTIONS lSQTm(n,7),E=3-2000 keV; m e a s u r e d a ( c a p t u r e ) . IV°Tin d e d u c e d r e s o n a n c e s , parameters,s-,p-,d-wave strength functions. NSENA 82 143.

77

KEY

NUMBERS

A 17OHf

R

17O0s

D 82Dell

82Pe10:

82En03

17Olr

179pt

D 82Dell

D

82En03

R 82Kr03

171Hf

R 82PelO

171ir

D 82Dell

17'~pt

D 82En03

R 82PelO:

'7206

R 82Du13:

17"air

D

82Dell:

170

continued

E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea . E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. A N P H A 7 149. R A D I O A C T I V I T Y 17',17a,t73,17'4Pt [ f r o m 1 4 4 S m ( a 2 S , x n ) , E = I 3 9 . 5 - 2 0 1 MeV]; 197,198,199,1700S [ f r o m 171,17a,173,t74pt a - d e c a y ] ; measured Ea,Ia,T1/a. 179pt; m e a s u r e d Ea . 187,168,169,17'90S d e d u c e d a-branching. Recoil mass selector,thin gas AE,surface barrier d e t e c t o r s . PRVCA 25 1830. R A D I O A C T I V I T Y ••2••63•164W•••••167•••••169Re••67••••••69•17•••'1•••169•17•••7"•••72••73Ir••75 •7"6Pt• 1SlDy,lSlm,lsl,lSaHo,lSz,iSaEr,lSa,154Tm,154yb [from l°7',199Ag,196,n°Cd,naln,l12,119Sn(6aCu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d targets,precision measurement,He-jet transport. ANPHA 7 149. R A D I O A C T I V I T Y 171,176,173,17'4pt [ f r o m 144Sm(a~S,xn),E=139.5-201 MeV]; 197 166 169,1790s [ f r o m 171 17'2 173,174pt ~ - d e c a y ] ; measured Ea,la,Tl/a. 179pt; measured Ea. 197,198,169,1790S d e d u c e d a-branching. Recoil mass selector,thin gas AE,surface barrier d e t e c t o r s . PRVCA 25 1830.

=

171

NUCLEAR REACTIONS 179Er(190,150),E=lE0 MeV; m e a s u r e d i S O v - c o i n , G ( E ( 1 5 0 ) ) . 171Er d e d u c e d levels,-/-branching,K-mixing. Q3D s p e c t r o m e t e r . Q u a s i p a r t i e l e p l u s r o t o r m o d e l . PRVCA 25 866. NUCLEAR REACTIONS 16°Gd(190,4n),(190,5n),E=80,90 MeV; 1 9 O G d ( 1 6 0 , 6 n ) , ( l ° 0 , 7 n ) , E = l 1 0 - 1 3 4 MeV; 1 9 9 G d ( 1 6 0 , 8 n ) , E = 1 2 0 , 1 E 9 , 1 3 4 MeV; m e a s u r e d E-/,Iv. 17a,171,178,169,188Hf transitions deduced average -/-multiplicity,width distribution. ]A N P A 46 1431. R A D I O A C T I V I T Y 162 , 193 , 194 W . 199 . 197 . . 169 199 Re . 167 . 198 . . 199 170 Os . 168. 1fl9 . 179 . . 171. 172 173 I t , 175 , 176 P t , 151Dy,lSlm,151,1SaHo,15z,15aEr,15a,154Tm,lS4yb [ f r o m 197,199Ag,19a,ll°Cd,llaln,l12,119Sn(63Cu,X), E = 2 4 5 - 3 0 0 MeV]; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n measurement,He-jet transport. ANPHA 7 149. R A D I O A C T I V I T Y 17'1,17'2,173,174pt [ f r o m 1 4 4 S m ( a a S , x n ) , E = 1 3 9 . 5 - 2 0 1 MeV]; 167,168,169,17'90S [ f r o m 17'1 172,173,17'4pt a - d e c a y ] ; measured Ea,la,Tl/2. 17'°Pt; m e a s u r e d Ea. 167,168,169,1790s d e d u c e d a-branching. Recoil mass selector,thin gas AE,surface barrier d e t e c t o r s . PRVCA 35 1830.

A 172Hf

=

NUCLEAR REACTIONS l ° S G d ( l s O , 4 n ) , ( 1 6 0 , 5 n ) , E = 8 0 , 9 0 MeV; 1 9 ° G d ( 1 6 0 , S n ) , ( 1 6 0 , 7 n ) , E = l 1 0 - 1 3 4 MeV; l ° ° G d ( 1 6 0 , 8 n ) , E = 1 2 0 , 1 3 9 , 1 3 4 MeV; m e a s u r e d E-/,I~/. 172,17",17'°,189,168Hf transitions deduced average v-multiplicity,width distribution. I A N F A 46 1431. R A D I O A C T I V I T Y 162 . 163. 164 . w . 196. 167 . 18s 199Re . 167 . 168 . . 169 1700s . 166. 169 . 170 . . 171. 172 173ir,17'5,176pt, 151D y, 151rn ,151 , t52Ho, 15Z ,153EF ,153 ,154Tm , I 5 4 y b [ f r o m 197,1°9Ag,19a,119Cd,1131 n , 1 1 2 , 1 1 6 S n ( g a c u , X ) ,

A 17'IEr

AND KEYWORDS

=

17E

NUCLEAR REACTIONS 16°Gd(160,4n),(160,5n),E=80,90 MeV; 1 6 ° G d ( 1 6 0 , 6 n ) , ( " 6 0 , 7 n ) , E = l 1 0 - 1 3 4 MeV; l S ° G d ( 1 6 0 , S n ) , E = 1 2 0 , 1 2 9 , 1 3 4 MeV; m e a s u r e d E-/,I V. 172,171,17'°,199,i68Hf transitions deduced average -/-multiplicity,width distribution. I A N F A 46 1431. NUCLEAR REACTIONS 14SSm(~SSi,4n),E=145 MeV; 158Sm(aSSi,4n),E=138 MeV; m e a s u r e d T - / - c o i n , -/(0). 17'a,1740s d e d u c e d levels,J,~r,yrast band,band crossing characteristics differences. PYLBB 115 367. R A D I O A C T I V I T Y ••2••63••64W••66••67"•168•••9Re•1•7••6••1•9••79•••••8•169••79•17•••7••173•r•17••176Pt• 151Dy,lSlm,151,15aHo,lS2,153Er,193,154Tm,154yb [ f r o m 197,1°9Ag,1°8,119Cd,tlaln,lla,116Sn(Sacu,X),

E=245-300 MeV]; m e a s u r e d Ea. Enriched targets,precision m e a s u r e m e n t , H e - j e t t r a n s p o r t , ANPHA 7 149. 17apt

D

82En03:

R A D I O A C T I V I T Y 171 176,173,17'¢pt [ f r o m 1 4 4 S m ( a a S , x n ) , E = 1 3 9 . 5 - 3 0 1 MeV]; 167',169,169,17°0s [ f r o m 171 17'a 173174pt a - d e c a y ] ; measured E a , I a , T l / 2 . 17°pt; m e a s u r e d Ea . 107,198,169,1790S d e d u c e d a-branching. Recoil mass selector,thin gas AE,surface barrier d e t e c t o r s . PRVCA 25 1830.

A 17'3yb

D 82Bu16:

173Lu

D 82Bu16:

17air

D 82Dell:

=

173

R A D I O A C T I V I T Y 17ULu(EC) [ f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d TT(0),-/(ce)(0). 17'3Yb l e v e l s deduced T-branching,-/ multipolarity,6. Quasiparticle plus phonon model,Coriolis interaction. RRPQA 27 143. R A D I O A C T I V I T Y 173Lu(EC) [ f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d V-/(0),v(ce)(0 ). 173yb l e v e l s deduced -/-branching,-/ multipolarity,5. Quasiparticle plus phonon model,Coriolis interaction. RRPQA 27 143. R A D I O A C T I V I T Y 16a 163,1641~],ls6,167,16s,169Re,167,168 169 1700s,168,169,170,171,172 1 7 3 i r , 1 7 5 , 1 7 6 p t ' 151Dy,lSlm,lS1,15ZHo,15a,lSaEr,153,154Tm,154yb [ f r o m i°7',1°SAg,1°s,11°Cd,ilaln,lla,llSSn(SaCu,X),

E=245-300 MeV]; m e a s u r e d Ea. Enriched targets,precision m e a s u r e m e n t , H e - j e t t r a n s p o r t . ANPHA 7 149.

78

KEY

NUMBERS

A IVapt

D 82En03:

R 82Is05:

82Sh04:

~74Lu

R 81Do14:

1740S

R 82Du13:

174pt

D 82En03:

R 821s05:

173

continued

=

MeV]; 167,168,169,1760S [ f r o m Ea. ~6~ ~68 ~eg~70Os d e d u c e d d e t e c t o r s . PRVCA a5 1830.

174

NUCLEAR REACTIONS ~4a,t43,145Nd,iSs,~57Gd,~Si,162,~64Dy,165Ho,174,tTayb(n,7),E=thermal; m e a s u r e d ET. ~43,~4,1~6Nd,~Ss,tSSGd,~a2,~63,t64,1eSDY,16eHo,t75,~v4Yb deduced n e u t r o n separation energy. PRVCA 25 3184. NUCLEAR REACTIONS t73yb(n,-},),E=0.01-0.86 keV; m e a s u r e d E7,I7. 1 7 4 y b d e d u c e d r e s o n a n c e s , J , FT,eorrelations,neutron separation energy. Enriched t a r g e t , G e ( L i ) d e t e c t o r . PRVCA 25 1283. NUCLEAR REACTIONS 176Yb(p,3n),E n o t given; m e a s u r e d E7,I7. ~74Lu d e d u c e d l e v e l s , m u l t i p l e t structure. Bent crystal spectrometer. HPACA 54 32,8. NUCLEAR REACTIONS ~48Sm(a°Si,4n),E=145 MeV; ~5°Sm(aeSi,4n),E=138 MeV; m e a s u r e d 7 7 - c o i n , 7(0). ~v~,t~40s d e d u c e d levels,J,rr,yrast b a n d , b a n d c r o s s i n g c h a r a c t e r i s t i c s differences. PYLBB 115 367. RADIOACTIVITY t~,17a,~Ta,174pt [ f r o m ~ 4 S m ( a 2 S , x n ) , E = 1 3 9 . 5 - 2 0 1 MeV]; ~67,168,~eg,~7°Os [ f r o m 171,172,173,174pt a - d e c a y ] ; measured Ea,Ia,Ti/a. 17°Pt; m e a s u r e d Ea. ~s7 168 t69 t T a O s d e d u c e d a-branching. Recoil m a s s s e l e c t o r , t h i n gas A E , s u r f a c e b a r r i e r d e t e c t o r s . PRVCA 25 1830.

A

~syb

=

KEYWORDS

R A D I O A C T I V I T Y ~Tl,tva,lva,~74pt [ f r o m t 4 4 S m ( a a S , x n ) , E = 1 3 9 . 5 - 2 0 1 171,17~,173,174pt a - d e c a y ] ; measured Ea,Ia,Tt/a. ~ ° P t ; m e a s u r e d a-branching. Recoil m a s s s e l e c t o r , t h i n gas A E , s u r f a c e b a r r i e r

A tv4yb

AND

=

175

NUCLEAR REACTIONS 14a,14a,145Nd,15s,157Gd,te~,te~,~e4Dy,tSaHo,t~4,1~ayb(n,7),E=thermal; m e a s u r e d neutron separation energy. PRVCA 25 3184. NUCLEAR REACTIONS i74,~76Yb(a,xn),E=27 MeV; m e a s u r e d E 7 , I 7 , a 7 ( t ) . tv5,~76,~77,~TSHf l e v e l s deduced T~/a,B(X ). E n r i c h e d targets,Ge detectors. Nilsson plus pairing calculations. NUPAB 376 451. RADIOACTIVITY ~ 6 ~ , ~ 6 3 , ~ 6 4 W ~ 6 6 ~ 7 ~ 6 ~ , ~ e 9 R e ~ 6 ~ 6 ~ t 6 ~ s ~ 6 9 , ~ 7 ~ t 7 a ~ r , ~ 7 5 ~ 7 e ~ t ~ t 51Dy,lS~m,~S~,lSZHo,iSa,153Er,lSa,lS4Tm,154Y b [ f r o m t67,169Ag,~°8,~ toed,113I n , l t a , l ~ S S n ( 6 3 C u , X ) , E = 2 4 5 - 3 0 0 MeV3; m e a s u r e d Ea. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149.

ET. 143,144,146Nd,156,158Gd,16a,163,~64,~65Dy,166Ho,175,174yb d e d u c e d 175Hf

R 82Ko08:

175pt

D 82De11:

A lVSLu 176Hf

D 82Sg01: R 82Ko08:

~760s

R 82Bl19:

82Dr03:

176pt

D 82Bo04:

8~Deil

R 81St28

177Hf

R 82Ko08

176

R A D I O A C T I V I T Y 176Lu; measured E T , I 7 , 7 7 - c o i n , T 1 / a . CJPHA 60 361. NUCLEAR REACTIONS t74,176Yb(a,xn),E=27 MeV; m e a s u r e d ET,17,aT(t). t75,t76,t77,tTaHf l e v e l s deduced T1/a,B(X). E n r i c h e d targets,Ge detectors. Nilsson plus pairing calculations. NUPAB 376 451. NUCLEAR REACTIONS ~2°,laaSn(SeFe,X),E=330-456 MeV; m e a s u r e d o r ( e v a p o r a t i o n r e s i d u e 0), or(fragment 0) v s m a s s ; d e d u c e d s t a t i s t i c a l f i s s i o n d e c a y y i e l d l i m i t , t760s d e d u c e d fission barrier v s J. PRVCA 26 1471. NUCLEAR REACTIONS 164,166,168Er(lSO,4n),E=80-105 MeV; m e a s u r e d g ( E , 0 ) , 7 7 - c o i n , 7 7 ( t ) . 1761x8 t860s d e d u c e d l e v e l s , J j r , T , r o t a t i o n a l b a n d s , I C C , la°Os d e d u c e d i s o m e r , c o n f i g u r a t i o n . Ge, Ge(Li),Compton-suppressed d e t e c t o r . B a n d - m i x i n g c a l c u l a t i o n s . NUPAB 383 119. RADIOACTIVITY

156••5•Dy•151••51m•t••••5•mH••15a•15•Er•••••154•154rnTm••79••7•••77•176•t•••5Yb••••,197rn•

19Qmpo,ataFr,ZXZRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,Tl/a. 149Tb,SU,a14,zls,als,eiTAt, a64,ais,a19Fr,alt,atlrn,~la,ala,a~4po,atT,alaRn [from U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941. RADIOACTIVITY 16a 163,164~r,166,167,168,169Re,167,t68,t69 t70Os,t68,t69,170,t71,172 1 7 3 i r , l T S , t 7 6 p t ' 151Dy,lSlm,lSl,tSaHo,t52,153Er,iSa,154Tm,154yb [ f r o m 167,1°gAg,l°a,ll°Cd,llaIn,na,l16Sn(eaCu,X), E = ~ 4 5 - 3 0 0 MeV3; m e a s u r e d Ec~. E n r i c h e d t a r g e t s , p r e c i s i o n m e a s u r e m e n t , H e - j e t transport. ANPHA 7 149.

A 1:77Lu

=

=

177

NUCLEAR REACTIONS 1 7 6 L u ( n , 7 ) , E = t h e r m a l ; m e a s u r e d 7 7 ( t ) . 177Lu d e d u c e d i s o m e r f e e d i n g , rotational band transitions. Ge(Li),NaI(TI) s c i n t i l l a t i o n d e t e c t o r s . FZKAA 13 43. NUCLEAR REACTIONS 174,176Yb(a,xn),E-27 MeV; m e a s u r e d ET,lT,aT(t). tvs,~76,1v7,17OHf l e v e l s deduced Tt/a,B(X ). E n r i c h e d targets,Ge detectors. Nilsson plus pairing calculations. NUPAB 376 451.

79

KEY

NUMBERS

A ~77Ta

R 82Ao0~:

82Ao04:

177pt

D 82Bo04:

R 82ZuO~:

17SHf

D 82Ve08: R 82Ha25:

82Ko08:

R 82Dr03:

*~8pt

D 82Bo04:

D 82Ki04:

179Lu

D 82Ki04:

179Hf

R 82Be47:

179Ta

R 82Ba21: 82WalO:

179pt

D 82Bo04:

R

82Be47:

continued

=

178

=

179

R A D I O A C T I V I T Y 179yb,iSi,iSaLu [ f r o m W,Ta(tSSXe,X),E=9 M e V / n u c l e o n , m a s s s e p a r a t i o n S ; measured ET,IT,77-,Tfl-coin,T1/a; deduced l o g f t . *~9Lu,lSl,lSZHf d e d u c e d levels,J,w. Plastic scintillator,Ge(Li) d e t e c t o r s . N U P A B 378 5 4 9 . R A D I O A C T I V I T Y 179yb,lSi,iS2Lu [ f r o m W,Ta(136Xe,X),E=9 M e V / n u c l e o n , m a s s separation]; measured ET,IT,77-,Tfl-coin,T1/a; deduced log f t . i 7 9 L u , l S t , i S 2 H f d e d u c e d levels,J,rr. Plastic scintillator,Ge(Li) d e t e c t o r s . N U P A B 378 5 4 9 . NUCLEAR REACTIONS i T s , 1 7 9 , 1 a ° H f ( n , 7 ) , E = 2 . 6 - 2 0 0 0 k e V ; m e a s u r e d a t E ) ; d e d u c e d iS°Ta s - , r-process nueleosynthesis, i~°Hf d e d u c e d parameters,strength functions,average level spacings,r-process a b u n d a n c e . 179,tStHf deduced r e s o n a n c e p a r a m e t e r s , s t r e n g t h functions, average level spacings. Maxwellian averaging procedure. P R V C A 26 1 4 0 4 . NUCLEAR REACTIONS / 7 6 y b ( T L i , 4 n ) , E = 3 5 - 4 5 MeV; m e a s u r e d ET,17,a(ET,07,E),77(t),~LiT(t). 179Ta d e d u c e d levels,Jjr,Ti/a,(g(K)-g(R)),ICC. E n r i c h e d t a r g e t s . N U P A B 379 20'5. NUCLEAR REACTIONS l a i T a ( p , t ) , E = 1 9 MeV; m e a s u r e d a(0),a(Et). 17STa d e d u c e d levels,L, tentative J,rr,rotational b a n d . DWBA a n a l y s i s . P R V C A 25 2353. R A D I O A C T I V I T Y •5•••5•Dy••5•••5•m••52•I52rnH•••52••53Er••53••54••54mTm••79•178••77•••6P•••55Yb••98•197rn• 199mpo,213Fr,212Ra [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,Ti/2. 14gTb,an,zl4,zls,ais,elTAt, 2°4,21s,219Fr,211,211m,21a,213,214Po,217,218Rn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A lSOHf

177

NUCLEAR REACTIONS 1 7 a y b ( t , p ) , E = 1 5 MeV; m e a s u r e d a ( E p ) , a ( 0 ) ; d e d u c e d Q. 17syb d e d u c e d levels,L,J,Tr,band structure. Magnetic spectrograph. DWBA a n a l y s i s . P R V C A 26 965. R A D I O A C T I V I T Y 17smHf(IT); m e a s u r e d I7 f o r A J = l t r a n s i t i o n s ; deduced 17 f o r & J = 2 transitions,total intensities. Anti-Compton spectrometer,ICC d a t a i n p u t . NUIMA 201 531. NUCLEAR REACTIONS 17s,ls°Hf(saKr,S6Kr%(136Xe,lSSXe'),E=384-594 MeV; 17aHf(136Xe,136Xe'),E=628, 652,68~ MeV; m e a s u r e d ET,lT,Coulomb excitation,recoil,Doppler broadening, tTs,ia°Hf l e v e l s deduced Tl/2,moment o f i n e r t i a . ~TSHf d e d u c e d i s o m e r e x c i t a t i o n . Cranked shell model calculations. PYLBB 112 327. NUCLEAR REACTIONS 1 7 4 , 1 7 6 y b ( a , x n ) , E = 2 7 MeV; m e a s u r e d E T , I T , a T ( t ) . 17s,176,177,178Hf l e v e l s deduced TI/a,B(X ). E n r i c h e d targets,Ge detectors. Nilsson plus pairing calculations. N U P A B 376 451. NUCLEAR REACTIONS *64,16s,iSSEr(~60,4n),E=SO-105 MeV; m e a s u r e d a ( E , 0 ) , 7 7 - c o i n , 7 7 ( t ) . 1761~ *8°Os d e d u c e d levels,Jjr,T,rotational b a n d s , I C C , ia°Os d e d u c e d isomer,configuration. Ge, Ge(Li),Compton-suppressed detector. Band-mixing calculations. N U P A B 383 119. R A D I O A C T I V I T Y ~15~Dy~51~5~m~2mH~5~53Er~53~5~mTm~7~7~77~76Pt~5~Yb~98~7rn~ 199mpo,~13Fr,21ZRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,TI/2. 149Tb,all,~l¢,215,~lS,~17At, z°4,21s,a*OFr,aU,enm,e~a,zi3,Zt4Po,alv,a~SRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeVS; m e a s u r e d E~. H e l i u m j e t r e c o i l product s e p a r a t i o n . P R V C A 25 941.

A

~7~yb

=

KEYWORDS

NUCLEAR REACTIONS *TSLu(a,2n),E=29.5 MeV; m e a s u r e d 7(0),E7,I7,I7(0=90°,9); d e d u c e d l i n e a r polarization mixing coefficient. 177Ta t r a n s i t i o n deduced ~(E2/MI). l°spd(a,xn),E=31.5 MeV; m e a s u r e d E7,I7. S u m - c o i n c i d e n c e technique,high polarization sensitivity,detection efficiency. NUIMA 196 421. NUCLEAR REACTIONS 1 7 5 L u ( a , 2 n ) , E = 2 9 . 5 MeV; m e a s u r e d ET,17,a(ET,0),77-coin,77(t),linear polarization,l(ce). 177Ta d e d u c e d l e v e l s , J , T r , ~ , T l / ~ , # , B ( M 1 ) , B ( E 2 ). Natural target,Ge(Li) detectors,SJ-Li d e t e c t o r . N U P A B 381 13. RADIOACTIVITY ~5~5~Dy~5~m~52~52mH~5~53Er~5~54~4mTm~79~78~77~7~t~55Yb~98~97ra~ l~mPo,~iSFr,aleRa [from U , T h , A u , T a ( p , X ) , E = 5 GeVS; m e a s u r e d E a , T t / z . l*gTb,ati,~*4,zts,zis,al7At, a°4,eis,atgFr,~U,eUm,Zie,zls,e~*Po,at7,~lSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A ~Tsyb

AND

=

180

NUCLEAR REACTIONS i t s * 7 9 , 1 e O H f ( n , 7 ) , E = 2 . 6 _ 2 0 0 0 k e V ; m e a s u r e d o(E); d e d u c e d la°Ta s - , r-process nucleosynthesis. 18°Hf d e d u c e d parameters,strength functions,average level spacings,r-process abundance. 17S,lSiHf d e d u c e d r e s o n a n c e p a r a m e t e r s , s t r e n g t h functions, average level spacings. Maxwellian averaging procedure. P R V C A 26 1 4 0 4 .

80

KEY

NUMBERS

A laOHf

R 82Ha25:

~86 W

D 8lAy04:

~8OOs

D 82Ne01: R

82Dr03:

D 82Ki04:

~SIHf

D 82Ki04:

R 82Be47:

t~tTa

R 81Zi02 82Zu01

181W

D 82Va20

~S~Os

R 82Li04

D 8SKi04

182Hf

D

taZOs

R 82Fa01

82Ki04

82Li04

D 81Av04 J 81Rull

continued

=

181

=

182

RADIOACTIVITY 179yb,tSl,lB2Lu [ f r o m W,Ta(13SXe,X),E=9 M e V / n u c l e o n , m a s s separation3; measured ET,IT,77-,Tfl-coin,Tl/2; deduced log f t . 179Lu,lel,iS2Hf d e d u c e d levels,J,Tr. P l a s t i c s c i n t i l l a t o r , G e ( L i ) d e t e c t o r s . NUPAB 378 549. RADIOACTIVITY 179Yb,JSl,lS2Lu [ f r o m W,Ta(t36Xe,X),E=9 M e Y / n u c l e o n , m a s s separation]; measured ET,I-y,-/7-,~fl-coin,T1/2; deduced log f t . ~79Lu,~Sl,lSZHf d e d u c e d levels,J,~. P l a s t i c s c i n t i l l a t o r , G e ( L i ) d e t e c t o r s . NUPAB 378 549. NUCLEAR REACTIONS 17°Er(tgO,4n),E=81 MeV; 17°Er(160,5n),E=96 MeV; m e a s u r e d E%I%~7(t),7(0), ICC. 1820s d e d u c e d levels,J,vr,rotational bands. Oe,Ge(Li) d e t e c t o r s , e n r i c h e d targets. NUPAB 375 263. NUCLEAR REACTIONS 168Er(~SO,xnT),E=81 MeV; m e a s u r e d E%I%a(ET,0),77-coin,I(ce) f o r x=4,5. 181,1820s d e d u c e d levels,J,~,ICC,8,7-branching. Enriched t a r g e t s , G e ( L i ) , S i - L i a n d NaI(T1) detectors,mini--orange conversion electron spectrometer. NUPAB 375 291.

A 183Re

180

RADIOACTIVITY 179Yb,'al,taaLu [ f r o m W,Ta(136Xe,X),E=9 M e V / n u c l e o n , m a s s separationJ; measured ET,IT,77-,'yfl-eoin,T~/z; deduced log f t . l~gLu,tal,~aaHf d e d u c e d levels,J,~r. P l a s t i c s c i n t i l l a t o r , G e ( L i ) d e t e c t o r s . NUPAB 378 549. RADIOACTIVITY ~79Yb,ial,~aaLu [ f r o m W,Ta(la6xe,X),E=9 M e V / n u c l e o n , m a s s separation]; measured ET,IT,vT-,-yfl-coin,Tt/z; deduced log f t . 179Lu,~el,18aHf d e d u c e d levels,J,~r. P l a s t i c s e i n t i l l a t o r , G e ( L i ) d e t e c t o r s . NUPAB 378 549. NUCLEAR REACTIONS ~T8,~79,1S°Hf(n,*/),E=2.6-2000 keV; m e a s u r e d or(E); d e d u c e d iS°Ta s - , r-process nucleosynthesis. ~S°Hf d e d u c e d parameters,strength functions,average levei spacings,r-process abundance. ~,'SlHf deduced resonance parameters,strength functions, a v e r a g e l e v e l s p a c i n g s . M a x w e l l i a n a v e r a g i n g p r o c e d u r e . PRVCA 26 1404. NUCLEAR REACTIONS ~S~Ta(7,7),E=6.2 MeV; m e a s u r e d M o s s b a u e r s p e c t r a . ~8~Ta t r a n s i t i o n d e d u c e d i s o m e r s h i f t . C u b i c Cu3TaS 4 s a m p l e . PYLAA 87 130. NUCLEAR REACTIONS a a a u ( % 7 ) , E = ~ . 7 5 - 6 . 5 MeV; m e a s u r e d (~(0),total ( ~ ( a b s o r p t i o n ) v s E; ~ 8 ' T a ( v , 7 ) , E = 3 - 6 . 7 5 MeV; ~gSHo(7,~),E=3.5-6.75 MeV; m e a s u r e d t o t a l i f ( a b s o r p t i o n ) v s E. a38U, ~8ITa,t65Ho d e d u c e d average 7-branching ratio,El transition strength distribution, n o n s t a t i s t i c a l d e v i a t i o n s f r o m GDR L o r e n t z i a n . N u c l e a r r e s o n a n c e f l u o r e s c e n c e . PYLBB 114 99. RADIOACTIVITY ~mW(EC),~gSEr(EC); m e a s u r e d ( X - r a y ) ( X - r a y ) - c o i n ; deduced double K-shell vacancy production. PLRAA 26 2749. NUCLEAR REACTIONS ~eSEr(~80,xnq0,E=81 MeV; m e a s u r e d E%l%(~(E%0),7-/-coin,I(ce) f o r x=4,5. ts~,~SaOs d e d u c e d levels,J,rr,ICC,6,~/-branching. Enriched t a r g e t s , G e ( L i ) , S i - L i a n d NaI(Tl) detectors,mini-orange conversion electron spectrometer. NUPAB 375 291.

A tSaLu

=

KEYWORDS

NUCLEAR REACTIONS ~78,~80Hf(SOKr,sgKr'),(136Xe,t36Xe'),E=384-594 MeV; t78Hf(13SXe,tSeXe'),E=628, 652,682 MeV; m e a s u r e d E % I % C o u l o m b e x c i t a t i o n , r e c o i l , D o p p l e r b r o a d e n i n g . ~T8,18°Hf l e v e l s deduced Twz,moment of inertia. 178Hf deduced isomer excitation. Cranked shell model calculations. PYLBB i12 327. RADIOACTIVITY '83mRe,~86mw [ f r o m ~mTa(a,3n),~eZW((~,t),~Hf(a,n),E=31 MeV]; measured E7,17, T~/a; deduced 7 - b r a n c h i n g . Enriched target,Ge(Li) detector. IANFA 45 3124. RADIOACTIVITY ~S°Os; measured -/-~-coin,7(0),I(ce),~(t),ET,I~; deduced y r a s t , r o t a t i o n a l bands,J,Tr,inter-band ~ - m u l t i p o l a r i t y , 7 - b r a n c h i n g , g ( k ) , c o n f i g u r a t i o nZPAAD . 304 277. NUCLEAR REACTIONS l~4,~66,'6SEr(~60,4n),E=80-105 MeV; measured ~(E,0),77-coin,~/7(t). ~TetTs ~°0s deduced levels,J,Tr,T,rotational bands,ICC, tS°Os deduced isomer,configuration. Ge, Ge(Li),Compton-suppressed detector. B a n d - m i x i n g calculations. NUPAB 383 119.

A ~8~Lu

AND

=

183

R A D I O A C T I V I T Y t83mRe,tSOmw [ f r o m 181Ta((~,2n), 18~W(~,t), 1"77Hf(a,n),E=31 T1/2; d e d u c e d 7 - b r a n c h i n g . E n r i c h e d t a r g e t , G e ( L i ) d e t e c t o r . IANFA NUCLEAR MOMENTS lS3Re [ f r o m 185Re(d,4n)ta3Os(fl++EC)decay]; m e a s u r e d i n Fe; d e d u c e d / z , r e l a x a t i o n t i m e . C a r r i e r f r e e Os e l e c t r o p l a t e d i n

81

MeV]; m e a s u r e d E-f,IT, 45 3124. NMR on o r i e n t e d nuclei Fe f o i l . HYIND 11 37.

KEY

NUMBERS

A i84 W

D 82A105:

184Re

D 82A105:

RADIOACTIVITY 184mRe; f i e l d f o r W i n Fe. 184W RADIOACTIVITY 184mRe; f i e l d f o r W i n Fe. 184W

J

i85Au

D 82Bo27:

laSHg

D 82Bo27:

82Bu14:

D 82Al11: R 82Le02:

186ir

D 82Al11:

186TI

R 81Kr20:

J

82Bu14:

R 82Ka28:

82Le02: 82Po07:

188T1

R 81Kr20:

R 82Po07:

190Hg

R 82Gu10:

=

186

=

187

=

hyperfine

c o n s t a n t s . ABMR,

188

NUCLEAR REACTIONS t a V O s , 1 9 S p t ( n , 3 , ) , E = t h e r m a l ; m e a s u r e d I ( c e ) , E 7 , I ? . lSO0s,196Pt d e d u c e d levels,B(E0)/B(E2),E0 transition strength. Interacting b o s o n model,O(6) l i m i t . PYLBB 117 15. NUCLEAR REACTIONS les,1880s,194,196Pt(aaS,SeS'),E ~ 80 MeV; m e a s u r e d 7(0,H) in p o l a r i z e d Fe, C o u l o m b excitation,?aaS-coin,T(O). 188,18SOs,194,196pt l e v e l d e d u c e d g. PRVCA 25 293. NUCLEAR REACTIONS 188,tgo,lgaOs,19%i96,198pt,t98,zo°,z°z,Z°4Hg,a°sPb(n,n'7),E=O.15-1 MeV; measured (9"; d e d u c e d o p t i c a l m o d e l p a r m e t e r s , iae,19°,lgZ0s,194,196,198pt,198,a°°,z°z,Z°4Hg,a°sPb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . IANFA 46 892. NUCLEAR REACTIONS 168Er(e7A1,5n),E=130-160 MeV; 169Tm(2SMg,4n),E=120 MeV; t76Hf(19F,5n), E = 8 5 - 1 2 0 MeV; t S a T m ( e 4 M g , 5 n ) , E = l 1 5 - 1 3 5 MeV; 1 5 9 T b ( a Z s , 5 n ) , E = 1 6 0 - 1 6 5 MeV; lSSGd(asCI,4n), E = 1 5 5 - 1 7 0 MeV; m e a s u r e d a ( E T ) , T ( 0 ) , ' y T - c o i n , I ( K X - r a y ) . 186,1ae,tg°T1 d e d u c e d levels,J,~r, isomer T1/a,ICC,?-multipiolarity,configuration. Anti-Compton shield,Ge(Li) detector, p u l s e d b e a m . PRLTA 47 1709.

A

l~OOs

hyperfine

185

NUCLEAR MOMENTS t85,187Re; m e a s u r e d h f s , i s o t o p e s h i f t ; d e d u c e d l a s e r i n d u c e d f l u o r e s c e n c e . ZPAAD 307 201.

A

laaOs

=

hyperfine

RADIOACTIVITY tSSlr [ f r o m laSRe((x,3n),E=40 MeV]; m e a s u r e d I T ( 0 ) , o r i e n t e d n u c l e i i n Fe; d e d u c e d /~. 1860s t r a n s i t i o n s d e d u c e d 8. B a n d m i x i n g c a l c u l a t i o n s . JPHGB 8 857. NUCLEAR REACTIONS 186,~S80s,194,196pt(SaS,azS'),E ~ 80 MeV; m e a s u r e d 7(0,H) i n p o l a r i z e d Fe, C o u l o m b e x c i t a t i o n , T O S S - c o i n , 7 ( 0 ) . 188,tSSOs,~ga,laSPt l e v e l d e d u c e d g. PRVCA 25 293. RADIOACTIVITY tOSlr [ f r o m 185Re((x,3n),E=40 MeVS; m e a s u r e d I T ( 0 ) , o r i e n t e d n u c l e i i n Fe; d e d u c e d /z. taSOs t r a n s i t i o n s d e d u c e d 8. B a n d m i x i n g c a l c u l a t i o n s . JPHGB 8 857. NUCLEAR REACTIONS l~SEr(eTAI,Sn),E=130-160 MeV; Je9Tm(ZSMg,4n),E=120 MeV; 176Hf(19F,Sn), E = 8 5 - 1 2 0 MeV; 1 6 9 T m ( a a M g , 5 n ) , E = l 1 5 - 1 3 5 MeV; 1 5 9 T b ( S a S , 5 n ) , E = l S 0 - 1 6 5 MeV; 155Gd(asc1,4n), E = 1 5 5 - 1 7 0 MeV; m e a s u r e d a ( E T ) , 3 , ( 0 ) , ? 7 - c o i n , I ( K X - r a y ) . las,lss,19°T1 d e d u c e d l e v e l s , J , w , isomer Tt/z,ICC,?-multipiolarity,configuration. A n t i - C o m p t o n s h i e l d , O e ( L i ) d e t e c t o r , p u l s e d b e a m . PRLTA 47 1709.

A

187Re

184

NUCLEAR MOMENTS 185,t87Re; m e a s u r e d h f s , i s o t o p e s h i f t ; d e d u c e d h y p e r f i n e c o n s t a n t s . ABMR, l a s e r i n d u c e d f l u o r e s c e n c e . ZPAAD 307 201. RADIOACTIVITY 185mHg(IT),t85Hg(EC),(fl+) [ f r o m Au(p,xn)Hg,on-line mass-separation]; m e a s u r e d E T , I T , I C C , 7 7 - , 7 ( X - r a y ) - c o i n . lSnmHg d e d u c e d IT d e c a y b r a n c h i n g . 185Hg d e d u c e d levels. 185Au d e d u c e d levels,J,rr,ICC,7 multipolarity. Hyperpure Ge,Ge(Li),Si(Li) detectors,magnetic spectrograph. NUPAB 386 308. RADIOACTIVITY t85mHg(IT),taSHg(EC),(fl+) [ f r o m Au(p,xn)Hg,on-line mass-separation]; measured E T , 1 7 , l C C , 7 7 - , 7 ( X - r a y ) - c o i n . 185mHg d e d u c e d IT d e c a y branching, lSSHg d e d u c e d levels. 185Au d e d u c e d levels,J,Tr,ICC,7-multipolarity. Hyperpure Ge,Ge(Li),Si(Li) detectors,magnetic spectrograph. NUPAB 386 308.

A

~8eOs

=

KEYWORDS

m e a s u r e d ? ( O , H , t ) , ? ? ( 0 ) , o r i e n t e d n u c l e i i n Fe; d e d u c e d l e v e l s d e d u c e d g(R),8. ZPAAD 305 157. m e a s u r e d ?(O,H,t),77(O),oriented n u c l e i i n Fe; d e d u c e d l e v e l s d e d u c e d g(R),8. ZPAAD 305 157.

A

taSRe

AND

=

190

NUCLEAR REACTIONS 188,19°,19ZOs,i94,19%19ept,19s,a°°,a°2,a°4Hg,a°sPb(n,n'3'),E =0.15-1 MeV; 18B, 190 , 192Os, 194 , 196 , 198 Pt . 198 measured G; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . . 2.0 0 . 2 0 2 8 0 4 Hg, 2 0 6 P b l e v e l d e d u c e d fla- C o u p l e d - c h a n n e l s a n a l y s i s . IANFA 46 892. NUCLEAR REACTIONS tSlTa(t4N,5n),E=100 MeV; m e a s u r e d E ? , I s , , ? ~ / - e o i n , ? ( 0 ) . 19°Hg d e d u c e d levels,J,Tr, N a t u r a l t a r g e t s , G e ( L i ) , N a I d e t e e t o r s . C r a n k i n g m o d e l c a l c u l a t i o n s . NUPAB 383 541.

82

KEY

NUMBERS

A 19OT1

R

81Kr20

D

81La25

1alp t

D

81La25

R A D I O A C T I V I T Y ~91pt [ f r o m d e d u c e d tt. 191Ir t r a n s i t i o n s R A D I O A C T I V I T Y ~91Pt [ f r o m deduced tt. 19tit t r a n s i t i o n s

R 82Bl17 82Po07:

19aTl

R

82Da17

D 82Ha28

t94pt

R 82Bl17 82Le02 82Po07:

194Hg

R 82Ra06

83Ri02

194TI

D 82Hi04

194pb

D 82Hi04

D 83Hi04:

195pb

D 82Hi04:

=

191

=

nuclei; nuclei

192

=

194

R A D I O A C T I V I T Y 194Ir [ f r o m ~Salr(n,7)]; m e a s u r e d NMR o n o r i e n t e d n u c l e i in Fe,Ni; d e d u c e d g, electric quadrupole moment. Z P A A D 306 73. NUCLEAR REACTIONS 193Ir(3He,d),(d,aHe),E=40 MeV; m e a s u r e d or(0). 194pt,19aOs l e v e l s , d e d u c e d L,C2S. S u p e r s y m m e t r i c s c h e m e m o d e l s , D W B A a n a l y s i s . NUPAB 388 77. NUCLEAR REACTIONS 186,laeOs,194,196pt(aas,3aS'),E ~ 80 MeV; m e a s u r e d 7(0,H) i n p o l a r i z e d Pc, Coulomb exeitation,TaaS-eoin,7(0). 188,1860s,la4,196pt l e v e l d e d u c e d g. P R V C A 25 293. NUCLEAR REACTIONS 1 8 s , 1 9 ° , l S a O s , Z 9 4 , 1 9 6 , 1 9 S p t , 1 9 8 , a ° ° , a s e , a ° 4 H g , a ° 6 p b ( n , n ' ~ ) , E = O . 1 5 - I MeV; measured a; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . 188,19°,19aOs,194,19s,198pt,198,2°°,2°a,a°4Hg,2°spb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . I A N F A 48 892. NUCLEAR REACTIONS l S a W ( z a C , F ) , ( l a C , p ) , ( l e C , d ) , ( 1 2 C , t ) , ( l a C , ~ ) , E = 7 7 - 1 6 7 MeV; 175Lu(19F,F),(19F, p),(19F,d),(19F,t),(19F,(~),E=135,184 MeV; 1 7 4 Y b ( a ° N e , F ) , ( ~ ° N e , p ) , ( a O N e , d ) , ( a ° N e , t ) , ( a S N e , c ~ ) , E = 1 2 5 , 2 5 2 MeV; 1 5 4 S m ( 4 ° A r , F ) , ( 4 ° A r , p ) , ( 4 ° A r , d ) , ( 4 9 A r , t ) , ( 4 ° A r , a ) , E = 1 9 6 - 3 4 0 MeV; m e a s u r e d a(E),(~(fission),a(fusion),a(evaporation r e s i d u e ) v s E; d e d u c e d r e a c t i o n m e c h a n i s m . 194Hg deduced fission,evaporation competition spin,energy dependences. Statistical model. P R V C A 35 2417. NUCLEAR REACTIONS 1 1 6 S n , 1 5 4 S m , i 9 7 A u ( 4 ° A r , p F ) , ( 4 O A r , d F ) , ( 4 ° A r , t P ) , ( 4 O A r , a F ) , E = 3 3 3 MeV; measured (fragment)p-,(fragment)d-,(fragment)t-,(fragment)a-coin,cr(fragment 0,0p,Ep), a(fragment O,Oo~,Ea); d e d u c e d r e a c t i o n m e c h a n i s m , a3VBk,194Hg,i56Er d e d u c e d emission barriers,level density parameters,rms(J), Evaporation,statistical m o d e l s . P R V C A 25 2 4 3 0 . R A D I O A C T I V I T Y 194,195,196pb [ f r o m 197Au(SLi,xn),E=95 MeV]; m e a s u r e d E T , I T , 7 7 - c o i n ; d e d u c e d log f t . 194 195,196rnpb d e d u c e d T l / a . 194,196,196T1 d e d u c e d tevels,J,rr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A 25 2710. R A D I O A C T I V I T Y 194,195,196Pb [ f r o m 197Au(SLi,xn),E=95 MeV]; m e a s u r e d E-y,I-/,TV c o i n ; d e d u c e d log f t . 194 195,196mpb d e d u c e d T1/a. 194,195,198T1 d e d u c e d levels,J,Tr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A 25 2710.

A 195T1

continued

NUCLEAR REACTIONS 193Ir(aHe,d),(d,aHe),E=40 MeV; m e a s u r e d o'(0). 194pt,~Sa0s l e v e l s , d e d u c e d L,C2S. S u p e r s y m m e t r i c s c h e m e m o d e l s , D W B A a n a l y s i s . N U P A B 388 77. NUCLEAR REACTIONS 188,19°,19aOs,194,196,198Pt,I98,a°9,a°a,a°4Hg,2°sPb(n,n'7),E=O.15-1 MeV; measured or; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . Ias,19°,lSaOs,194,196,198pt,19s,a°oa°a,aO4Hg,a°spb level deduced fla. C o u p l e d - c h a n n e l s a n a l y s i s . I A N F A 46 893. NUCLEAR REACTIONS l°SAg(13C,3n),E=52 MeV; 181Ta(160,5n),E=100 MeV; m e a s u r e d I7(0,t). uaI l e v e l d e d u c e d g,T1/a, 19aT1 l e v e l d e d u c e d g , q u a d r u p o l e moment,T1/a. NUPAB 383 431.

A 194ir

190

1 9 ~ I r ( d , 2 n ) , E = 2 0 MeV]; m e a s u r e d I7(0),NMR,oriented d e d u c e d d. M o d e l c a l c u l a t i o n s . J P H G B 7 1713. ~9~Ir(d,2n),E=20 MeV]; measured IT(0),NMR,oriented d e d u c e d d. M o d e l c a l c u l a t i o n s . J P H G B 7 1713.

A

~92Os

=

KEYWORDS

NUCLEAR REACTIONS 16SEr(a7Al,5n),E=13O 160 MeV; ~69Tm(aSMg,4n),E=120 MeV; ~76Hf(19F,5n), E = 8 5 - 1 2 0 MeV; 1 6 9 T m ( a 4 M g , 5 n ) , E = l 1 5 - 1 3 5 MeV; 159Tb(3aS,5n),E=160--165 MeV; 155Gd(35C1,4n), E = 1 5 5 - 1 7 0 MeV; m e a s u r e d a(ET),'~(a),77-eoin,I(K X-ray). ~as,tsa,tsaT1 d e d u c e d levels,J,rr, isomer Tl/a,ICC,7-multipiolarity,configuration. Anti-Compton shield,Ge(Li) detector p u l s e d b e a m . P R L T A 47 1709.

A tOtlr

AND

=

195

R A D I O A C T I V 1 T Y 194,195,196pb [ f r o m 197Au(VLi,xn),E=95 MeV]; m e a s u r e d ET,I7,7"/-coin; d e d u c e d log f t . 194,195,t96rnpb d e d u c e d TI/2. 194,195,196T1 d e d u c e d levels,J,Tr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A 25 2710. R A D I O A C T I V I T Y 194,t95,196pb [ f r o m 197Au(SLi,xn),E=95 MeV]; m e a s u r e d E 7 , I 7 , - / 7 - c o i n ; d e d u c e d log f t . 194,195,196mpb d e d u c e d T l / a . ls4,195,196T1 d e d u c e d levels,J,rr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A 25 2710.

83

KEY

NUMBERS

A '96pt

R 82Ka28:

8~LeO2 8~Po07

I96Au

D

190TI

D 82Hi04

196pb

D 82Hi04

82Ha04

D 82So05

197Hg

R 82Be21

19Vpo

D 8gBoO4

D 82Ta08:

198pt

D 82TaO8: R 82Po07:

198Hg

R 82Po07:

'98po

D 82Bo04:

D 82Ha39:

199Hg

D 82A123:

I99TI

R 82Ca10:

199p0

D 82Bo04:

=

197

=

198

R A D I O A C T I V I T Y igSIr [ f r o m 198pt(n,p)3; measured E7,17. 19apt d e d u c e d new transition intensity upper limit. Enriched t a r g e t , G e d e t e c t o r . J U P S A 51 31. R A D I O A C T I V I T Y 198Ir [ f r o m 198pt(n,p)3; measured E7,]7. 198pt d e d u c e d new transition intensity upper limit. Enriched t a r g e t , G e d e t e c t o r . J U P S A 51 31. NUCLEAR REACTIONS * 8 8 , 1 9 o , 1 9 2 0 s , 1 9 4 , 1 9 s , 1 9 8 p t , 1 9 a , a o ° , a ° 2 , a ° 4 H g , 2 ° s P b ( n , n ' 7 ) , E = 0 . 1 5 - 1 MeV; measured a; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . 188,19°,1920s,194,196,198pt,198,a°°,2°2,a°4Hg,2°sPb level deduced flu. C o u p l e d - c h a n n e l s a n a l y s i s . I A N F A 46 892. NUCLEAR REACTIONS l s 8 , 1 9 9 , 1 9 a O s , 1 9 4 , ~ 9 6 , 1 9 8 p t , 1 9 8 , u ° ° , 2 ° a , a ° 4 H g , a ° s P b ( n , n ' 7 ) , E = 0 . 1 5 - 1 MeV; measured or; d e d u c e d o p t i c a l m o d e l p a r m e t e r s , lSS,19°,lgaOs,t94,196,198Pt,los,z°°,z°e,ea4Hg,gO6pb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . I A N F A 46 892. RADIOACTIVITY ~5~51Dy~5~5~m~5a~52mH~5~'~53Er~53~54~54mTm~7~78~77~17~P~55Yb~98~97m 199mpo,ZI[Fr,ZlaRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV[; m e a s u r e d Ea,T1/2. J49Tb,an,2~a,aJs,aJs,~lTAt, 2°4,z~s,2~9Fr,Zll,anrn,~la,ala,~apo,alT,aiSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A

199AI/

196

R A D I O A C T I V I T Y i97mpt [ f r o m *gSPt(n,7)3; m e a s u r e d E T , I T ( t ) , 7 7 ( t ) , 7 7 ( 0 , H , T ) , T I / a . ~97pt l e v e l s deduced B(A),jz,g. Enriched target,Ge(Li),hyperpu re Ge,Nal(T1) detectors. Particle-vibrator c o u p l i n g m o d e l . P R V C A 25 1587. NUCLEAR REACTIONS 199Hg(p,t),E=25 MeV; m e a s u r e d cr(Et),Q. ~97Hg d e d u c e d m a s s excess. PRVCA 25 E848. R A D I O A C T I V I T Y 15°,i51Dy,151,151rn,153,15~m Ho,15~,153 E r,153,154,154 -mTm,179,i78,177,176pt,155y b,19s,197m, 199rnpo,a13Fr,21aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV[; m e a s u r e d Ea,T~/a. 149Tb,~ll,214,a15,alS,alTAt, a°4,al8,algFr,all,allrn,ala,al3,al4po,alT,elSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A

1981F

=

KEYWORDS

NUCLEAR REACTIONS l a 7 0 s , 1 9 5 p t ( n , 7 ) , E = t h e r m a l ; measured I(ce),ET,I 7. ~880s,t96Pt d e d u c e d levels,B(E0)/B(Ea),E0 transition strength. Interacting b o s o n m o d e l , O ( 6 ) l i m i t . PYLBB 117 15. NUCLEAR REACTIONS ~s6,18aOs,i94,~96pt([aS,[aS'),E ~ 80 MeV; m e a s u r e d 7(O,H) i n p o l a r i z e d Fe, Coulomb excitation,73aS-coin,7(0), ls8,1860s,194,tgapt l e v e l d e d u c e d g. P R V C A 25 ~93. NUCLEAR REACTIONS ~ s 8 , 1 9 0 , l g Z O s , 1 9 4 , 1 9 ° , ~ g S p t , 1 9 a , 2 ° o , a ° a , a O 4 H g , 2 ° 6 P b ( n , n , 7 ) , E = 0 . 1 5 - 1 MeV; measured ~; d e d u c e d o p t i c a l m o d e l p a r m e t e r s , la8,~9°,lgaOs,194,19°,~98pt,198,a°°,a°a,2°4Hg,2°°pb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . I A N F A 46 892. R A D I O A C T I V I T Y 19amAu [ f r o m 198pt(d,4n)]; m e a s u r e d IT(O,T),NMR o n o r i e n t e d n u c l e i . 196mAu deduced g,#,configuration of isomeric state. Recoil implantation i n t o Ni. NUPAB 373 256. R A D I O A C T I V I T Y 194,195,196Pb [ f r o m t97Au(SLi,xn),E=95 MeV]; m e a s u r e d E T , I 7 , 7 7 - e o i n ; d e d u c e d log f t . 194,195,196rapb d e d u c e d Ti/~. i94,195,196T1 d e d u c e d levels,J,zr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A 25 2710. R A D I O A C T I V I T Y 194,195,*9~pb [ f r o m 197Au(SLi,xn),E=95 MeV]; m e a s u r e d E T , I T , 7 7 - c o i n ; d e d u c e d log f t . 194,195,196mpb d e d u c e d T1/a. 194,195,196T1 d e d u c e d levels,J,Tr,Nilsson configurations. Ge(Li) d e t e c t o r s . P R V C A ~5 2710.

A 197pt

AND

=

199

R A D I O A C T I V I T Y 199Au(•-) [ f r o m 199pt decay~; m e a s u r e d N M R , o r i e n t e d n u c l e i i n Fe; d e d u c e d hyperfine splittings. Z P A A D 307 159. R A D I O A C T I V I T Y i99mHg [ f r o m Hg(n,n'),E=reactor spectrum]; measured specific activity. R R A L A 51 41. NUCLEAR REACTIONS 1 9 7 A u , l Z l S b ( a , n ) , ( a , a n ) , E = l l . 5 - 2 7 MeV; m e a s u r e d a ( E ) . a°°,199Tl,~a4,123I deduced level density,average 7-strength. N U P A B 383 251. R A D I O A C T I V I T Y 15~t~Dy~t5t~t5~m~l~e~52mH~52~53Er~53~54~54mTm~79~78~j7~j-]BPt~55Yb~j9~~97m 199mpo,g13Fr,212Ra [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d EoGTI/2. 149Tb,all,214,215,ZlS,a17At, 2°4,218,alOFr,an,anm,ZlZ,ala,a14Po,~lT,alSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ecx. Helium jet recoil product separation. P R V C A 25 941.

84

KEY

NUMBERS

A 2OOHg

R 82Po07

aOOTl

R 82Ca10

aoOpb

J

82Th05

R 82Hi09

82Le05

AND

=

200

NUCLEAR REACTIONS t88,19°,lgaos,t94,196,19Spt,198,a°°,aoa,2°4Hg,a°sPb(n,n'7),E=O.15-I MeV; measured or; d e d u c e d o p t i c a l m o d e l p a r m e t e r s , ls8,t9°,1920s,194,196,198pt,ls8,2°°,a°2,2°4Hg,2°6pb l e v e l d e d u c e d fla- C o u p l e d - c h a n n e l s a n a l y s i s . IANFA 46 892. NUCLEAR REACTIONS 1 9 7 A u , i a l S b ( a , n ) , ( a , 2 n ) , E = l i . 5 - 2 7 MeV; m e a s u r e d ~(E). 2°°,i99T1,!24,i23I deduced level density,average v-strength. NUPAB 383 251. NUCLEAR MOMENTS 2°°,ZOl,ZOz,203,z°4,aes,a°s,a°7,aÙspb; measured hfs. ao°,z°z,2o4,a°sPb deduced isotopes s h i f t s , r m s radii, e°1,z°3,z°5,e°7pb deduced isotope s h i f t s , t i n s radii,/x. High resolution laser spectroscopy. ZPAAD 305 89. NUCLEAR REACTIONS 18'Ta(19F,X),(19F,F),E=80-125 MeV; 17°Er(a°Si,X),(3°Si,F),E=i25-170 MeV; measured (;(fragment E,0). 2°°pb deduced fission probability versus angular m o m e n t u m . Statistical model fits. NUPAB 385 109. NUCLEAR REACTIONS ~a~Ta(~SF,X),(19F,F),E=80-126 MeV; 17°Er(3°Si,X),(S°si,F),E=125-168 MeV; measured ff(fission),cr(evaporation residue) vs E,0; deduced (~(fusion,E). e°°Pb deduced total fission probability vs (L). Bohr independence hypothesis,complete fusion. PRLTA 48 527.

A = ZOlT1

R 82Bu04:

2oIpb

J 82Th05:

aOlBi

R 82Br21

R 82Po07

aoapb

J

2O2Bi

D 81Va29

82Th05

R 82Hu07

J

aOSBi

D 82Lo14

82Th05

R 82Hu07: 82Lo14

SOaps

D 82Lo14

R 82Po07

203

=

NUCLEAR MOMENTS 2°°,2°1,2°2,2°3,2°4,3°5,2°6,2°7,2°8Pb; m e a s u r e d h f s . a°°,2°~,a°4,2oSpb d e d u c e d isotopes shifts,rms r a d i i . 2°1,2°3,2°5,2°7pb d e d u c e d isotope shifts,rms radii,#. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. RADIOACTIVITY a°arnpo(EC),(f+) [ - f r o m a ° 4 p b ( a H e , 4 n ) , E = 2 7 . 4 MeVS; m e a s u r e d ET,IT(t). Z°3Bi deduced levels,J,rr,isomer Tw2,7-branching,T-multipolarity,ICC,configuration. ZPAAD 307 175. NUCLEAR REACTIONS 2 ° S T l ( a , x n ) , E - 6 4 MeV; m e a s u r e d 7(0,H,t). z°z,2°s,2°SBi l e v e l s d e d u c e d g. NUPAB 382 56. NUCLEAR REACTIONS e°a,a°STl(SHe,3n),E=20 26.6 MeV; m e a s u r e d ET,17,ff(ET),7(t),T(O),I(ce), 7T-eoin. 2°3,2°5Bi d e d u c e d isomer Tl/2,1evels,J,rr,T-branching,7-multipolarity,ICC, configuration. ZPAAD 307 175. R A D I O A C T I V I T Y 2°Smpo(EC),(f+) [ f r o m 2 ° 4 P b ( a H e , 4 n ) , E = 2 7 . 4 MeV2; m e a s u r e d ET,IT(t). a°aBi deduced levels,J,rr,isomer T1/2,7-branching,7-multipolarity,lCC,configuration. ZPAAD 307 175.

A aO4Hg

= 202

NUCLEAR REACTIONS Iss,tg°,tgaos,194,196,tgaPt,19a,a°°,ao2,a°4Hg,2°spb(n,n'7),E=0.15-1 MeV; measured G; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . 188,19°,19a0s,194,t96,lSSpt,198,2°°,2°a,a°4Hg,2°6pb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . IANFA 46 892. NUCLEAR MOMENTS a°°,~°l,z°~,aes,2°4,a°s,a°6,aOT,aOSpb; m e a s u r e d h f s . a°°,ao2,a°4,a°sPb d e d u c e d isotopes shifts,rms r a d i i , z°l,2°a,a°5,a°Tpb deduced isotope s h i f t s , r m s radii,~. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. RADIOACTIVITY 210,a°a,aes,a°4At,ei2Fr; m e a s u r e d Ea,Ia. ao2,e°4,a°aBi,aSSAt d e d u c e d l e v e l s , a-branching,hindrance f a e t o r , J , r r . IANFA 45 1966. NUCLEAR REACTIONS 203Tl(a,xn),E=64 MeV; m e a s u r e d 7(0,H,t). zea,aoa,Z°SBi l e v e l s d e d u c e d g. NUPAB 382 56.

A 2o3pb

201

NUCLEAR REACTIONS a°Tpb(Ix-,xn),E at r e s t ; m e a s u r e d E7,17; deduced c a p t u r e m e c h a n i s m , single,multi-neutron e m i s s i o n p r o b a b i l i t i e s . 2°~T1 l e v e l d e d u c e d e x c i t a t i o n probability. PYLBB 110 375. NUCLEAR MOMENTS 2°°,z°l,2°2,2°3,ao4,2°5,2os,z°7,2°sPb; m e a s u r e d h f s . 20°,20z,zO4,Zo6pb deduced isotopes s h i f t s , r m s radii, a°l,2°a,2°5,2°7pb deduced isotope shiffis,rms radii,/~. High resolution laser spectroscopy. ZPAAD 305 89. NUCLEAR REACTIONS 2°STl(a,6n),E=66,70,77 MeV; measured ET,17,7(t),7(0),77-coin. a°iBi deduced ]evels,J,~r,Ti/2, NUPAB 389 366.

A 2O2Hg

KEYWORDS

=

204

NUCLEAR REACTIONS tss,tg°,19aOs,194,t96,198Pt,19s,2o°,2°2,2°4Hg,2°sPb(n,n'7),E=0.15-1 MeV; measured or; deduced optical model parmeters. 188,19°,1920s,194,196,t98pt,198,2o°,zog,2°¢Hg,a°sPb level deduced fz. Coupled-channels analysis. IANFA 46 892.

85

KEY

NUMBERS

A ao4pb

J

aa4Bi

D 81Va29:

aO4po

R 82Hal6:

SO,At

D 81Va27:

82Th05:

81Va29: aO4Fr

D 82Bo04:

R 82Ca14:

82Ma05: aoSpb

J

82Th05:

aasBi

R

82Hu07

82Lo14

aOSAt

R 82SjOI

R

82Be38

aospb

J

82Th05

R 81Fi07 82Ca14

82Ge06

82Po07

82St03: ZOSBi

D 81E107:

81Va29: 2O6po

D 81E107:

204

continued

=

305

NUCLEAR REACTIONS 2°STl,aasPb(e,e),E=502 MeV; m e a s u r e d cr(0),ratio vs m o m e n t u m transfer; deduced shell model validity in nuclear interior,3s radial wave function. 2°sPb,a°ST1 deduced charge density difference. Density-dependent H a r t r e e - F o c k t h e o r y . PRLTA 49 978. NUCLEAR REACTIONS a°4Hg(t,an),E=16 MeV; m e a s u r e d 7(0,H,t); d e d u c e d g(~rhn/z-l), a°ST1 level d e d u c e d g. T h i c k , e n r i c h e d l i q u i d t a r g e t . PRLTA 48 466. NUCLEAR MOMENTS z°°,a°l,a°a,z°3,aa4,a°s,z°6,a°7,a°sPb; m e a s u r e d h f s . zoo aoa ao4,aospb d e d u c e d isotopes shifts,rms r a d i i . ~°l,a°3,a°s,a°7pb d e d u c e d isotope shifts,rms radii,~. High r e s o l u t i o n l a s e r s p e c t r o s c o p y . ZPAAD 305 89. NUCLEAR REACTIONS aO3Tl(a,xn),E=64 MeV; m e a s u r e d 7(0,H,t). a°2,z°3,Z°5Bi l e v e l s d e d u c e d g. NUPAB 382 56. NUCLEAR REACTIONS a o 3 , a ° S T l ( a H e , 3 n ) , E = 2 0 - 2 6 . 6 MeV; m e a s u r e d ET,IT,a(ET),7(t),7(0),I(ce), 77-coin. z°3,2°SBi d e d u c e d isomer T,/a,levels,J,~,7-branching,7-multipolarity,ICC, configuration. ZPAAD 307 175. NUCLEAR REACTIONS 197Au(laC,4n),E=77 MeV; m e a s u r e d 77-coin,7(0),7(t),ET,IT. a°SAt d e d u c e d l e v e l s , J , T r , T 1 / 2 , B ( ) , ) , 7 - m u l t i p o l a r i t y . PRVCA 25 889.

A aOSHg

=

KEYWORDS

NUCLEAR MOMENTS 2°°,a°l,a°a,2°3,aa4,a°5,a°e,2°7,2°spb; m e a s u r e d h f s . a°°,a°a,2°4,2°spb d e d u c e d isotopes shifts,tins r a d i i . 2°l,z°3,2°s,e°TPb d e d u c e d isotope shifts,rms radii,/~. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. R A D I O A C T I V I T Y ala,2°s,a°s,a°4At,alaFr; m e a s u r e d Ea,Ia. a°a,aa4,a°SBi,a°SAt d e d u c e d l e v e l s , a-branching,hindrance f a c t o r , J , T r . IANFA 45 1966. NUCLEAR REACTIONS a°4pb(a,4n),E=50 MeV; m e a s u r e d ce(0,H,t); d e d u c e d s p i n p r e c e s s i o n of Po i n Ni. a ° 4 p o l e v e l d e d u c e d g,B(Ea). I n - b e a m recoil implantation,iron free orange spectrometer. ZPAAD 305 1. RADIOACTIVITY alo,aas,2°6,a°4At,alaFr; m e a s u r e d Ea,Ia; d e d u c e d a - b r a n c h i n g . ~r s q u a r e - r o o t two magnetic spectrometer. IANFA 45 1861. RADIOACTIVITY al°,2°s,a°6,a°4At,alaFr; m e a s u r e d Ea,la. a°a,a°4,a°SBi,2°aAt d e d u c e d l e v e l s , a-branching,hindrance f a c t o r , J j r . IANFA 45 1966. RADIOACTIVITY ~ D y ~ ' ~ m ' ~ 5 2 ~ 5 2 m H ~ 5 ~ 5 3 E r ~ 5 3 ~ 5 4 ~ 4 m T m ~ 7 9 ~ 7 8 ~ i 7 7 ~ 7 ~ P t ' ~ 5 Y b ~ 9 8 ' 197m, 199mpo,213Fr,aiZRa C f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,Tl/a. 149Tb,an,a14,ais,zla,a'7At, a°4,a~a,algFr,Zll,Z'~m,a'a,al3,al4po,al7,alaRn [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV3; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA ~5 941.

A aOST1

AND

=

206

NUCLEAR REACTIONS 2°~Hg(t,p),E=16 MeV; m e a s u r e d 7 ( 0 , H ) , 7 - y i e l d s ; d e d u c e d 3s p r o t o n g. Z°SHg l e v e l s d e d u c e d J,Tr,g,Tl/2. PRVCA 26 914. NUCLEAR MOMENTS a°°,2°l,2°z,2°a,2°4,2°s,a°s,2°~,2°spb; m e a s u r e d h f s . z°°,a°z,z°4,a°sPb d e d u c e d isotopes shifts,rms r a d i i , a°l,a°3,a°s,Z°TPb d e d u c e d isotope shifts,rms radii,~. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. NUCLEAR REACTIONS 2 ° s P b ( p , p ' ) , E = 3 5 MeV; m e a s u r e d cr(0). Z°sPb d e d u c e d l e v e l s , t r a n s i t i o n s t r e n g t h s : C o l l e c t i v e DWBA a n a l y s i s . PYLBB 107 182. NUCLEAR REACTIONS a°5Tl,Z°spb(e,e),E=502 MeV; m e a s u r e d (r(0),ratio v s m o m e n t u m transfer; deduced shell model validity in nuclear interior,3s radial wave function. Z°sPb,Z°STl deduced charge density difference. Density-dependent H a r t r e e - F o c k t h e o r y . PRLTA 49 978. NUCLEAR REACTIONS a°spb,n%n(a,SHe),E=218 MeV; m e a s u r e d a(E(SHe)),(~(0); d e d u c e d r e a c t i o n m e c h a n i s m , n4Sn,Z°sPb d e d u c e d l e v e l s , J , T r , L , c o n f i g u r a t i o n . Z e r o - r a n g e DWBA a n a l y s i s . PYLBB 117 20. NUCLEAR REACTIONS 1 8 8 , 1 9 ° , 1 9 a O s , 1 9 4 , 1 9 6 , 1 9 8 p t , 1 9 8 , a ° ° , a ° a , a ° 4 H g , a ° s P b ( n , n ' 7 ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d or; d e d u c e d o p t i c a l m o d e l p a r m e t e r s . 188,19°,iOaOs,194,196,198pt,198,a°°,a°2,aO4Hg,a°sPb l e v e l d e d u c e d fla. C o u p l e d - c h a n n e l s a n a l y s i s . IANFA 46 892. NUCLEAR REACTIONS a ° n , a ° s P b ( 7 , 7 ) , E = 9 . 5 - 1 2 MeV; m e a s u r e d cr(0,E), a ° s P b d e d u c e d p o s s i b l e r e s o n a n c e , F , a°aPb d e d u c e d f i n e s t r u c t u r e dipole assignment. PRVCA 25 780. RADIOACTIVITY Z°SPo C f r o m Z°sPb(aHe,3n),E=29 MeV]; m e a s u r e d 7 7 ( 0 ) , o r i e n t e d nuclei,ET,IT. Z°°Bi t r a n s i t i o n s deduced directional correlation coeffieients,~. Multichannel g o n i o m e t e r . ZPAAD 303 103. RADIOACTIVITY al°,2°s,a°6,a°4At,aiaFr; m e a s u r e d E a , I a . a°a,a°4,aa6Bi,a°SAt d e d u c e d l e v e l s , a-branching,hindrance f a c t o r , J , w . IANFA 45 1966. RADIOACTIVITY Z°SPo [ f r o m aOSpb(3He,3n),E=29 MeV]; m e a s u r e d 7 7 ( 0 ) , o r i e n t e d nuclei,ET,IT. a°SBi t r a n s i t i o n s deduced directional correlation coefficients,6. Multichannel g o n i o m e t e r . ZPAAD 303 103.

86

KEY

NUMBERS

A 2o6po

D 82Br07:

aO6At

D

81Va27: 81Va29 82Br07

J

82Th05

R 81St25 82Ba38 82La12

2O7Bi

D 82Ta18

2O~po

D 81Ch38 81Ch39

2OTAt

D 81Ch38 81Ch39

J

82Th05

R 81Ac02

81A127

81St25 82Be04 82C101:

82Dj01:

82Ga02:

82Gu02:

82He03:

206

continued

=

207

NUCLEAR MOMENTS 2°°,2°l,2°z,2°3,a°4,205,2°6,2°7,a°spb; m e a s u r e d h r s . 2°°,202,2°4,2°sPb d e d u c e d isotopes shifts,rms r a d i i . 2°1,2°3,2°5,2°7pb d e d u c e d isotope shifts,rms radii,p.. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. NUCLEAR REACTIONS 2 ° 8 P b ( a , a ' n ) , E = 1 0 4 MeV; m e a s u r e d n a - c o i n , E a , E n , a°sPb d e d u c e d GQR branching r a t i o . 2°Tpb l e v e l s d e d u c e d p o p u l a t i n g 7 - m u l t i p o l a r i t y . PRLTA 47 1702. NUCLEAR REACTIONS 2 ° 7 p b ( p , p ' ) , E = 9 5 MeV; m e a s u r e d s t e p ' , 0 ) . 2°7Pb d e d u c e d l e v e l s , f l ( L ) . Semi-microscopic DWBA,DWIA c a l c u l a t i o n s . NUPAB 386 45. NUCLEAR REACTIONS nSSn,a°spb(aHe,(x),E=283 MeV; m e a s u r e d cr(E(x),a(0), nSSn l e v e l s d e d u c e d CaS,lgg/2,1f5/2,lfT/2 n e u t r o n h o l e s t r e n g t h f r a g m e n t a t i o n . 2°Tpb d e d u c e d n o g9/2 s t r e n g t h concentration. DWBA a n a l y s i s . PYLBB 114 103. R A D I O A C T I V I T Y z°~Bi; m e a s u r e d 7(X-ray)-coin; deduced subshell capture probabilities, Q(EC). NUPAB 388 498. R A D I O A C T I V I T Y 2°TAt; m e a s u r e d ET,IT,I(ce),ceT-coin. 2°7Po t r a n s i t i o n s deduced "y-multipolarity. IANFA 45 1865. R A D I O A C T I V I T Y a°VAt; m e a s u r e d ET,I3',I(ce),77-,7(ce)-coin. 2°~Po d e d u c e d levels,J jr, 7-multipolarity. IANFA 45 2102. R A D I O A C T I V I T Y 2°TAt; m e a s u r e d ET,17,I(ce),ceT-coin. Z°7po t r a n s i t i o n s deduced 7-multipolarity. IANFA 45 1865. RADIOACTIVITY 2°7At; m e a s u r e d ET,IT,I(ce),77-,7(ce)-coin. 267po d e d u c e d tevels,J,Tr, ~/-multipolarity. IANFA 45 2102.

A Zospb

=

KEYWORDS

R A D I O A C T I V I T Y 2°SAt; m e a s u r e d E T , I T , I ( c e ) , ( e e ) ~ / - c o i n . a°SPo d e d u c e d levels,J,Tr,ICC, -y-branching. Ge(Li),Si-Li detectors,magnetic spectrometer. IANFA 46 45. R A D I O A C T I V I T Y 21°,a°s,2°s,a°4At,alZFr; m e a s u r e d E(x,I(x; d e d u c e d ( x - b r a n c h i n g . 7r s q u a r e - r o o t two magnetic spectrometer. IANFA 45 1861. RADIOACTIVITY zl°,z°s,z°6,Z°4At,ZlZFr; m e a s u r e d E(x,l(x. 2°a,z°4,~°sBi,Z°SAt d e d u c e d l e v e l s , (x-branching,hindrance f a c t o r , J j r . IANFA 45 1966. R A D I O A C T I V I T Y 2°SAt; m e a s u r e d ET,IT,I(ce),(ee)7-eoin. 2°6po d e d u c e d levels,J,w,lCC, 7-branching. Ge(Li),Si-Li detectors,magnetic spectrometer. IANFA 46 45.

A Zo7pb

AND

308

=

NUCLEAR MOMENTS 2°°,2°l,2°2,2°3,2°4,2°5,2°s,2°7,2°Spb; m e a s u r e d h f s . 2°°,2°2,2°4,2°6Pb d e d u c e d isotopes shifts,rms r a d i i . 2°1,2°3,2°5,2°7pb d e d u c e d isotope shifts,rms radii,p`. High resolution l a s e r s p e c t r o s c o p y . ZPAAD 305 89. NUCLEAR REACTIONS 58Ni,208Pb(7,7),E < 10 MeV; m e a s u r e d at0). 58Ni d e d u c e d levels,Jjr,rT,E1, MI t r a n s i t i o n strength. Z°sPb l e v e l s d e d u c e d F'y. E n r i c h e d targets,nuclear resonance fluorescence technique. NUPAB 372 1. NUCLEAR REACTIONS 1 1 6 S n , 5 S N i ( a , ( x ) , ( ( x , a ' ) , E = 4 8 0 MeV; 208Pb((x,c~),((x,a'),E=340,480 MeV; m e a s u r e d or(0); d e d u c e d G ( t o t a l ) . 2 ° s P b , n S S n d e d u c e d g i a n t r e s o n a n c e e x c i t a t i o n . FZKAA 13 83. NUCLEAR REACTIONS 2°spb((x,~'n),E=104 MeV; m e a s u r e d n(x coin,E(x,En. 2°spb d e d u c e d GQR branching r a t i o . 2°TPb l e v e l s d e d u c e d p o p u l a t i n g 7-multipolarity. PRLTA 47 1702. NUCLEAR REACTIONS 2 ° S p b ( 7 , n ) , E = 9 . 9 - 1 1 . 2 MeV; m e a s u r e d G(En,0); d e d u c e d multipole interference e f f e c t s . 2 ° s p b d e d u c e d E1 s t r e n g t h distribution. PRVCA 25 791. NUCLEAR REACTIONS 16,1SO,24Mg,28Si,32S,36Ar,4OCa,54Cr,144,152,154Sm,2°sPb,Z32Th(polarized d,d), (polarized d , d ' ) , E = 1 8 - 2 3 MeV; m e a s u r e d (y(0),iTn(0). 16,180,24Mg,28Si,32S,36Ar,4°Ca,54Cr,144, 152,154SITI,2°8pb,232Th l e v e l s d e d u c e d i s o s e a l a r q u a d r u p o l e , o c t u p o l e transition s t r e n g t h . 154 152,144Sm,232Th d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082. NUCLEAR REACTIONS 2°sPb(p,p'),E=201 MeV; m e a s u r e d or(0), a°sPb d e d u c e d c o l l e c t i v e s t a t e , g i a n t r e s o n a n c e e x c i t a t i o n s t r e n g t h s . M a c r o s c o p i c D W B A , m i c r o s c o p i c DWIA a n a l y s e s . NUPAB 380 42. NUCLEAR REACTIONS 9°Zr,12°Sn,144Sm,2°spb(p,p'),E=800 MeV; m e a s u r e d (7(0). 9°Zr,lZ°Sn,144Sm, Zospb,4°Ca,5SNi d e d u c e d d e f o r m a t i o n lengths,neutron,proton matrix element ratios. Optical m o d e l , D W B A a n a l y s e s . PRVCA 25 408. NUCLEAR REACT]ONS 54,56Fe,SS,6ONi,lZ°Sn,Z°sPb(polarized n , n ' ) , E - 1 0 MeV; m e a s u r e d A(0). 54 56Fe,5S,S°Ni,lU°Sn,2°sPb l e v e l d e d u c e d s p i n - o r b i t to C o u l o m b d e f o r m a t i o n parameter ratio. Coupled-channels a n a l y s i s . PRVCA 25 2854. NUCLEAR REACTIONS a s s P b ( e , e ' ) , E - 5 0 - 3 3 5 MeV; m e a s u r e d g(E(e'),0). Z°sPb l e v e l s d e d u c e d transition charge,current d e n s i t i e s . DWBA a n a l y s i s . PRVCA 25 229~.

87

KEY

NUMBERS

A ~oapb

R 82HilO: 82Le14: 82Pa05: 82Sa19:

82St03: 82Wi06: 82Wo08:

82Ya02:

~Oapo

D 81Va26: 82Dr02:

aOaAt

D 81Va26: 81Va27: 81Va29: 82DrO2:

D 81Di14:

~Ogpb

R 82Ki05:

aogBi

D 81Di14:

J 81Ph01: R 82Sa19:

~OgAt

R 79Su15:

R 82No10:

a~OAt

D 81Va27: 81Va29:

208

continued

=

209

RADIOACTIVITY a29Th,aa5Ra,225Ac,221Fr,21aBi,2°gT1; m e a s u r e d ET,I 7 f o l l o w i n g a - d e c a y , f l - d e c a y . 225Ra,22SAe,221Fr,217At,a~aBi,2°OTl,Z°gBi l e v e l s d e d u c e d absolute I% 213po d e d u c e d levels, a b s o l u t e I% RRALA 47 331. NUCLEAR REACTIONS 2°aPb(n,~),E=7-13 MeV; m e a s u r e d a(0). 2°gPb levels d e d u c e d dipole EWSR i n GDR r e g i o n . D i r e c t - s e m i d i r e c t , p u r e r e s o n a n c e m o d e l c a l c u l a t i o n s . NUPAB 384 129. RADIOACTIVITY 2Z9Th,a~SRa,225Ac,221Fr,ZlaBi,209T1; m e a s u r e d ET,I~/ f o l l o w i n g a - d e c a y , f l - d e c a y . 2ZSRa,225Ac,221Fr,217At,21aBi,299Tl,UOOBi l e v e l s d e d u c e d absolute I7. 21aPo d e d u c e d levels, a b s o l u t e I~/. RRALA 47 331. NUCLEAR MOMENTS 2°gBi; m e a s u r e d m u o n i c hfs; deduced h y p e r f i n e c o n s t a n t s . HPACA 54 648. NUCLEAR REACTIONS 16~'2~Mg~2~Si~4~Ar~4o~44~4~Ca'4~4~'5~Ti~54~6Fe'5~'6~'62~64Ni~9Y~9~Zr~9~'i~M~ 1 4 4 S m , 2 ° s P b , Z ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d a(0),A(0); deduced optical model parameters, l°o,24Mg,2aSi,4°A r,4°,44,4eCa,46,48,5°Ti,54,SSFe,58,s°,62,64Ni,agY,9°Zr,Oa,19°Mo,144Sm, 2°sPb,2°gBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 944. NUCLEAR REACTIONS 197Au(IZC,F),E=72.5 MeV; m e a s u r e d f r a g m e n t b l o c k i n g p a t t e r n . 2°gAt d e d u c e d TI/2. Mica t r a c k d e t e c t o r . YTHLD 1 93.

A 2~Opo

=

KEYWORDS

NUCLEAR REACTIONS 2°aPb(e,e'),E=40.5,50.4,60.3,75.2 MeV; m e a s u r e d (7(0=180°). 2°aPb d e d u c e d levels,transverse form factors. Enriched target,magnetic spectrometer. PRVCA 26 920. NUCLEAR REACTIONS 2°8pb(7Li,%i),E=52 MeV; m e a s u r e d (r(0). 2°spb deduced lhg/~ n e u t r o n o r b i t rms radius,neutron excess distribution. NUPAB 382 115. NUCLEAR REACTIONS a°spb(e,e'),E n o t g i v e n ; m e a s u r e d G(O) v s m o m e n t u m t r a n s f e r . ~98pb levels deduced transition c h a r g e d e n s i t i e s . PYLBB 108 279. NUCLEAR REACTIONS ~4Mg~2~Si~4~Ar~4~4~4~Ca~46~48~Ti~4~56Fe~5~6~a~6~Ni~89Y~9~Zr~8~M~ 1 4 4 S m , 2 ° a P b , 2 ° g B i ( p o l a r i z e d p , p ) , E = 6 5 MeV; m e a s u r e d (~(0),A(0); d e d u c e d optical model parameters. 160,~4 Mg,~aSi,4°A r,4°,44,48Ca,46,4a,sgTi,Sa,56Fe,5a,6°,6~,s4 Ni,sgy,99Zr,98,1OOMo,144Sin, ~°aPb,~°gBi d e d u c e d p o i n t n u c l e o n d i s t r i b u t i o n . PRVCA 26 9 4 4 . NUCLEAR REACTIONS 2°6,~°spb(7,-/),E=9.5-12 MeV; m e a s u r e d a(0,E). ~°sPb d e d u e e d p o s s i b l e r e s o n a n c e , F . ~°aPb d e d u c e d f i n e s t r u c t u r e dipole assignment. PRVCA 25 780. NUCLEAR REACTIONS 2°8Pb(polarized %7),E=10 MeV b r e m s s t r a h l u n g ; m e a s u r e d E % I % a s y m m e t r y . 2°aPb d e d u c e d l e v e l , J , r r , B ( M 1 ) , F o a / F . L i n e a r l y p o l a r i z e d b e a m . PRLTA 49 18. NUCLEAR REACTIONS 2 ° 8 P b ( t , a ) , E = 8 . 5 , 9 MeV; 2 ° 8 p b ( t , t ) , E = 8 . 5 , 9 , 1 0 , 1 2 MeV; m e a s u r e d a(0), a ( E a ) ; d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . ~°8Pb d e d u c e d s i n g l e p r o t o n s t a t e S , r m s r a d i u s , b i n d i n g e n e r g y . DWBA a n a l y s i s . PYLBB 116 320. NUCLEAR REACTIONS 1 4 4 S m ( a , a ' ) , E = 8 3 . 8 , 9 9 . 1 , 1 0 8 . 6 MeV; Z ° s P b ( a , ( x ' ) , E = 8 3 . 8 , 8 9 , 1 1 8 . 7 MeV; m e a s u r e d a(0,E). 144Sm,2°aPb d e d u c e d g i a n t m o n o p o l e , q u a d r u p o l e resonances,F,deformation parameters fl(L). D i p o l e p l u s t r i p l e t quadrupole magnetic detection system,enriched t a r g e t . DWBA a n a l y s i s . NUPAB 381 277. RADIOACTIVITY ~°8At [ f r o m T h ( p , X ) , E = 6 6 0 MeV3; m e a s u r e d E%I-/,I(ce). 2°SPo t r a n s i t i o n s deduced 7-multipolarity. Ge(Li),Si-Li detectors,magnetic spectrometers. IANFA 45 1841. RADIOACTIVITY ~°SAt [ f r o m ~°gBi(aHe,4n),E=38.5 MeV]; m e a s u r e d ET,I%I(ee ). a°apo d e d u c e d transition energy,subshell ICC r a t i o s . CZYPA 32 711. RADIOACTIVITY a°aAt [ f r o m T h ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d ET,lT,I(ce). 2°8po t r a n s i t i o n s deduced 7-multipolarity. Ge(Li),Si-Li detectors,magnetic spectrometers. IANFA 45 1841. RADIOACTIVITY 21°,2°a,z°6,~°4At,2~Fr; m e a s u r e d E a , l a ; d e d u c e d a - b r a n c h i n g . 7r s q u a r e - r o o t two magnetie spectrometer. IANFA 45 1861. RADIOACTIVITY 21°,2°8,296,2°4At,212Fr; m e a s u r e d E a , I a . 2°2,2°4,2°SBi,2°SAt d e d u c e d l e v e l s , a-branching,hindrance f a c t o r , J , T r . IANFA 45 1968. RADIOACTIVITY 2°aAt [ f r o m a°gBi(3He,4n),E=38.5 MeV~; m e a s u r e d ET,I%I(ce). a°8Po d e d u c e d transition energy,subshell ICC r a t i o s . CZYPA 32 711.

A 209T1

AND

=

210

NUCLEAR REACTIONS a°gBi(p,F),E=60 MeV; m e a s u r e d f i s s i o n f r a g m e n t mass distribution, T-multiplicity first,second moments, < E7 >; d e d u c e d scission point shell effects, fragment spin dependence on rotational m o d e s . ZZ°Po d e d u c e d fission mechanism. Moretto-Schmitt m o d e l . PRVCA 26 1114. R A D I O A C T I V I T Y 21°,2°s,2°6,2°4At,212Fr; m e a s u r e d E a , l a ; d e d u c e d a - b r a n c h i n g . ~r s q u a r e - r o o t two magnetic spectrometer. 1ANFA 45 1861. RADIOACTIVITY 21°,2°s,a°6,Z°4At,g12Fr; m e a s u r e d E a , I a . 2°2,2°4,2°°Bi,2°SAt d e d u c e d levels, a-branching,hindrance f a c t o r , J , T r . IANFA 45 1966.

88

KEY

NUMBERS

A

ZiOAt

D 82Lo18:

aiORn

R 82Po03:

D

82Bo04:

210

:

KEYW0RDS

continued

R A D I O A C T I V I T Y 2~°At [ f r o m aogBi(a,3n)]; measured ET,1-/,y(0),Ty-coin,Tl/a,I(ce); deduced levels,isomer,J,~r,eonfiguration,multiplet splitting,y-multipolarity,E1 transition hindrance f a c t o r . J P H G B 8 L153. NUCLEAR REACTIONS a°STl(l°B,Sn),E ~ 70 MeV; 198pt(lSO,4n),E ~ 90 MeV; igSpt(170,5n),E a 96 MeV; m e a s u r e d yy-,ny-coin,nT(t),Ey,17,7(0),ICC, a~°Rn d e d u c e d l e v e l s J , r r , T , c o n f i g u r a t i o n s , yrast traps. Ge(Li),Ge,NESl3,Si-Li detectors,enriched targets. Shell-model. NUPAB 380 335.

A

anpo

AND

=

211

RADIOACTIVITY •5•••5•Dy••••••5•m••5•••52mH•••5•••5•E••••3•••4•••4mTm••79••78••77••7•P•••••Yb••9•••97m•

199mpo,alaFr,alaRa

[from

U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d E a , T l / z . 149Tb,all,a14,als,alS,alTAt, [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 35 941. NUCLEAR REACTIONS a ° g B i ( d , y ) , E = 8 - 1 1 . 5 MeV; m e a s u r e d a(E),a(ground state)/a(isomer), zn alimpo deduced T,particle emission branching r a t i o . NUPAB 380 493. R A D I O A C T I V I T Y ~ 5 ~ 1 5 1 D y ~ 5 i ~ i 5 ~ m ~ 5 ~ 5 ~ m H ~ 1 ~ i 5 ~ E r ~ 5 ~ 5 4 ~ 5 4 m T m ~ 7 9 ~ 7 8 ~ 7 7 ~ 7 6 P t ~ 5 ~ Y b ~ i 9 ~ 197m, ~9~mpo,a~aFr,a~aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,T~/a. 149Tb,aU,z14,2~s,als,Z~TAt, a°4,a~a,algFr,aU,anm,a~a,ai3,a~4po,alT,alSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. PRVCA 35 941.

2°4,218,219Fr,all,211rn,a12,213,a14po,217,alSRn R alIAt

82Ze03:

D 82Bo04:

A Slaps

D 82BeO9

83Bo04

aiaAt

R 82LoOl

a~aFr

D 81Va27 81Va29

alaRa

D 8~Bo04

D 81Di14

213po

D 81Di14

82Bo04

213Fr

D 82Bo04

312

R A D I O A C T I V I T Y ZaSTh [ f r o m natural aaSTh]; m e a s u r e d E y , I y , t ( c e ) , y y ( O ) , f l a ( t ) . ZiaPo l e v e l s deduced J. S l a P s l e v e l d e d u c e d Tl/a,nuclear strength parameter,B(E2),a-width. Ge(Li), Nal(Tl) detectors,plastic scintillators surface-barrier silicon detector,magnetic fl-ray spectrometer. N U P A B 378 1. R A D I O A C T I V I T Y 15°,151Dy,151,~5~m,15a,152mHo,iSa,153Er,153,154,154mTm,179,178,177,176pt,~SSy b,lOS,197m, ~gOmpo,alaFr,a~aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d E a , T l / a . 149Tb,a~l,a~4,a15,zia,ZiTAt, a°4,ais,algFr,aU,ZUm,a~2,z~a,a~4Po,a~v,ZlSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. NUCLEAR REACTIONS 2 ° 9 B i ( ~ , n ) , E = 1 8 - 2 8 MeV; m e a s u r e d yT-,(X-ray)y-coin,T~/2,1%I(ce),7(0), a ( E T ) . 2~aAt d e d u c e d levels,J,Tr,configurations,B(k). N U P A B 376 ~9. R A D I O A C T I V I T Y 21°,z°s,a°6,a°4At,alaFr; m e a s u r e d Ea,Ia; deduced a-branching, m" s q u a r e - r o o t two magnetic spectrometer. I A N F A 45 1861. R A D I O A C T I V I T Y 2~°,a°8,a°s,a°4At,a~aFr; m e a s u r e d E a , I a . a°a,a°4,2°SBi,a°SAt d e d u c e d levels, a-branching,hindrance f a e t o r , J , v r . I A N F A 45 1966. RADIOACTIVITY ~i~iDy~i5i~i5'm~'i~mH~i~a~Er~i53~4~54mTm~i7~i7~7'i7sPt~5~Yb~9~ xoTm, 199mpo,alaFr,ZlZRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,Tl/a. 149Tb,Zll,a~4,a~5,als,ZlTAt, a°4,als,a~gFr,an,aUm,a~a,a~a,a~4po,alT,a~aRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A alaBi

=

=

213

R A D I O A C T I V I T Y 229Th,aZ5Ra,SZSAc,ZSlFrY3Bi,Z°OT1; m e a s u r e d E7,1~ f o l l o w i n g a - d e c a y , f l - d e c a y . 2aSRa,a25Ac,aSlFr,a~TAt,~'3Bi,2°gTl,a°gBi l e v e l s d e d u c e d absolute IT. 213po d e d u c e d levels, a b s o l u t e 17. R R A L A 47 331. R A D I O A C T I V I T Y aZgTh,aZ5Ra,aZSAc,SalFr,Zl3Bi,2°gT1; m e a s u r e d Ey,I7 f o l l o w i n g a-decay,fl-decay. 225Ra,a25Ac,SZlFr,aiTAt,a13Bi,Z°gTl,2°gBi l e v e l s d e d u c e d a b s o l u t e 17. a!3po d e d u c e d l e v e l s , absolute I7. R R A L A 47 331. R A D I O A C T I V I T Y •••••5•Dy••5•••••rn•i52••52mH••••2••53Er••5••154••54mTm••79••78••77••76Pt•••5Yb••9•' 197m, logmpo,U13Fr,ZlaRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d E a , T I / m 140Tb,all,el%els,21s,alTAt, 2o4,als,219Fr,211,211m,212,z13,a14po,ZlT,alSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y ~5~'15~Dy~5~'~5~m'~52~i5~mH~5~53E~53~154~1~4mTm'179~17~'~77~176Pt~5Yb~98~ 197m, 199mpo,ZJ3Fr,ZlZRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,T1/2. la9Tb,Zn,ul4,zls,uls,217At, 2°4,218,219Fr,a~l,211r",21z,sla,214Po,alT,alSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 35 941.

89

KEY

NUMBERS

A 2~4pb

D 82Fa10

a*4Bi

D 82FalO

2i4po

D 82Bo04

Z~4At

D 82Bo04

82EwOl:

AND

=

D 8~BoO4

D 82Bo04

D 81Di14

82Bo04

a,TRn

D 82Bo04

atTAc

R 82Ri06

=

=

D 82Va09 D 82Bo04

218Fr

D 82Bo04

82Ew01

217

R A D I O A C T I V I T Y aagTh,aaSRa,225Ac,2alFr,213Bi,269Tl; m e a s u r e d E7,I7 f o l l o w i n g a - d e c a y , f l - d e c a y . aaSRa,225Ac,aalFr,ZlTAt,2~SBi,a°gTl,2°gBi l e v e l s d e d u c e d absolute I7. alSPo d e d u c e d levels, a b s o l u t e 17. R R A L A 47 331. RADIOACTIVITY 15°,tSlDy,151,15Im,15a,15amHo,lSa,153Er,153,154,154mTm,179,17s,177,176pt,155y b,198,t97m 199mpo,a13Fr,ai2Ra [-from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea,TI/2. 149Tb,211,2'4,215,~ls,217At, 2°4,ais,a19Fr,aH,aHm,aiz,ais,a~4po,a~7,~SRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. PRVCA 25 941. RADIOACTIVITY 15°,Â51Dy,151,151m,15a,15am Ho,15z,i53Er,153,154,154mTm,179,178,177,176pt,155y b,198,197m, ~99mpo,a~aFr,a1~Ra [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea,T~/a. ~49Tb,a~1,~i4,z*5,~16,a~TAt, a°4,2ls,al9Fr,211,aHm,21z,ais,~14po,217,a~SRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. PRVCA 25 941. NUCLEAR REACTIONS 197Au(a6Ne,pF),(a°Ne,dF),(2°Ne,tF),(a°Ne,aF),E=265 MeV; measured fission f r a g m e n t ( l i g h t partiele)-coin,
A 21Spo aiSRn

216

RADIOACTIVITY ~5~iDy~i5i~i~m~15a~*5~mH~*5~53Er~i53~'54~54mTm~i79~i7~77~76Pt~t55Yb~98~97m~ 199mpo,ai3Fr,a~Ra [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea,T~/z. '49Tb,Zil,214,z*5,ais,2'TAt, ~°4,ais,aigFr,~i',alim,ala,ai3,a'4po,alT,aiSRn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. PRVCA 25 941.

A al7At

215

RADIOACTIVITY ~5~5~Dy~5~5~m~52~52mH~52~53Er~53~i54~54mTm~I79~78~77~I76Pt~55Yb~I98~97m~ 199mpo,213Fr,a~Ra [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; m e a s u r e d E a , T I / a . *~gTb,~n,a~4,2ts,~,a~At, 2°4,218,219Fr,211,211m,21z,213,214po,217,218Rn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941.

A a,SAt

214

R A D I O A C T I V I T Y ea°Ra(a),al4pb(fl-),2'4Bi(a),(fl-); measured relative I7. H i g h r e s o l u t i o n Ge(Li) d e t e c t o r s , Z Z a R a s o u r c e , d a u g h t e r s in equilibrium. NUIMA 200 593. R A D I O A C T I V I T Y Za~Ra(a),e~4Pb(fl-),e~4Bi(a),(fl-); m e a s u r e d relative I7. H i g h r e s o l u t i o n Ge(Li) d e t e c t o r s , 2 2 6 R a s o u r c e , d a u g h t e r s in equilibrium. NUIMA 260 593. R A D I O A C T I V I T Y 15°,151Dy,151,151 m,15~,z 5amH o,i 52,153 EF,153,154,154 mTm,179,178,177,17{~pt,155y b,198,197 rn, *99mpo,~lSFr,212Ra [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,TI/2. 14STb,2ii,~14,215,216,217At, z°4,~s,algFr,all,al~m,ala,ats,al4po,alT,2~aRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y ~ 5 o ' ~ 5 i D y ~ ' i ~ m ~ i ~ 5 z m H ~ ' i 5 a ' i 5 3 E r ~ i 5 3 ' i 5 4 ~ 1 5 4 m T m ' i 7 9 ' ~ 7 8 ~ 7 7 ~ 7 6 ~ t ~ i 5 5 Y b ' i 9 8 ~ 197m, t99mpo,213Fr,aiaRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,Tl/~. *49Tb,Zn,a14,a*5,z~s,alTAt, z°4,zls,algFr,Zil,Ztim,Zla,z13,a14po,aiv,a18Rn [ f r o m U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y ZlSFr [ f r o m Z38U(p,15n6p),chemical mass separation]; a~4At [ f r o m Z~SFr(a-decay)]; measured Ea,Ia,T~/~,aa-coin. ~lSFr d e d u c e d i s o m e r d e c a y c h a r a c t e r i s t i c s . 214At d e d u c e d l e v e l s , J j r , c o n f i g u r a t i o n . Surface barrier s i l i c o n d e t e c t o r s . NUPAB 380 423.

A = ~,SAt

KEYWORDS

218

R A D I O A C T I V I T Y a18po; m e a s u r e d E a , I a , T 1 / 2 . P R V C A 25 2802. RADIOACTIVITY ~5~5~Dy~5~5~m~52~52mH~52~53Er~53~54~1~4mTm~79~78~77~7~Pt~155Yb~98~97m~ 199mpo,alaFr,a12Ra [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeVS; m e a s u r e d Ea,T1/a. 149Tb,aJl,a14,a15,a16,217At, a°4,als,a*9Fr,all,alim,ala,ala,ai4po,alT,alSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 15°,151Dy,lSl,t51m,152,iSam Ho,15a,153Er,153,154,154mTm,179,178,177,176pt,155y b,19s,197m, 199mpo,alSFr,21aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV3; m e a s u r e d Ea,Tj/a. 149Tb,all,a14,als,a~6,217At, a64,a18,algFr,aH,allm,alz,ala,214po,a17,alSRn [from U,Th,Au,Ta(p,X),E=5 GeV]; measured Ea. Helium jet recoil product separation. P R V C A 25 941. R A D I O A C T I V I T Y 2*8Fr [ f r o m a38U(p,15n6p),chemieal mass separation]; Zi4At [from alSFr(a-decay)3; measured Ea,la,T1/a,aa-coin. alSFr d e d u c e d i s o m e r d e c a y c h a r a c t e r i s t i c s . al4At deduced levels,J,rr,configuration. S u r f a c e b a r r i e r s i l i c o n d e t e c t o r s . NUPAB 380 423.

90

KEY

NUMBERS

A algFr

D 82Bo04:

D 81Di14

D 81V328

=

=

D 81Di14

aaSAc

D 81Di14

D 82Ak03 82Fa10

D

81Va38 82An02:

D 82Ru04

a28Ra

D 82Ru04

3eaTh

D 82Be09

D 81Di14

225 f o l l o w i n g a - d e c a y , f l decay. IV. al3po d e d u c e d levels, following a-decay,fl-deeay. IT. a*apo d e d u c e d levels,

326

=

237

=

228

RADIOACTIVITY aeSFr [ f r o m a a S U ( p , 5 n 6 p ) , m a s s s e p a r a t i o n ] ; m e a s u r e d EV,IT,TT-coin,Tw2; d e d u c e d log f t . aZaRa d e d u c e d l e v e l s , J j r . Ge(Li) d e t e c t o r s . NUPAB 383 1. RADIOACTIVITY 2ZSFr [ - f r o m a a S U ( p , 5 n 6 p ) , m a s s s e p a r a t i o n ] ; m e a s u r e d ET,IT,T'Y c o i n , T l / z ; d e d u c e d log f t . ZZSRa d e d u c e d l e v e l s , J , r r . Ge(Li) d e t e c t o r s . NUPAB 383 1. R A D I O A C T I V I T Y aaSTh [ f r o m n a t u r a l aaeTh]; m e a s u r e d ET,iT,I(ce),TV(0),fla(t). elaPo l e v e l s d e d u c e d J. alapo l e v e l d e d u c e d T w 2 , n u c l e a r strength parameter,B(E2),a-width. Ge(Li), NaI(TI) detectors,plastic scintillators surface-barrier silicon detector,magnetic fl-ray spectrometer. NUPAB 378 1.

A

2agTh

transitions,

RADIOACTIVITY a27Ac; m e a s u r e d EV,Iv f o l l o w i n g a - d e c a y . 2eaFr d e d u c e d transitions, T branching,T-multipolarity. Ge(Li) d e t e c t o r . IANFA 45 1895. R A D I O A C T I V I T Y 227Ac [ f r o m ea~pa a - d e c a y ] ; measured Ey,Iy,yy(O,t),y(a),oriented nuclei. a37Ac l e v e l s d e d u c e d J j r , 6 . G e ( L i ) , i n t r i n s i e Ge d e t e c t o r s , P a G d s o u r c e . JPHGB 8 369.

A 32SFr

=

deduced

RADIOACTIVITY 22SRa; m e a s u r e d ET,IT f o l l o w i n g a - d e c a y , f l - d e e a y . RRALA 51 1. RADIOACTIVITY e a 6 R a ( a ) , a 1 4 p b ( f l - ) , a ' 4 B i ( a ) , ( f l - ) ; m e a s u r e d relative I V. H i g h r e s o l u t i o n Ge(Li) d e t e c t o r s , a e 6 R a s o u r c e , d a u g h t e r s in e q u i l i b r i u m . NUIMA 200 593.

A Z27Ae

223

RADIOACTIVITY aaaTh,2a5Ra,aa5Ac,2alFr,alaBi,2°gT1; m e a s u r e d ET,17 eeSRa,eeSAe,eZlFr,alTAt,eiaBi,a°gTl,a99Bi l e v e l s d e d u c e d absolute a b s o l u t e IV. RRALA 47 331. RADIOACTIVITY 239Th,aeSRa,aaSAe,aalFr,alaBi,a°gTl; m e a s u r e d ET,IT 225Ra,aaSAe,aalFr,217At,213Bi,aOgTl,a°gBi l e v e l s d e d u c e d absolute a b s o l u t e I V. RRALA 47 331.

A eZSRa

221

RADIOACTIVITY ZeTAc; m e a s u r e d ET,IT f o l l o w i n g a - d e c a y . 3eaFr v-branching,y-multipolarity. Ge(Li) d e t e c t o r . IANFA 45 1895.

A = a25Ra

219

RADIOACTIVITY aegTh,ae5Ra,ZeSAc,aelFr,eiaBi,Z°gT1; m e a s u r e d EV,IT f o l l o w i n g a - d e e a y , f l - d e c a y . ea5Ra,ZZSAe,eZlFr,elTAt,e~aBi,a°UTl,aOgBi l e v e l s d e d u c e d absolute 17. aiapo d e d u c e d levels, a b s o l u t e IV. RRALA 47 331.

A 223Fr

=

KEYWORDS

R A D I O A C T I V I T Y 15~5~Dy~5~5~m~5~52mH~52~5~Er~153~54~54mTm,~79~78~77~76Pt~55Yb~198~97m~ 199mpo,alaFr,21aRa [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea,TI/z. 149Tb,an,314,els,e16,a17At, 2o4,ais,algFr,en,el~m,21e,ala,a14po,e~7,Z*SRn [ f r o m U , T h , A u , T a ( p , X ) , E = 5 GeV]; m e a s u r e d Ea. H e l i u m j e t r e c o i l p r o d u c t s e p a r a t i o n . PRVCA 25 941.

A ZelFr

AND

-

E29

R A D I O A C T I V I T Y eegTh,Z25Ra,ZeSAe,ZZlFr,a13Bi,2°gT1; m e a s u r e d ET,IT f o l l o w i n g c ~ - d e c a y , f l - d e c a y . 225Ra,aeSAe,ZalFr,e17At,2~3Bi,a°OT1,2°gBi l e v e l s d e d u c e d absolute IV. alaPo d e d u c e d levels, a b s o l u t e IT. RRALA 47 331.

91

KEY

NUMBERS

A 230Th

R 82NaO6:

D 82Va04:

231pa

R 82Ku07:

asymmetric

fission

82Ch21:

82C101:

82C103:

82Ha02: 82Ha03:

82Ha34: 82Kn03: 82Mo11:

820w01:

82Ra21:

82Si03: 232pa

R 82Ku07:

asymmetric

fission

820106:

=

heights.

Statistical

model.

PRVCA 25 3011.

232

barrier

A

R 82Er03:

231

NUCLEAR REACTIONS 232Th(e,F),E=5.5-7 MeV; m e a s u r e d o r ( f r a g m e n t 0). 232Th deduced E2 fission p r o b a b i l i t y , E W S R . N a t u r a l t a r g e t . PRVCA 25 1689. NUCLEAR REACTIONS 232Th,238U(n,n'v),E=0.8-2.5 MeV; m e a s u r e d T - y i e l d s ; d e d u c e d a ( i n e l a s t i c ) v s E. 232Th,a3Su d e d u c e d levels,J,~r,K,rotational,vibrational bands,band parameters. Compound nucleus,direct interaction m o d e l a n a l y s i s . PRVCA 26 841. NUCLEAR REACTIONS 16,1So,24Mg,28Si,a2S,36Ar,4°Ca,54Cr,144,1sa,154Sm,2°sPb,aa2Th(polarized d,d), (polarized d , d ' ) , E = 1 8 - 2 3 MeV; m e a s u r e d cr(0),iT11(0). 16,1aO,24Mg,28Si,32S,36Ar,4°Ca,54Cr,144, 152,154Sm,2°sPb,232Th l e v e l s d e d u c e d i s o s c a l a r q u a d r u p o l e , o c t u p o l e transition s t r e n g t h , i54 15a,144Sm,232Th d e d u c e d neutron,proton deformation differences. Q3D s p e c t r o g r a p h . C o l l e c t i v e m o d e l . PRLTA 48 1082. NUCLEAR REACTIONS 160,4o,48Ca,OOZr,144,152,154Sm,2°sPb,232Th(polarized d , d ) , ( p o l a r i z e d d,d'), E=20 MeV; m e a s u r e d G(0),iT11(0). 152,154Sm,232Th l e v e l s d e d u c e d s t a t i c m a s s q u a d r u p o l e moments. Coupled-channels a n a l y s i s . PYLBB 116 109. NUCLEAR REACTIONS 23ZTh,e38U(p,p),(p,p'),E=26 MeV; m e a s u r e d (~(0); d e d u c e d potential multipole moments. 232Th,238U d e d u c e d f12,f14. C o u p l e d - c h a n n e l s a n a l y s i s . PRVCA 25 189. NUCLEAR REACTIONS 23aTh,238U(~271,127I'),E=4.1 M e V / n u c l e o n ; a32Th,a38U(142Nd,142Nd'),E-5- .1 MeV/ nucleon; measured ET,IT,multiple Coulomb excitation,recoil in ferromagnetic Gd,~/(~27I) - , 7(142Nd)-coin. 232Th,23Su d e d u c e d h i g h - s p i n y r a s t s t a t e g , h i g h - j n u c l e o n a l i g m e n t . PRLTA 48 383. NUCLEAR REACTIONS a32Th,233,235,238 U,23g,242Pu(n,n),(n,n,),E_0_ . 6 - 3 . 4 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 232Th,a35,238U,23gPu l e v e l s d e d u c e d fla,fl4. NSENA 81 491. NUCLEAR REACTIONS 23aTh(%F),E=4.95-6.76 MeV b r e m s s t r a h l u n g ; m e a s u r e d f i s s i o n a(E). a32Th deduced inner,outer barrier heights,possible vibrational s t a t e s . PYLBB 116 315. NUCLEAR REACTIONS 23aTh,238U(a,a'),E=100,172 MeV; m e a s u r e d or(0). 232Th,a3Su d e d u c e d GQR, giant octupole,hexadecapole,monopole r e s o n a n c e s , F , m o n o p o l e s t r e n g t h s p l i t t i n g . PRVCA 25 2939. NUCLEAR REACTIONS 23ZTh,e34,236U(268pb,268Pb'~/),E=5.3 M e Y / n u c l e o n ; m e a s u r e d E(V),I(v)(0). 232Th,234,236U d e d u c e d l e v e l s , g r o u n d b a n d E2 t r a n s i t i o n matrix element. Enriched targets. NUPAB 388 421. NUCLEAR REACTIONS 23aTh(polarized 7,F),(7,F),E=10,12 MeV b r e m s s t r a h l u n g ; m e a s u r e d f i s s i o n a(fragment 0),asymmetry. 232Th d e d u c e d E1 e x c i t a t i o n r o l e i n f i s s i o n . L i n e a r l y p o l a r i z e d beam,parallel p l a t e a v a l a n c h e d e t e c t o r s . ZPAAD 308 63. NUCLEAR REACTIONS 2°sPb(23aTh,232Th'),E=5.6 M e V / n u c l e o n ; m e a s u r e d E%I%projectile C o u l o m b e x c i t a t i o n . 232Th d e d u c e d q u a s i p a r t i c l e , g r o u n d s t a t e b a n d c r o s s i n g . PYLBB 108 87. NUCLEAR REACTIONS 2 3 e T h ( p , F ) , ( p , n ) , ( p , 2 n ) , ( p , 3 n ) , E = 8 - 2 2 MeV; m e a s u r e d c r ( f i s s i o n ) , c r ( t o t a l ) , a(evaporation) v s E , p r o d u c t i o n G v s E f o r ST,88Kr,gl,92Sr,aS,97Zr,gTNb,ggMo,99Tc,l°3Ru,l°5Rh, 112pd,112 A g, 115 Cd, 115 I n , 127,12e, 129 S b , 132 Te, 135 I, 13S Cs, 141 ,143 Ce, 147 N d ,148,151pm . 233,232,231pa deduced

233Th

=

barrier

A R 82At05:

230

RADIOACTIVITY 235U,231Th; m e a s u r e d EV,Iv; d e d u c e d e m i s s i o n p r o b a b i l i t i e s . High p u r i t y Ge, S i - L i d e t e c t o r s . NUIMA 193 191. NUCLEAR REACTIONS a 3 2 T h ( p , F ) , ( p , n ) , ( p , 2 n ) , ( p , 3 n ) , E = 8 - 2 2 MeV; m e a s u r e d c r ( f i s s i o n ) , c r ( t o t a l ) , a(evaporation) v s E , p r o d u c t i o n a v s E f o r 87,88Kr,gl,a2sr,g5,gVZr,gTNb,ggMo,gSTc,163Ru,165Rh, 112pd,l12Ag,llScd,l15in,127,128,12gSb,132Te,1351,136Cs,141,143Ce,147Nd,149,151pm" 233,232,a3~pa deduced

232Th

=

KEYW0RDS

NUCLEAR REACTIONS 68zn,g°,g2,g4zr,g4,gs,gs,l°°Mo,la4Te,138Ba,142Ce,146Nd,15°Sm,a32Th(p,t),E=52 MeV; m e a s u r e d a ( E t , 0 ) . 9%n,96,g2Zr,92,94,96Mo,14°Ce,144Nd,148Sm,23OTh d e d u c e d d e e p t w o - h o l e s t a t e s . E n r i c h e d t a r g e t s . NUPAB 376 513.

A 231Th

AND

=

heights.

Statistical

model.

PRVCA 25 3011.

233

NUCLEAR REACTIONS Z3ZTh(n,F),E=reactor s p e c t r u m ; m e a s u r e d i n d e p e n d e n t yields f o r SZBr,S6Rb, 96,9aNb,iZsSb,136Cs. 233Th d e d u c e d c h a r g e d i s t r i b u t i o n parameters,even-odd proton,neutron enhancement factors. Activation,radiochemieal techniques. PRVCA 25 2519. NUCLEAR REACTIONS 232Th(n,X),E=0.007-15 eV,0.015-4 keV; m e a s u r e d t r a n s m i s s i o n ; d e d u c e d (7(E). 233Th d e d u c e d r e s o n a n c e s , p a r a m e t e r s , < FV >. NSENA 82 289.

92

KEY

NUMBERS

A

233pa

R 82Ku07

82Sa08

233 U

D 79Ce04

R 82Sa08

z34 U

D 80Ar23 R 81Sul0

82Ar14

820w01

82Pa14

~34Np

D 80Ar23

234pu

R 82Bo29

R 81Wa31:

aa5 U

D 83Va04: R 82De38:

82Ha34: 82Th04:

235Am

R 82Bo29:

continued

=

234

NUCLEAR REACTIONS 232Th(p,F),E=140,250,500,1000 MeV; 23aTh(d,F),E=70,140,500,1000 MeV; a3aTh(~,F),E=69.2,140,280,1000 MeV; m e a s u r e d ( f r a g m e n t ) ( f r a g m e n t ) ( 0 ) ; deduced dominating p r o c e s s e s , c o r r e s p o n d i n g r e g i o n s , a33,a34pa,a3SU d e d u c e d f o r w a r d m o m e n t u m transfer during f i s s i o n . PYLBB 110 372. R A D I O A C T I V I T Y a34Np(EC) [ f r o m a35U(d,3n),E=23 MeVS; m e a s u r e d ET,I 7. 234U d e d u c e d levels. RRALA 45 41. NUCLEAR REACTIONS z35,a36,Z38U,aa9pu(n,'y),E ~ 9.001-10 MeV; 238,S4°pu(n,7),E ~ 0.001-0.3 MeV; S33U(n,7),E ~ 0.002-1 MeV; measured ~(E). a34,23s,237,239U,a39,24°,241pu deduced n e u t r o n binding energy,average level widths. Statistical,direct s e m i - d i r e c t models. YTHLD 3 97. NUCLEAR REACTIONS 234U(e,F),E-5.5-85 MeV; measured fission G(fragment {9). as4,z36,Z38U deduced dominant fission channel K,multipolarity,E2 fission strength functions,GQR role. NUPAB 389 378. NUCLEAR REACTIONS 23aTh,234,aaSu(2°sPb,a°sPb'7),E=5.3 MeV/nucleon; measured E(7),l(7)(e). e3aTh,Z34,aSSu deduced levels,ground band E2 transition m a t r i x e l e m e n t Enriched targets. NUPAB 388 481. NUCLEAR REACTIONS aS3u(d,pF),E=13.5 MeV; measured Ep,fragment kinetic energies, velocities; deduced f r a g m e n t total kinetic energy,variance vs excitation. S34U deduced energy dissipation,scission configuration changes,fragmentation mode. Liquid drop mode]. NUPAB 382 31. RADIOACTIVITY 234Np(EC) [ f r o m 235U(d,3n),E=23 MeVJ; measured E7,17. 234U deduced levels. RRALA 45 41. NUCLEAR REACTIONS ZSMg,Z¢AI,5°Ti,S2Cr,SSFe,6~Ni(2°sPb,X),E=5.2-8 MeV/nucleon; measured ~(fragment 0,E) v s m a s s , a v e r a g e 7-multiplicity,E(X-ray),l(X-ray); 48Ca(a°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a ( f r a g m e n t 0,E) v s m a s s , a v e r a g e 7 - m u l t i p l i c i t y ; d e d u c e d a ( c a p t u r e ) , effective m o m e n t of inertia,coalescence model parameters, aa4pu,Z35Am,ZS~Fm,ZSs104,269106, aeSl08,27all0 deduced T~/~ limits. NUPAB 388 334.

A a35Th

= 233

KEYWORDS

NUCLEAR REACTIONS 2 3 2 T h ( p , F ) , ( p , n ) , ( p , 2 n ) , ( p , 3 n ) , E = 8 - 2 2 MeV; m e a s u r e d ( ~ ( f i s s i o n ) , g ( t o t a | ) , ~(evaporation) vs E,produetion avs E f o r 87,88Kr,9~,9~Sr,95,97Zr,97Nb,99Mo,9~Tc,~°3Ru,l°SRh, t~apd,~aAg,~sCd,~Sln lzT,~zu,IZSSb,13ZTe,t35i,~3~Cs,~41,143Ce,147Nd,149,15~pm" a33,232,a3~pa deduced asymmetric f i s s i o n b a r r i e r h e i g h t s . S t a t i s t i c a l m o d e l . PRVCA 25 3011. NUCLEAR REACTIONS 23~Th(p,F),E=140,250,500,lO00 MeV; Z3aTh(d,F),E=70,140,500,1000 MeV; ~3aTh((x,F),E=69.2,140,280,1000 MeV; m e a s u r e d ( f r a g m e n t ) ( f r a g m e n t ) ( 0 ) ; deduced dominating p r o c e s s e s , c o r r e s p o n d i n g r e g i o n s . 233,234pa,a36U d e d u c e d f o r w a r d m o m e n t u m transfer during f i s s i o n . PYLBB 110 373. R A D I O A C T I V I T Y e33U,~a~Np,~3s,aas,za°,~4~Pu,24~Am; m e a s u r e d ET,I~/. ENNLA 26 526.

A a34pa

AND

=

335

NUCLEAR REACTIONS 153Gd(n,(x),5°V(n,p),E=thermal; m e a s u r e d (r(Ea),~(Ep); d e d u c e d Q. ~SaGd d e d u c e d m a s s . 5°V,5°Ti,153Gd,lS°Sm d e d u c e d m a s s d i f f e r e n c e , a35Th d e d u c e d m a s s . A n a l y z e d (n, a ) data,238U m a s s i n p u t . NUIMA 190 167. R A D I O A C T I V I T Y aanu,a31Th; m e a s u r e d ET,IT; d e d u c e d e m i s s i o n p r o b a b i l i t i e s . High p u r i t y Ge, S i - L i d e t e c t o r s . NUIMA 193 191. NUCLEAR REACTIONS 23s,a38U(7,F),E=I2,50,20,30 MeV b r e m s s t r a h l u n g ; measured fractional, independent,cumulative fission chain yields for Br,Kr,Rb,Sr,Zr,Sn,Sb,l,Te,Xe,Cs,Ba,La isotopes; deduced fragment charge distribution,most p r o b a b l e c h a r g e . 235,Z38U d e d u c e d width parameter,postneutron m a s s v s e x c i t a t i o n e n e r g y . PRVCA 26 1356. NUCLEAR REACTIONS 2 3 Z T h , e a a , a a s , a 3 8 U , 2 3 9 , 2 4 2 p u ( n , n ) , ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d ~(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . ZS~Th,aa5,238U,239pu l e v e l s d e d u c e d f12,f14. NSENA 81 49I. NUCLEAR REACTIONS 235,238U(7,F),E=12,15,20,30 MeV b r e m s s t r a h l u n g ; measured independent i s o m e r i c y i e l d r a t i o o f 134I. Z35,338U d e d u c e d r m s (J) v s e x c i t a t i o n . A c t i v a t i o n t e c h n i q u e . S t a t i s t i c a l m o d e l . PRVCA 25 1546. NUCLEAR REACTIONS aSMg,ZTAl,5OTi,52Cr,SSFe,64Ni(a°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d o r ( f r a g m e n t 0,E) v s m a s s , a v e r a g e 7-multiplicity,E(X-ray),I(X-ray); 48Ca(U°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a ( f r a g m e n t 0,E) v s m a s s , a v e r a g e 7 - m u l t i p l i c i t y ; d e d u c e d o r ( c a p t u r e ) , effective moment of i n e r t i a , c o a l e s c e n c e m o d e l p a r a m e t e r s . 234pu,235Am,ZSSFm,a5s104,ae°106, 2se108,a72110 d e d u c e d T l / 2 l i m i t s . NUPAB 388 334.

93

KEY

NUMBERS

A 236 U

R

81Sul0:

82Ar14:

82Go0~:

82Go08:

820w01:

82Sa08:

R 81Sul0:

ZaTNp 237pu

D R

~37Bk

R 82Ri02:

7gCe04: 82Ra04:

D 78Ka40: 78Ri07:

82De22: R

82Ar14:

82Ch21:

82De07: 82De38:

82Do09:

82Go02:

82Ha02: 82Ha03:

236

=

=

237

NUCLEAR REACTIONS a35,u36,U3eU,z39pu(n,7),E ~ 0.001-10 MeV; 238,24°Pu(n,7),E ~ [3.001-0.3 MeV; 233U(n,7),E ~, 0.002-1 MeV; measured (;(E). 234,z36,237,239U,239,24°,241pu deduced n e u t r o n binding energy,average level widths. Statistical,direct s e m i - d i r e c t models. YTHLD 3 97. RADIOACTIVITY Z33U,Z37Np,238,zag,z4°,eaIPu,241Am; measured ET,I7. ENNLA 26 526. NUCLEAR REACTIONS 235U((x,2n),E=25.2 MeV; measured 7(0,H,T). 237pu deduced fission isomer g, Nilsson configuration. PRLTA 48 982. NUCLEAR REACTIONS i16Sn,154Sm,197Au(4°Ar,pF),(4OAr,dF),(4°Ar,tF),(4°Ar,~F),E=333 MeV; measured (fragment)p-,(fragment)d-,(fragment)t-,(fragment)(~-coin,o'(fragment 0,0p,Ep), (;(fragment 0,0~,Ea); d e d u c e d reaction mechanism. Z37Bk,*~4Hg,*S6Er d e d u c e d e m i s s i o n barriers,level density parameters,tins(J). Evaporation,statistical m o d e l s . PRVCA 25 2430.

A 338 U

KEYW0RDS

NUCLEAR REACTIONS z35,z36,Z38u,Z39Pu(n,7),E ~ 0.001-10 MeV; z38,Z4°pu(n,7),E ~ 0.001-0.3 MeV; ZZZU(n,T),E ~ 0 . 0 0 2 - 1 MeV; m e a s u r e d a ( E ) . zz4,za~,z37,Z39U,Z39,z4°,Z~tPu deduced neutron binding energy,average level widths. Statistical,direct semi-direct m o d e l s . YTHLD 3 97. NUCLEAR REACTIONS a34U(e,F),E=5.5-25 MeV; m e a s u r e d f i s s i o n ( ; ( f r a g m e n t 0). z34,a36,e3SU deduced dominant f i s s i o n c h a n n e l K , m u l t i p o l a r i t y , E 2 f i s s i o n s t r e n g t h f u n c t i o n s , G Q R role. NUPAB 389 378. NUCLEAR REACTIONS z3a,ZZsU(d,np),E=20 MeV; m e a s u r e d l ( c e ) , c e ( f r a g m e n t ) ( t ) , z3~,a38U d e d u c e d shape isomer decay charaeteristics,K/L ratio,transition multipolarity,vibrational band characteristics. PRLTA 48 1160. NUCLEAR REACTIONS a35U(n,F),E=10-200 keV; m e a s u r e d ( ; ( t o t a l ) , ( ; ( f r a g m e n t 0) v s E; d e d u c e d target polarization d e p e n d e n c e . Z3~u d e d u c e d p a r t i a l K c o n s e r v a t i o n , d o m i n a n t J,rr f o r p-wave f i s s i o n . PZETA 35 176. NUCLEAR REACTIONS e3ZTh,Z34,Z36u(ZOepb,Z°sPb'7),E=5.3 M e V / n u c l e o n ; m e a s u r e d E(7),I(7)(0). Z3ZTh,Z3¢,ZZ~U d e d u c e d l e v e l s , g r o u n d b a n d E2 t r a n s i t i o n m a t r i x e l e m e n t . E n r i c h e d t a r g e t s . NUPAB 388 421. NUCLEAR REACTIONS Z3ZTh(p,F),E=140,250,500,1000 MeV; Z32Th(d,F),E=70,140,500,1000 MeV; e3ZTh(a,F),E=69.2,140,280,1000 MeV; m e a s u r e d ( f r a g m e n t ) ( f r a g m e n t ) ( 0 ) ; deduced dominating p r o c e s s e s , c o r r e s p o n d i n g r e g i o n s . 233,a34pa,~36U d e d u c e d f o r w a r d m o m e n t u m transfer during f i s s i o n . PYLBB 110 372.

A

237 U

AND

=

238

RADIOACTIVITY 238U(SE); measured T~/z,fragment kinetic energy. Cylindrical gridded ionization chamber. NUIMA 154 335. RADIOACTIVITY 23SU(SF); measured decay constant. AABCA fi0 303. RADIOACTIVITY Z38U(SF); measured decay constant. Etched track technique. NUIMA 197 417. NUCLEAR REACTIONS Z34U(e,F),E=5.5-25 MeV; measured fission G(fragment 0). 234,z36,Z3Su deduced dominant fission channel K,multipolarity,E2 fission strength functions,GOR role. NUPAB 389 378. NUCLEAR REACTIONS 232Th,ZsSU(n,n'7),E=0.8-2.5 MeV; measured v-yields; deduced (;(inelastic) vs E. a3aTh,238U deduced levels,J,ir,K,rotational,vibrational bands,band p a r a m e t e r s . Compound nucleus,direct interaction mode] analysis. PRVCA 26 841. NUCLEAR REACTIONS a38U(a,(~'F),E=I20 MeV; measured (;(fragment,9~,e),fission probabilities. Z3eU deduced fission decay mode in giant resonance region. NUPAB 373 509. NUCLEAR REACTIONS 235,a3SU(v,F),E=I2,50,20,30 MeV bremsstrahlung; measured fractional, i n d e p e n d e n t , c u m u l a t i v e fission chain yields for Br,Kr,Rb,Sr,Zr,Sn,Sb,i,Te,Xe,Cs,Ba,La isotopes; deduced f r a g m e n t charge d i s t r i b u t i o n , m o s t probable charge, a35,~SSu deduced width p a r a m e t e r , p o s t n e u t r o n mass vs excitation energy. PRVCA 26 1356. NUCLEAR REACTIONS 23SU(e,e'F),E=46.5,56.9,67.1 MeV; measured (;(E(e')),(fragment)(e')-eoin, (;(E,0(e'),fragment 0) vs excitation energy. ~38U deduced E2/E0 s t r e n g t h function. PRLTA 49 113. NUCLEAR REACTIONS zss,238U(d,np),E=20 MeV; measured I(ce),ee(fragment)(t). asn,a38U deduced shape isomer decay characteristics,K/L r a t i o , t r a n s i t i o n m u l t i p o l a r i t y , v i b r a t i o n a l band characteristics. PRLTA 48 1160. NUCLEAR REACTIONS Z3ZTh,a3eU(p,p),(p,p'),E=26 MeV; m e a s u r e d (;(0); d e d u c e d potential multipole m o m e n t s . Z32Th,Z3eU d e d u c e d fla,fl4. C o u p l e d - c h a n n e l s a n a l y s i s . PRVCA 25 189. NUCLEAR REACTIONS ZaZTh,Z38U(lZTI,lUTI'),E=4.1 M e V / n u c l e o n ; Z3ZTh,Z38U(14~Nd,14ZNd'),E=5.1 MeV/ n u c l e o n ; m e a s u r e d E T , I T , m u l t i p l e C o u l o m b e x c i t a t i o n , r e c o i l in f e r r o m a g n e t i c Gd,7(~zTI) - , 7(142Nd)-coin. 23ZTh,Z3Bu deduced high-spin yrast state g,high-j nucleon aligment. PRLTA 48 383.

94

KEY

NUMBERS

A a38 U

R 82Ha34 82Moll

82Ru03 82Th04

83Zu01

aS~pu

D 79Ce04 8lAg06

R 81Su10

82B102

239pu

D 79Ce04 82He02 R 81Sul0

82Ha34

D 79Ce04 81Zh06 R 81Sul0

Z4OAm

D 81Lu06

D 79Ce04: R 81Su10:

a4~Am

D R

79Ce04:

82Dm01:

D 82Al13: 83Ed01:

=

239

=

240

=

241

R A D I O A C T I V I T Y ZS3u,23~Np,a38,z39,a4°,a41pu,241Am; m e a s u r e d ET,I 7. ENNLA 26 526. NUCLEAR REACTIONS a3sa36ZSSU,239pu(n,7), E ~ 0.001-10 MeV; 238,24°Pu(n,7),E ~ 0.001-0.3 MeV; a3SU(n,v),E ~ 0 . 0 0 2 - 1 MeV; m e a s u r e d cr(E). ~34,236,~sv,ZSSU,e39,24°,Z41pu deduced neutron binding energy,average level widths. Statistical,direct semi-direct m o d e l s . YTHLD 3 97. R A D I O A C T I V I T Y a33U,Z37Np,Z3e,z39,24°,Z41pu,Z41Am; m e a s u r e d E7,I7. ENNLA 26 526. NUCLEAR REACTIONS 237Np,a38U,z49Cf(c~,F),E=28,36 MeV; m e a s u r e d f i s s i o n a ( f r a g m e n t ) vs m a s s . 241Am,24apu,aS3Fm d e d u c e d s y m m e t r i c , a s y m m e t r i c f i s s i o n b a r r i e r d i f f e r e n c e . YAFIA 35 1112.

A a4apu

continued

R A D I O A C T I V I T Y 233U,237Np,~Ss,239,24°,24tpu,e41Am; m e a s u r e d ET,I 7. ENNLA 26 526. RADIOACTIVITY Z4°Pu(SF),a4z,244Cm(SF); m e a s u r e d p r o m p t n e u t r o n average n u m b e r , d i s t r i b u t i o n . YTHLD 3 149. NUCLEAR REACTIONS a35,zs6,a3SU,a39pu(n,7),E ~ 0.001-10 MeV; zss,z4°pu(n,7),E ~ 0.001-0.3 MeV; aSSU(n,7),E ~ 0 . 0 0 2 - 1 MeV; m e a s u r e d (~(E). a34,236,e37,239U,Z39,z4°,a4~pu d e d u c e d neutron binding energy,average level widths. Statistical,direct semi-direct m o d e l s . YTHLD 3 97. R A D I O A C T I V I T Y aS4Cf(SF),Z4o,a4Zm,a44mAm(SF) [ f r o m ~SeU(e°sPb,X),E=8 MeV/nucleon3; m e a s u r e d fragment distribution. Gas j e t , f i s s i o n t r a c k c o u n t i n g t e c h n i q u e s . ZPAAD 303 115.

A a4~pu

238

NUCLEAR REACTIONS z35,23s,23UU,~39Pu(n,7),E ~ 0.001-10 MeV; a38,Z4°pu(n,7),E m 0.001-0.3 MeV; Z~3U(n,7),E ~ 0 . 0 0 2 - 1 MeV; m e a s u r e d a ( E ) . as*,a36,a37,a39U,a39,a*°,a41Pu d e d u c e d neutron binding energy,average level widths. Statistical,direct semi-direct m o d e l s . YTHLD 3 97. NUCLEAR REACTIONS ZaSu(n,7),E=6.67,20.9,36.8,66.1,80.7 eV; m e a s u r e d c a p t u r e y i e l d . ~3OU r e s o n a n c e s d e d u c e d Pn,F7. T o f , s e l f - i n d i c a t i o n measurements,open self-shielding,improved accuracy. Multi-level formalism. NSENA 80 263. RADIOACTIVITY Z33U,aS~Np,a38,aa,a~°,24*Pu,a4~Am; measured E7,I7. ENNLA 26 528. R A D I O A C T I V I T Y a39pu; m e a s u r e d E T , r e l a t i v e I7 f o l l o w i n g ~ - d e e a y ; deduced emission probabilities. I J A R A 33 23. NUCLEAR REACTIONS ~35,ass,Z38U,z39pu(n,7),E ~ 0.001-10 MeV; ~ss,~4°Pu(n,7),E ,~ 0.001-0.3 MeV; ~3SU(n,7),E ~ 0 . 0 0 2 - 1 MeV; m e a s u r e d a(E). a3~ a3oz37,a39u,a39,a40,Z,ipu d e d u c e d neutron binding energy,average level widths. Statistical,direct semi-direct m o d e l s . YTHLD 3 97. NUCLEAR REACTIONS a3aTh,233,a35,aSSU,a39,a4aPu(n,n),(n,n'),E=0.6-3.4 MeV; m e a s u r e d ~(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s , aaaTh,aas,a38U,z3~pu l e v e l s d e d u c e d f12,f14. NSENA 81 491.

A a4Opu

=

KEYWORDS

NUCLEAR REACTIONS ~ 3 Z T h , ~ 3 3 , a s s , a S O U , ~ 9 , a 4 a p u ( n , n ) , ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d (7(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . ~3aTh,Z3s,Z38U,zaSpu l e v e l s d e d u c e d flz,fl4. NSENA 81 491. NUCLEAR REACTIONS a3aTh,a3SU(~x,a'),E=100,172 MeV; m e a s u r e d a(0). ~3UTh,a38U d e d u c e d GQR, giant octupole,hexadeeapole,monopole r e s o n a n e e s , P , m o n o p o l e s t r e n g t h s p l i t t i n g . PRVCA 25 2939. NUCLEAR REACTIONS 2 3 S U ( 7 , 7 ) , ( 7 , 7 ' ) , E = 2 . 7 5 - 9 . 7 2 MeV; m e a s u r e d ET,I7,a(0),elastic scattering,nuclear r e s o n a n c e f l u o r e s c e n c e , aaSu d e d u c e d l e v e l s , 7 - b r a n c h i n g . NUPAB 382 79. NUCLEAR REACTIONS ~35,a3SU(7,F),E=12,15,20,30 MeV b r e ~ s s t r a h l u n g ; measured independent i s o m e r i c y i e l d r a t i o of taaI. aas,aSau d e d u c e d r m s (J) v s e x c i t a t i o n . A c t i v a t i o n t e c h n i q u e . S t a t i s t i c a l m o d e l . PRVCA 25 1546. NUCLEAR REACTIONS a 3 8 U ( 7 , 7 ) , E = 2 . 7 5 - 6 . 5 MeV; m e a s u r e d a(0),total a(absorption) v s E; I a ~ T a ( 7 , 7 ) , E = 3 - 6 . 7 5 MeV; 16SHo(7,7),E=3.5-6.75 MeV; m e a s u r e d t o t a l a ( a b s o r p t i o n ) v s E. ZSeU, *S~Ta,~5Ho d e d u c e d average 7-branching ratio,E1 transition strength distribution, n o n s t a t i s t i c a l d e v i a t i o n s f r o m GDR L o r e n t z i a n . N u c l e a r r e s o n a n c e f l u o r e s c e n c e . PYLBB 114 99. R A D I O A C T I V I T Y a33U,a37Np,a38,a39,a4°,a41Pu,~4*Am; m e a s u r e d E7,I7. ENNLA 26 526. R A D I O A C T I V I T Y a38pu; m e a s u r e d Tl/a. A l p h a s p e c t r o m e t r y , a 3 9 p u s t a n d a r d . RRALA 46 69.

A 239 U

AND

=

242

R A D I O A C T I V I T Y 242,244pu(SF); m e a s u r e d c o m p l e m e n t a r y f r a g m e n t kinetic energies; deduced energy,mass distributions,mass-energy c o r r e l a t i o n s . NUPAB 380 61. R A D I O A C T I V I T Y ZSZCf(SF),z4Zpu(SF); m e a s u r e d p r o m p t n e u t r o n m u l t i p l i c i t y a v e r a g e , v a r i a n c e distributions. ANEND 9 127.

95

KEY

NUMBERS

A Z4apu

R 82Dm01:

a4aAm

D 81Lu06: 82Wi05:

ZaaCm

D 79Ch41: 81Zh06:

D 82Ah04:

R 81Be54:

D 82Al13:

244Am

D 81Lu06:

244Cm

D 81Zh06: R 81An25:

e44Fm

D 82Bo21:

D 82Bo21:

R 82Ho07:

a49Bk

R 82Be12:

249Cf

D 82Ah04:

D 79Ch40: 8OLi20: 81He22:

81Li26: 81Mo25:

243

=

244

=

246

=

fragment

total

kinetic

energies,

249

NUCLEAR REACTIONS 248Cm(n,-?),E=thermal; m e a s u r e d E%I% 249Cm d e d u c e d levels,J,rr,Nilsson assignments,neutron b i n d i n g e n e r g y . PRVCA 25 2232. NUCLEAR REACTIONS 249Bk(a,a),(a,a'),E=17.06 MeV; m e a s u r e d ( r ( E a , 0 = 1 5 0 ° ) . 249Bk l e v e l s deduced B(E2),B(Ml),quadrupole moment,#. E n r i c h e d t a r g e t . PRVCA 25 1637. RADIOACTIVITY Z49Cf,Z43Am; m e a s u r e d E T , a b s o l u t e Iv,E(K X - r a y ) , a b s o l u t e I(K X - r a y ) following a-decay. Electromagnetic isotope separator,243Am-239Np source in equilibrium. NUIMA 193 9.

A 252Cf

=

R A D I O A C T I V I T Y 244 ~ 4 6 F m ( S F ) ; m e a s u r e d (fragment)(fragment)-coin. PYLBB 113 213.

A a4OCm

continued

R A D I O A C T I V I T Y 24a,244pu(SF); measured complementary fragment kinetic energies; deduced energy,mass distributions,mass-energy correlations. N U P A B 380 61. R A D I O A C T I V I T Y ea4Cf(SF),Z4°,e4zm,a44mAm(SF)Cfrom 23BU(2°aPb,X),E=8 MeV/nucleon3; measured fragment distribution. Gas jet,fission track counting techniques. Z P A A D 303 115. R A D I O A C T I V I T Y a4°Pu(SF),e42,a44Cm(SF); measured prompt neutron average number,distribution. Y T H L D 3 149. N U C L E A R REACTIONS 243Cm(n,X),E=0.4-66 eV; measured transmission. 244Cm deduced resonances, r,resonance parameters. Tof,Cm203 target. Single level Breit-Wigner analysis. A E N G A 51 330. RADIOACTIVITY 244,U4SFm(SF); measured fragment total k i n e t i c energies, (fragment)(fragment)-coin. P Y L B B 113 213.

A

246Fm

242

R A D I O A C T I V I T Y Z4°Cf,243Am; m e a s u r e d E%absolute 17,E(K X-ray),absolute I(K X-ray) following a-decay. Electromagnetic isotope separator,243Am-239Np source in equilibrium. N U I M A 193 9. N U C L E A R R E A C T I O N S Ua3Am(a,a'),E=17 MeV; measured G(Ea',0=lS0°),Coulomb excitation, a43Am levels deduced B(E2),B(E4),quadrupole m o m e n t . Enriched target. P R V C A 24 2723.

A a44pu

=

KEYWORDS

NUCLEAR REACTIONS 237Np,2aSU,249Cf(a,F),E=28,36 MeV; m e a s u r e d f i s s i o n a ( f r a g m e n t ) v s m a s s . 241Am,Za2Pu,2S3Fm d e d u c e d s y m m e t r i c , a s y m m e t r i c f i s s i o n b a r r i e r d i f f e r e n c e . YAFIA 35 1112. RADIOACTIVITY 254Cf(SF),24°,U4amfi44mAm(SF) [ f r o m 23Su(aOapb,X),E=8 M e V / n u c l e o n 3 ; m e a s u r e d fragment distribution. Gas j e t , f i s s i o n t r a c k c o u n t i n g t e c h n i q u e s . ZPAAD 303 115. RADIOACTIVITY 242Am [ f r o m 241Am(n,-y),E=30 k e V ] ; m e a s u r e d Efl,Ifl,I(ce),fl-endpoint e n e r g y . NSENA 81 396. R A D I O A C T I V I T Y 2aeCm(SF); m e a s u r e d a-decay T 1 / z , T i / u ( S F ). YTHLD 1 21. RADIOACTIVITY Z4°Pu(SF),Z~z,U4aCm(SF); m e a s u r e d p r o m p t n e u t r o n average n u m b e r , d i s t r i b u t i o n . YTHLD 3 149.

A

a43Am

AND

=

252

RADIOACTIVITY 252Cf(SF); m e a s u r e d p r o m p t n e u t r o n a v e r a g e n u m b e r , d i s t r i b u t i o n . G d - l o a d e d liquid scintillator. YTHLD 1 9. R A D I O A C T I V I T Y 252Cf(SF); measured a v e r a g e p r o m p t n e u t r o n n u m b e r following a-decay. Gd-loaded liquid scintillation d e t e c t o r . G a u s s i a n f i t . YTHLD 2 53. RADIOACTIVITY 2S2cf(SF); m e a s u r e d (fragment)(fragment) energy correlation,fragment velocity; deduced pre-,post-neutron emission fragment mass,energy,velocity,mean total k i n e t i c e n e r g y , p r o m p t n e u t r o n n u m b e r v s f r a g m e n t m a s s . S u r f a c e b a r r i e r d e t e c t o r s . NUIMA 196 125. RADIOACTIVITY 252Cf(SF); m e a s u r e d t e r n a r y f i s s i o n p r o m p t n e u t r o n a v e r a g e n u m b e r vs Ea; deduced fragment deformation a t s e i s s i o n . YTHLD 3 281. R A D I O A C T I V I T Y aSeCf(SF); m e a s u r e d prompt neutron spectrum. T o f . YTHLD 3 163.

96

KEY

NUMBERS

A eSacf

D 81Rill: 83Bl14: 82EdO1 82FeOa 82Fr13 82No01 82Ra10 82Sp04

D 83Ah01:

Z53Fm

R 83Dm01:

R A D I O A C T I V I T Y 257Fm [ f r o m I(ce),Ev,Iv; deduced hindrance 373

D 81LuO6:

D 81Te02 R 82Bo29

R 82Bo29:

deduced

T~/2

D 82Wi08:

2~9No

D 82Wi08:

=

256

l i m i t s . NUPAB 388 334.

R A D I O A C T I V I T Y 257Fm [ f r o m I(ce),Ev,Iv; deduced hindrance 373 4 3 4 .

=

257

n e u t r o n i r r a d i a t i o n of Z¢¢Cm i n HFIR r e a c t o r ] ; m e a s u r e d Ea,Ia, f a c t o r s , aSSCf d e d u c e d levels,v-multipolarity,Jjr. NUPAB

=

258

NUCLEAR REACTIONS 26Mg,27A1,SOTi,SaCr,SaFe,64Ni(2°aPb,X),E=5.2-8 M e V / n u c l e o n ; measured g(fragment 0,E) v s m a s s , a v e r a g e 7-multiplicity,E(X-ray),I(X-ray); 4BCa(~QsPb,X),E=5.2-8 MeV/nucleon; measured a(fragment 0,E) v s m a s s , a v e r a g e v - m u l t i p l i c i t y ; deduced g(eapture), effective moment of inertia,coalescence model parameters. 234pu,a35Am,256Fm,25s104,260106, 266108,272110 d e d u c e d T I / 2 l i m i t s . N U P A B 388 3 3 4 .

A a59Md

~54

=

R A D I O A C T I V I T Y aSSFm(SF); m e a s u r e d p r o m p t n e u t r o n m u l t i p l i c i t y distribution parameters. Neutron multiplicity 3He-filled counter d e t e c t o r . NUIMA 190 119. NUCLEAR REACTIONS a S M g , 2 7 A l , S ° T i , S 2 C r , S a F e , 6 4 N i ( a ° s P b , X ) , E = 5 . 2 - 8 M e V / n u c l e o n ; measured a(fragment 0,E) v s m a s s , a v e r a g e v-multiplieity,E(X-ray),I(X-ray); ~SCa(Z°sPb,X),E=5.2-8 MeV/nucleon; measured ~(fragment 0,E) v s m a s s , a v e r a g e v - m u l t i p l i c i t y ; deduced a(capture), effective moment of inertia,coalescence model parameters. 234Pu,aSSAm,256Fm,25s104,zs°106,

A 25810 4

353

R A D I O A C T I V I T Y 254Cf(SF),24°,242m,a44mAm(SF) [ f r o m 238U(2°sPb,X),E=8 M e V / n u c l e o n 3 ; m e a s u r e d fragment distribution. Gas jet,fission track counting techniques. Z P A A D 303 115.

A

D 82AhOl

=

434.

2~6108,eTattO

257FIy1

continued

NUCLEAR REACTIONS aaVNp,Z38U,e49Cf(a,F),E=28,36 MeV; m e a s u r e d f i s s i o n c o ( f r a g m e n t ) v s m a s s . 241Am,242pu,aSSFm d e d u c e d s y m m e t r i c , a s y m m e t r i c f i s s i o n b a r r i e r d i f f e r e n c e . YAFIA 35 1112.

A 256Fm

252

n e u t r o n i r r a d i a t i o n of 244Cm i n HFIR reactorS; m e a s u r e d Ea,Ia, f a c t o r s . 253Cf d e d u c e d levels,v-multipolarity,J,rr. NUPAB

A

Z54Cf

=

KEYWORDS

R A D I O A C T I V I T Y a52Cf(SF); m e a s u r e d n ( f r a g m e n t ) - c o i n ; deduced average neutron number vs fragment m a s s . H P A C A 54 317. R A D I O A C T I V I T Y a52Cf(SF); m e a s u r e d a ( E n ) ; d e d u c e d m u l t i p l e s c a t t e r i n g e f f e c t s . Tof. NUIMA 198 455. R A D I O A C T I V I T Y 25aCf(SF),a42pu(SF); m e a s u r e d p r o m p t n e u t r o n m u l t i p l i c i t y average,variance distributions. ANEND 9 127. R A D I O A C T I V I T Y Z52Cf(SF); m e a s u r e d Ea,la. High resolution,CR-39 plastic track detector. NUIMA 197 517. R A D I O A C T I V I T Y 252Cf(SF); m e a s u r e d G(En). Tof,NE-213 scintillator. NUlMA 198 311. R A D I O A C T I V I T Y 252Cf(SF); m e a s u r e d p,d,t,a-emission,fragment energies; deduced fragment masses,total excitation e n e r g i e s . N U P A B 375 1B7. R A D I O A C T I V I T Y aSaCf(SF); m e a s u r e d f r a c t i o n a l c u m u l a t i v e y i e l d s of laaXe,139Cs. RAACA 30 15. R A D I O A C T I V I T Y 25aCf(SF); m e a s u r e d p r o m p t n e u t r o n n u m b e r . L i q u i d s c i n t i l l a t o r d e t e c t o r , h i g h p r e c i s i o n . NSENA 80 603.

A

253Cf

AND

=

359

R A D I O A C T I V I T Y 259No(EC),(a) [ f r o m 248Cm('eO,3na)2; m e a s u r e d a - d e c a y %/2- ZSaMd(SF) aSSNo(EC-deeay)]; measured Tl/z,(fragment)(fragment)-coin; deduced SF-deeay upper fragment mass,total kinetic energy distributions. P R V C A 26 1531. R A D I O A C T I V I T Y eSONo(EC),(a) [ f r o m aaSCm(lSO,3na)3; m e a s u r e d a - d e c a y %/2. 259Md(SF) aSSNo(EC-decay)]; measured Tl/e,(fragment)(fragment)-coin; deduced SF-decay upper fragment mass,total kinetic energy distributions. P R V C A 26 1531.

97

[from limit, [from limit,

KEY

NUMBERS

A

260106

R 82Bo29:

R 82Bo29:

R 8~Bogg:

~60

= ~66

NUCLEAR REACTIONS 26Mg,27A1,5°Ti,52Cr,SSFe,S4Ni(2°ePb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d ~ r ( f r a g m e n t O,E) v s m a s s , a v e r a g e - / - m u l t i p l i c i t y , E ( X - r a y ) , I ( X - r a y ) ; 48Ca(a°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a ( f r a g m e n t 0,E) v s m a s s , a v e r a g e - / - m u l t i p l i c i t y ; d e d u c e d a ( c a p t u r e ) , e f f e c t i v e m o m e n t of i n e r t i a , c o a l e s c e n c e m o d e l p a r a m e t e r s . 234Pu,235Am,25°Fm,258104,26°106, 2°6108,27~110 d e d u c e d Tl/2 l i m i t s . NUPAB 388 334.

A 27all 0

=

KEYWORDS

NUCLEAR REACTIONS 2SMg,27Al,~OTi,52Cr,SaFe,64Ni(2°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a(fragment 0,E) v s m a s s , a v e r a g e " y - m u l t i p l i c i t y , E ( X - r a y ) , l ( X - r a y ) ; 48Ca(2°sPb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a ( f r a g m e n t 0,E) v s m a s s , a v e r a g e 7 - m u l t i p l i c i t y ; d e d u c e d a ( c a p t u r e ) , e f f e c t i v e m o m e n t of i n e r t i a , c o a l e s c e n c e m o d e l p a r a m e t e r s , a34pu,2aSAm,2~SFm,25a104,a°6106, 266108,272110 d e d u c e d T1/2 l i m i t s . NUPAB 388 334.

A 26610 8

AND

=

272

NUCLEAR REACTIONS 26Mg,2VAl,~°Ti,SZCr,SSFe,S4Ni(2°spb,X),E=5.2-8 M e V / n u c l e o n ; m e a s u r e d a(fragment e,E) v s m a s s , a v e r a g e - / - m u l t i p l i c i t y , E ( X - r a y ) , I ( X - r a y ) ; 4SCa(a°aPb,X),E=5.a-8 M e V / n u e l e o n ; m e a s u r e d o r ( f r a g m e n t e,E) v s m a s s , a v e r a g e - / - m u l t i p l i c i t y ; d e d u c e d a ( c a p t u r e ) , e f f e c t i v e m o m e n t of i n e r t i a , c o a l e s c e n c e m o d e l p a r a m e t e r s . 234pu,~35Am,2~SFm,258104,2s°106, 26si08,272110 d e d u c e d TI/a l i m i t s . NUPAB 388 334.

98

REACTION

INDEX

(~,~) ~ 3 N a ( 7 , 7 ) , E = 7 - 1 4 , 1 6 - 3 1 MeV; m e a s u r e d ct(E) f o r A l ( T , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d o'(0). F e ( T , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d ~r(e). ~TFe(7,7),E=I4.4 k e V ; m e a s u r e d Mossbauer spectra. SaNi(7,T),E < 10 MeV; m e a s u r e d a(O). C u ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d a(8). Z n ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d a(O). M o ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d a(O). A g ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d or(0). S n ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d a(O). ~S~Ho(7,7),E=3.5-6.75 MeV; m e a s u r e d total ~e~Er(7,3,)~E=80.56 k e V ; m e a s u r e d Mossbauer spectra ~S*Ta(7,7),E=6.2 MeV; m e a s u r e d Mossbauer spectra.

821s01 8lGhOl 81Gh01 81Ve16 81Ac02 81GhOl 8tGh0[ 81Gh01 81Gh01 81Gh01 82ZuOl 81He31 81Zi02

~ a i T a ( 7 , 7 ) , E = 3 - 5 MeV; m e a s u r e d cr(0=90°,E). * S t T a ( 7 , T ) , E = 3 - 6 . 7 5 MeV; m e a s u r e d total W(7,3'),E=0.145 MeV; m e a s u r e d a(O). W ( 7 , 7 ) , E = 3 4 4 .... k e V ; m e a s u r e d a({9). *~TAu(7,T),E=77.3 keV; m e a s u r e d Mossbauer spectra. P b ( 7 , 7 ) , E = 0 . 1 4 5 MeV; m e a s u r e d a(O). ~ ° s P b ( 7 , ~ ) , E = 9 . 5 - 1 Z MeV; m e a s u r e d a(O,E). ~oePb(T,7),E < 10 MeV; m e a s u r e d a(O). Z ° s P b ( T , 7 ) , E = 9 . 5 - 1 2 MeV; m e a s u r e d a(e,E). Z ° a p b ( p o l a r i z e d 7 , 7 ) , E = 1 0 MeV b r e m . ; m e a s u r e d ET, a ~ S u ( T , T ) , E = 3 - 5 MeV; m e a s u r e d ff(e=90°,E). 2 3 8 U ( 7 , 7 ) , E = 2 . 7 5 - 9 . 7 2 MeV; m e a s u r e d ET,IT,a(O), Z3SU(T,7),E=2.75-6.5 MeV; m e a s u r e d ~(O),total

82Gall 82ZuOl 8tGh01 81Ta27 82Ts03 81Gh01 82St03 81Ac02 82St03 8~Wi06 82Gall

82Ru03 82Zu0!

(~,~') ~ 3 N a ( 7 , 7 ' ) , E = 7 - 1 4 , 1 6 - 3 1 MeV; m e a s u r e d a(E) for ~ ° C a ( 7 , 7 ' ) , E = 8 . 5 .... MeV b r e m . ; m e a s u r e d ET. ~°Zr(7,7'),E=8496 keV; measured E7,I7,77(0),~. *~*Cd(7,7'),E = r e s o n a n c e ; m e a s u r e d ET,IT,a(E). ~SSn(7,3,'),E=6325,6988 keV; measured E~,I~/,77(8),

821s01 82Mo05 82Be18 82Kr06 B2BelB

n S S n ( 7 , 7 ' ) , E = 6 . 9 8 8 MeV; m e a s u r e d E'y,I3,. l S ° S n ( 7 , 7 ' ) , E = 6 7 3 0 keV; m e a s u r e d ET,17,77(O),a. ~zsI(7,7'),E=27.8 keV; m e a s u r e d Mossbauer spectra. e S S U ( 7 , 7 ' ) , E = 2 . 7 5 - 9 . 7 2 MeV; m e a s u r e d ET,IT,a(e),

82Be35 82Be18 81De35 82Ru03

(7,ee + ) Fe(7,e*e-),E=2.615,... MeV; m e a s u r e d absolute F e ( 7 , e * e - ) , E = l . I 1 9 MeV; m e a s u r e d absolute C u ( 7 , e + e - ) , E = 2 . 6 1 5 .... MeV; m e a s u r e d absolute C u ( 7 , e * e - ) , E = l . l l 9 MeV; m e a s u r e d absolute S n ( 7 , e + e - ) , E = 2 . 6 1 5 .... MeV; m e a s u r e d absolute

82Av04 82Kh03 82Av04 82Kh03 83Av04

S n ( 7 , e * e - ) , E = l . l l 9 MeV; m e a s u r e d absolute P b ( T , e + e - ) , E = 2 . 6 1 5 .... MeV; m e a s u r e d absolute P b ( 7 , e * e - ) , E = l . l l 9 MeV; m e a s u r e d absolute U ( 7 , e + e - ) , E = 2 . 6 1 5 .... MeV; m e a s u r e d absolute U ( 7 , e + e - ) , E = l . l l 9 MeV; m e a s u r e d absolute

82Kh03 82Av04 8EKh03 82Av04 82Kh03

(~,=-) ~ L i ( 7 , ~ - ) , E = 4 0 0 MeV b r e m . ; m e a s u r e d o'(O,E(zr)). ~ ° B ( 7 , w - ) , E = 1 7 A 9 , 4 2 MeV; m e a s u r e d ~(O). ~ 2 C ( 7 , ~ r - ) , E = 2 0 0 - 3 9 0 MeV b r e m . ; m e a s u r e d cr(O,E(~r)) ~ Z C ( 7 , ~ - ) , E = 4 0 0 MeV b r e m . ; m e a s u r e d a(O,E(~r)).

82To10 82Ro04 82Ar06 82To10

13C(7,Tr-),E=lT,29,42 MeV; m e a s u r e d cr(E(~),e=90°). a4Mg(7,Tr-),E=400 MeV b r e m . ; m e a s u r e d a(O,E(~r)). Z S S i ( T J r - ) , E = 4 0 0 MeV b r e m . ; m e a s u r e d o(8,E(~r)). 4°Ca(7,Tr-),E=400 MeV b r e m . ; m e a s u r e d a(e,E(Ir)).

82Le06 82To10 82To10 82To10

(7,7r °) tH(polarized

7 , ~ r ° ) , E = 3 0 0 - 4 2 0 MeV; m e a s u r e d

82Be24

4 H e ( 7 , T r ° ) , E = l . 5 - 4 . 5 GeV h r e m . ;

measured,

~(O) '¢s

82A109

12C(7,~r+),E=400 MeV b r e m . ; m e a s u r e d a(0,E(Tr)). 24Mg(7,Tr+),E=400 MeV b r e m . ; m e a s u r e d a(O,E(Tr)). aSSi(7,~r+),E=400 MeV b r e m . ; m e a s u r e d a(0,E(lr)). 4 0 C a ( T J r + ) , E = 4 0 0 MeV b r e m . ; m e a s u r e d cr(0,E(~)).

82To10 82To10 82To10 82Tot0

52Cr('),,nT),E=10-32 MeV b r e m . ; m e a s u r e d ET,IT,cr(0), S ° N i ( 7 , n ) , E = 1 4 - 2 4 MeV b r e m . ; m e a s u r e d or(O), 74Se(T,n),E=14.5 MeV; m e a s u r e d S S S r ( T , n ) , E = I 4 . 5 MeV; m e a s u r e d 9 ° Z r ( 7 , n ) , E = i 4 . 5 MeV; m e a s u r e d SaMo(7,n),E=14.5 MeV; m e a s u r e d 1 S e D y ( 7 , n ) , E = 2 3 - 2 5 MeV b r e m . ; m e a s u r e d production l s s y b ( T , n ) , E = 2 3 - 2 5 MeV b r e r n . ; m e a s u r e d production z ° e p b ( 7 , n ) , E = 9 . 9 - 1 1 . 2 MeV; m e a s u r e d ~(En,O).

81Isl0 82Bo09 B2Fa08 82Fa08 82Fa08 82Fa08 81Le25 81Le25

(7,7r ÷) 6Li(7,~r+),E=400 MeV b r e m . ; m e a s u r e d a(O,E(~r)). 9 B e ( T j r + ) , E = 1 7 5 , 1 8 7 , 2 0 0 MeV; m e a s u r e d a(0=90°). l°B(7,~r+),E=17,19,42 MeV; m e a s u r e d or(0). *aC(Tjr+),E=20[}-390 Me¥ b r e m . ; m e a s u r e d a(O,E(Tr))

82To10 82Te01 82Ro04 82Ar06

(7,n) ~ H ( p o l a r i z e d 7 , n ) , E = l S . 8 MeV; m e a s u r e d cr(0) 4He(7,n),E=threshold-45 MeV; m e a s u r e d a(E). H B ( 7 , n ) , E = l S - 3 1 MeV b r e m . ; m e a s u r e d yields. l ~ N ( 7 , n ) , E = I 0 . 8 - 3 8 MeV; m e a s u r e d a(E),total ~ S O ( 7 , n ) , E = 6 0 - 1 6 0 MeV; m e a s u r e d a(ET,0n). ld~O(7,n),E=60--160 MeV; m e a s u r e d ct(0). 2 3 N a ( h , , n ) , E = 7 - 1 4 , i 6 - 3 t MeV; m e a s u r e d a(E) for ~ 4 C a ( 7 , n ) , E = l l - 2 6 MeV b r e m . ; m e a s u r e d cr(total) 45Sc(7,n),E=165,... MeV; m e a s u r e d or(E) r a t i o .

vs

82De21 81Ar23 81Br28 82Ju03 82Go09 82Se02 B21s01 81Ha50 81No12

82Be04

(7,P) I H ( 7 , p ) , E = 0 . 6 5 - 1 . 4 GeV; m e a s u r e d proton Z H ( 7 , p ) , E = 6 5 0 - 1 0 0 0 MeV b r e m . ; m e a s u r e d proton 2 H ( 7 , p ) , E = I 8 0 - 6 0 0 MeV; m e a s u r e d a(O) v s E. 2 H ( p o l a r i z e d 7 , p ) , E = 8 0 - 6 0 0 MeV; m e a s u r e d a(0), 2 H ( p o l a r i z e d 7 , p ) , E = 8 0 - 6 0 0 MeV; m e a s u r e d asymmetry 2 H ( 7 , p ) , E = 0 . 3 - 0 . 7 GeV b r e m . ; m e a s u r e d pn-coin, 3 H e ( 7 , p ) , E = 2 0 0 - 4 5 0 MeV; m e a s u r e d cr(0,E),pd-coin,

82Br06 12C(polarized 7,p),E ~ 0 . 7 5 - 2 GeV; m e a s u r e d proton 81Br29 ISO(7,p),E=24,32 M e V brem.; m e a s u r e d o(Ep),ff(Ed), 82Ba04 2 3 N a ( 7 , p ) , E = 7 - 1 4 , 1 6 - 3 1 MeV; m e a s u r e d o'(E) f o r 82Go07 4 5 S c ( 7 , p ) , E = 1 5 . 6 - 2 5 MeV b r e m . ; m e a s u r e d absolute 82Go12 5aCr(-/,pT),E=~O-32 MeV hrem.; measured ET,IT,•(O), 82Is03 S°Ni(7,p),E=14-24 MeV brem.; measured or(O), 81Ga34 Cu(T,p),E=150,300 MeV brem.; measured cr(Ep,8). continued

99

81Av05 82Ba03 83Is01 82Ry01 811slO 82B009 82Sc12

REACTION

continued

(7,P) B e ( 7 , p ) , E = 3 6 0 - 6 0 0 MeV; m e a s u r e d proton momentum S B e ( p o l a r i z e d 7,p),E=0.69,... GeV; m e a s u r e d l l B ( 7 , p ) , E = 1 5 - 3 1 MeV b r e m . ; m e a s u r e d a ( E p ) v s 0. C ( 7 , p ) , E = 3 6 0 - 6 0 0 MeV; m e a s u r e d proton momentum

INDEX

82Ba32 82Av06 81Br28 82Ba32

S 4 C u ( p o l a r i z e d */,p),E ~ 0 . 7 5 - 2 GeV; m e a s u r e d e S Y ( % p ) , E = 1 4 - 2 4 MeV b r e m . ; m e a s u r e d or(E) a b s o l u t e 2 ° T P b ( p o l a r i z e d 7,p),E ~ 0 . 7 5 - 2 GeV; m e a s u r e d

8lAy05 81Va24 81Av05

(y,2n) 1 5 N ( T , 2 n ) , E = 1 0 . 8 - 3 8 MeV; m e a s u r e d

a(E),total

8eauo3 (7,np)

laC(y,np),E not

given;

measured

a(O) v s

total

81Kh08

1 2 C ( ' y , n p ) , E = 3 4 - 1 5 0 MeV b r e m . ;

measured

(7(On),~(Op)

82Do08

(7,d) aHe(%d),E=150-350

MeV b r e m . ;

measured

a(O) v s E.

82Br12

1SO(%d),E=24,32 MeV b r e m . ;

measured

a(Ep),a(Ed),

82Be03

inclusive

82Ve06

(~,t) tSO(%t),E=24,32

MeV b r e m . ;

measured

a(Ep),a(Ed),

82Ba03

(Y,CO 1 8 0 ( 7 , a ) , E = 2 4 , 3 2 MeV b r e m . ;

measured

a(Ep),a(Ed),

82Ba03

(y,3cO iaC(%3a),E=42

MeV b r e m . ;

measured

cr.

81Me38

(~,4~)

leO(7,4a),E=42 MeV b r e m . ;

measured

a.

81Ma38

(~,xn) l S O ( % x n ) , E = e 4 - 1 3 3 MeV; m e a s u r e d integrated a for 3 ° S i ( 7 , x n ) , E ,~ 1 0 - 2 8 MeV b r e m . ; m e a s u r e d neutron

82Ca05 820d01

Zr('y,xn),g=8-134

MeV; m e a s u r e d

a(E)

for

(~,F) e a a T h ( % F ) , E = 5 . 4 - 6 . 4 MeV; m e a s u r e d a(total,E), a a a T h ( ' y , F ) , E = 4 . 9 5 - 6 . 7 6 MeV b r e m . ; m e a s u r e d fission 2 a S T h ( p o l a r i z e d 3,,F),E=IO,12 MeV b r e m . ; m e a s u r e d ZaSTh(7,F),E=IO,12 MeV b r e m . ; m e a s u r e d fission 235U(%F),E=12,... MeV b r e m . ; m e a s u r e d fractional,

8tBe55 82Kn03 82Rail 82Rail 82De38

2a~U(%F),E=12 .... 2aSU(3,,F),E=not 2aSU(%F),E=12,... 2aeU(3',F),E=12 ....

MeV b r e m . ; m e a s u r e d independent given; measured a(fragment 0). MeV b r e m . ; m e a s u r e d fractional, MeV b r e m . ; m e a s u r e d independent

82Th04 81Ka44 82De38 82Th04

(~,x) O ( % X ) , E = 5 g . 5 4 .... k e Y ; m e a s u r e d ~(total). P ( % X ) , E = 5 9 . 5 4 .... k e Y ; m e a s u r e d a(total). a4Mg(3,,X),E=4.5 GeV b r e m . ; m e a s u r e d 2e,24Na,tSF, 2SMg(3,,X),E=4.5 GeV b r e r n . ; m e a s u r e d ~a,24Na,laP,

aOMg(%X),E=4.5 GeV b r e r n . ; m e a s u r e d 2~,S4Na,leF, Cl(3',X),E=59.54 .... k e V ; m e a s u r e d a(total). 76Se(3',X),E=9-20 MeV; m e a s u r e d t o t a l a(E). BSSe(%X),E=9-20 MeV; m e a s u r e d t o t a l g(E).

82Sm03 82Sm03 82Ar07 82Ar07

82Ar07 82Sm03 78Gu~7 78Gu~7

(e,y) lgTAu(e,3,),E=l.5 MeV; m e a s u r e d

E')',ls',E(X-ray),

81HaS1

e,e) ln(e,e),E n o t g i v e n ; m e a s u r e d a(E). a H e ( e , e ) , E = 2 0 0 - 7 0 0 MeV; m e a s u r e d ~(0=155D). JSC(e,e),E=lO0-300 MeV; measured a b s o l u t e a(O). t 3 C ( e , e ) , E = 8 0 - 3 3 8 MeV; m e a s u r e d a{E,O). 4 0 A r ( e , e ) , E = l 1 6 , 2 4 9 MeV; m e a s u r e d or(8).

82Ro12 ° S C u ( e , e ) , E = 4 0 - 9 0 MeV; m e a s u r e d cr,magnetie form 82Ca15 S ~ C u ( e , e ) , E = 4 0 - 9 0 MeV; m e a s u r e d a,magnetic form 82Re12 SVSr(e,e),E=175-3~5,500 MeV; m e a s u r e d a(e,E). 82Hi07 S a N b ( e , e ) , E = 1 7 5 - 3 2 5 , 5 0 0 MeV; m e a s u r e d a(O,E). 820t01 Z°STl(e,e),E=502 MeV; m e a s u r e d a(O),ratio vs continued

100

82Se06 82Se06 82P104 82P104 82Ca14

INDEX

REACTION

(e,e)

continued

"Tl(e,e),E=175-325,500 MeV; m e a s u r e d o(8,E). 5'V(e,e),E=175-325,500 MeV; m e a s u r e d o(8,E). 58Co(e,e),E=175-325,500 MeV; m e a s u r e d o(8,E)

82P I 0 4 82P 104 82P104

'OsPb(e,e),~=502 MeV; m e a s u r e d o ( 8 ) , r a t i o v s 209~i(e,e),~=175-325,500 MeV; m e a s u r e d u(8,E).

'~i(e,e'),E=80-300 MeV; m e a s u r e d o(E,E(e'),B). 7 ~ i ( e , e ' ) , ~ = 4 0 - 7 MeV; 4 measured o(B),transverse 1BO(e,e'),~=112 MeV; m e a s u r e d o(8(er),E(e')), "0(e,e'),E=90-370 MeV; m e a s u r e d o ( E ( e t ) ) , f o r m 4 0 ~ a ( e , e ' ) , ~ = 3 1 - 6MeV; 5 m e a s u r e d o(B),o(E(e')), * ' c a ( e , e r ) , ~ = 3 0 - 5 8 MeV; m e a s u r e d o(E(er)),o(8). s0~i(e,e'),~=30-58 MeV; m e a s u r e d u(E(eC)),o(8). 5 2 Cr(e,e'),E=30-58 MeV; m e a s u r e d o(E(e')),o(B). 5 4 ~ e ( e , e ' ) , ~ = 3 0 - 5MeV; 8 m e a s u r e d o(E(er)),o(8).

82Be 1 1 82Bu09 82Vo05 82No04 82Bu05 82EuOl 82EuOi 82Eu01 82Eu01

"Sr(e,e8),E=36,42,50 MeV; m e a s u r e d "Y(e,er),E n o t g i v e n ; m e a s u r e d u(0) v s m o m e n t u m Q0Zr(e,e'),E=37.2,60.6MeV; m e a s u r e d o(8=180°). 'OZr(e,e'),E n o t g i v e n ; m e a s u r e d 018) v s m o m e n t u m '48Sm(e,e'),~=150-215 MeV; m e a s u r e d o(O,E(e)). 1 5 ' S m ( e , e ' ) , ~ = 1 5 ~ - 2 1 5MeV; m e a s u r e d v(B,E(e)). 208Pb(e,e'),E=50-335 MeV; m e a s u r e d o(E(e8),f3). 2 0 8 ~ b ( e , e ' ) , ~ = 4 0 . 5 ,MeV; ... m e a s u r e d o(8=180°). 208Pb(e,e'),E n o t g i v e n ; m e a s u r e d v(6) v s m o m e n t u m

82Va05 82Sc08 82Fa 11 82Sc08 82Do06 82Do06 82He03 82Hi 1 0 82Pa05

'H(e,.rr-f,~=200MeV; m e a s u r e d o ( e , ~ ( n ) ) .

82Se 1 1

3He(e,.rri),E=200 MeV; m e a s u r e d u(@,E(n.)).

82Sell

82Zu03

1 2 C ( e , e ' r r ' ) , ~ =MeV; ~ ~ ~ measured ~ ( E ( T F ) , ~ )

82G006 8 2JaO6 80Go21

' ' c ( e , e r p ) , ~ = 5 0 0 MeV; m e a s u r e d ' 8 0 ( e , e ' p ) , ~ = 5 0 0 MeV; m e a s u r e d 0(e,erp),E=112 MeV; m e a s u r e d v(6(e'),E(e')),

232Th(e,F),E=100-275 MeV; m e a s u r e d o(fission,E). 232Th(e,F),E=5.5-7 MeV; m e a s u r e d fragment 8). 233U(e,F),E=100-275 MeV; m e a s u r e d o(fission,E). 234U(e,F),E=5.5-25 MeV; m e a s u r e d f i s s i o n 235U(e,F),E=100-275 MeV; m e a s u r e d o ( f i s s i o n , E ) . 2 3 % ( e , ~ ) , ~ = 1 0 0 - 2 7 5MeV; m e a s u r e d o(fission,E). '3BU(e,F),E=100-275 MeV; m e a s u r e d o(fission,E).

8 1Vo 1 2 82Ar05 8 1Vo 1 2 82Ar14 8 1Vo12 8lVol2 8 1Vo 1 2

238~(e,F),E=100-:000 MeV; m e a s u r e d o , 238U(e,F),E=10-35 MeV; m e a s u r e d a b s o l u t e o . 2 3 7 ~ p ( e , ~ ) , ~ = 1 0 0 - 2MeV; 7 5 m e a s u r e d o(fission,E). 2 3 7 ~ p ( e , F ) , ~ = 1 0 0 MeV; - 1 ~ ~m ~easured a , 2 3 8 ~ u ( e , F ) , ~ = 1 0 0 - 2 7MeV; 5 m e a s u r e d o(fission,E). " 3 8 ~ u ( e , ~ ) , ~ = 1 0 0 - 1 0MeV; 0 ~ measured a , " 3 ~ m ( e , ~ ) , ~ = 1 0 0 - 1 0MeV; 0~ measured a ,

,'3sU(e,e'F),E=10-34 MeV; m e a s u r e d f i s s i o n o(E).

8 1 Ma4 1

'38U(e,e'F),E=46.5,...

' 2 ~ ( e , e ' . r r - ) , ~ = 2 0MeV; 0 m e a s u r e d o(E(.rr),@).

' ' ~ ( e , e ' . r r + ) , ~ = 1 5 8 . 5 - 1 6 5MeV; m e a s u r e d

o(B(.rr),E(.rr))

" ~ l ( e , p ) , ~ = 1 6 . 8 - 2 5 . 6 MeV; m e a s u r e d o(E,B).

45Sc(e,e'n),E=165,... MeV; m e a s u r e d u(E) r a t i o .

3He(e,e'p),E=643,806 MeV; m e a s u r e d 3He(e,e'p),E a t 310 MeV/c; m e a s u r e d 4He(e.e'p),E=974,1:86 MeV; m e a s u r e d a(@(e),Bp,Ep),

''

3H(e.t),~=77-147 MeV; m e a s u r e d o ( ~ t , e t )

!"Fe(e,X),E=ZO GeV; m e a s u r e d

fragment 8,E) f o r

MeV; m e a s u r e d o(E(eP)),

REACTION

INDEX

(e,e'X) a H e ( e , e ' X ) , E = 6 . 4 - 1 6 . 5 GeV; m e a s u r e d 4 H e ( e , e ' X ) , E = 6 . 4 - 1 6 . 5 GeV; m e a s u r e d

a(0,E(e')). a(0,E(e')).

82Ro16 82Ro16

100(e,e'X),E=112 MeV; m e a s u r e d

q(0(e'),E(e')),

82Vo05

E T.

82Fr08

(e+,F) aaSU(e+,F),E=10-35 MeV; m e a s u r e d

absolute

a.

82St05

(~-,v) 1e0(#-,T),E

at

rest;

measured

ET.

82Fr08

4OCa(/~-,T),E a t

rest;

measured

(~-,~) 12C(/~-,u),E a t

rest;

measured

capture

ratios.

81Ro15

t2C(polarized

/z-,u),E a t

rest;

measured

recoil

82Ro13

(~-,e) Sas(]~-,e-),E a t

rest;

measured

electron,positron

82Ba05

(]~-,e +) 32S(]~-,e+),E a t

rest;

measured

electron,positron

82Ba05

(~-,p) IH(~-,p),E

at

rest;

measured

muonic

X-rays.

821a01

(/z-,xn) 2°~Pb(~-,xn),E

at

rest; m e a s u r e d

BT,IT.

82Bu04

(K-,K-) IaC(K-,K-),E=442

MeV; m e a s u r e d

a(0).

82Ma16

a(O).

82Ma16

4 ° C a ( K - , K - ' ) , E = 4 4 2 MeV; measured a(O).

82Ma16

4 ° C a ( K - , K - ) , E = 4 4 2 MeV; m e a s u r e d

(K-,K-') I e C ( K - , K - ' ) , E = 4 4 2 MeV; m e a s u r e d

a(0).

82Ma16

(K+,K +) 12C(K+,K+),E=442

MeV; measured q(O).

4°Ca(K+,K+),F,=442

82Ma16

MeV; m e a s u r e d

o'(0).

82Ma16

4 ° C a ( K + , K + ' ) , E = 4 4 2 MeV; m e a s u r e d

a(0).

82Ma16

( K + , K +') ' a C ( K + , K + ' ) , E = 4 4 2 MeV; m e a s u r e d

a(0).

82Ma16 (~-,V)

IH(Tr-,T),E=27.4,39,3 MeV; m e a s u r e d

E7,17.

82Me03

14C(Tr-,7),E n o t

given;

measured

ET.

81Ba57

(~r-,Tr-) a H ( T r - , ~ - ) , g a t 0 . 9 8 - 1 . 7 6 , 2 . 4 5 GeV/c; m e a s u r e d S H ( ~ - , ~ ' - ) , E = 6 5 MeV; m e a s u r e d G(O). 4 H e ( T r - J r - ) , E = 5 1 MeV; m e a s u r e d (~(0).

c~(O)

7Li(Tr-,Tr-),E=143 MeV; m e a s u r e d (y(O),~(Ew'). 4 0 C a ( ~ - , v r - ) , E = 6 4 . 8 MeV; m e a s u r e d a(O).

81AbO6 82Ba16 82Ba16

82Gi01 82Da13

(~-,.-,) 4 H e ( z r - , ~ - ' ) , E = 1 2 0 , 2 2 0 MeV; m e a s u r e d a(0,E(~r')). 7Li(w-,Tr-'),E=143 MeV; m e a s u r e d a(O),t;(ETr). lZC(~r-,~r-'),E=80 MeV; m e a s u r e d cT(O),a(w').

82Ba19 82Gi01 82B109

lZC(Tr ,Tr-'),E=t00 .... MeV; m e a s u r e d cr(0,E(Tr)). 1Sc(~-,Yr-'),E=162 MeV; m e a s u r e d or(0). 4SCa(~r-,~r-'),E=80 MeV; m e a s u r e d (r(0),¢r(Tr').

102

82Mo01 82Se04 82B109

INDEX

REACTION

(71"-,71"0 ) I H ( r r - , r r ° ) , E = 2 7 . 4 , 3 9 . 3 MeV; m e a s u r e d E7,I7. 3He0r-,~r~),E=~00 MeV; m e a s u r e d a(O),a(O,E(rr%).

82Me03 8ZCo01

3He(rr-,n),E at

82Go04

rest;

measured

a(Ei,Ea)

vs r e l a t i v e

aHe(~r-,Tr°),E=285,428,525 MeV; m e a s u r e d 6*(0t,E). 4°Ca(Tr-,Tr°),E=164 MeV; m e a s u r e d ¢r(0,E0r°)).

82Ka02 82BaSO

(~-,p) S H e ( ~ r - , p ) , E = 5 0 - 3 0 0 MeV; m e a s u r e d 3He(~r~,p),E=400,475 MeV; m e a s u r e d ~ H e ( ~ r - , p ) , E = 5 0 - 3 0 0 MeV; m e a s u r e d ~ H e ( ~ r - , p ) , E = 4 0 0 , 4 7 5 MeV; m e a s u r e d

~(0,Ep). yields. ¢(0,Ep). yields.

12C(Tr-,p),E=400,475 MeV; m e a s u r e d yields. 2 7 A l ( ~ r - , p ) , E = 5 0 - 3 0 0 MeV; m e a s u r e d ~r(0,Ep). aVAl(~r-,p),E=400,475 MeV; m e a s u r e d yields. ¢°Ca(~r-,p),E a t r e s t ; m e a s u r e d energy spectra.

81Ka4l 81Ka43 81Ka41 81Ka43

81Ka43 81Ka41 81Ka43 82Ra15

7r-,Tr-n) C O r - , T r - n ) , E = 1 6 5 MeV; m e a s u r e d a(0~r,0n),cr(0~r,0p). ~aC(rr-,~r-n),E=150 MeV; m e a s u r e d ~rn-coin. ~ZC(~r , r r - n ) , E = 3 0 - 1 0 0 MeV; m e a s u r e d a(E). ~ 3 C ( w - , ~ - n ) , E = 1 5 0 MeY; m e a s u r e d ~rn-coin.

F e ( r r - , T r - n ) , E = 1 6 5 MeV; m e a s u r e d ~r(01r,0n),a(07r,0p). ~ 2 7 1 ( l r - j r - n ) , E = 6 0 - 3 5 0 MeV; m e a s u r e d production Bi(~r-,~r-n),E=165 MeV; m e a s u r e d a(0fr,0n),a(07r,0p).

82Pi04 81An20 82Bu20 B1An20

82Pi04 820h07 82Pi04

(rr-,rr-p) C O r - , ~ r - p ) , E = 2 4 5 MeV; m e a s u r e d F e ( ~ r - , ~ r - p ) , E = 2 4 5 MeV; m e a s u r e d

a(Ep,0p,0(~r)), tr(Ep,0p,0Or)),

82Pi03 82Pi03

1271(rr-,~ p ) , E = 6 0 - 3 5 0 MeV; m e a s u r e d production B i 0 T - , r r - p ) , E = 2 4 5 MeV; m e a s u r e d cr(Ep,0p,0(rr)),

820h07 82Pi03

Or-,en) SdMg(w-,2n),E a t r e s t ; m e a s u r e d V4Ge(rr-,2n),E a t r e s t ; m e a s u r e d a~Mo(~r-,2n),E a t r e s t ; m e a s u r e d

residuals residuals residuals

yield, yield, yield,

t14Cd('rr-,2n),E a t r e s t ; m e a s u r e d 14ZCe(rr-,2n),E a t r e s t ; m e a s u r e d 174ybOr-,2n),E at rest; measured

820r05

820r05 820r05

residuals residuals residuals

yield, yield, yield,

820r05 820r05 820r05

residuals yieid, residuals yield, residuals yield, residuals yield,

820r05 820r05

(w-,np) 3He(~r-,np),E SHe(~r-,np),E 26MgOr-,np),E 74GeOr-,np),E

at rest; measured at rest; measured at rest; measured at rest; measured

K X-ray(d)-,K a(E1,Es) v s residuals yield, residuals yield,

82Ba43 82Go04 820r05 820r05

97Mo(~r-,np),E n4Cd(rr-,np),E 14aCe(rr-,np),E 174ybOT-,np),E

at rest; measured at rest; measured at rest; measured at rest; measured

820r05

820r05

(~-,d) 3He(Tt-,d),E a t

rest;

measured

K X-ray(d)-,K

82Ba43

*OCa(~-,d),E a t

rest;

measured

energy

spectra.

82Ra15

(w-,2p) 'aLi(Tr-,Sp),E a t 7Li(rr-,Sp),E a t tZC(Tr ,Sp),E a t

rest; rest; rest;

measured measured measured

inclusive inclusive

cr(Ep), cr(Ep),

82Se08 82Se08 82Se09

59Co(~-,Sp),E at rest; m e a s u r e d 197Au(~-,2p),E at rest; m e a s u r e d

(~ :LSC(rr-,lr-d),E-160 .... MeV; m e a s u r e d

a(0(~r),Od),

82Se09 82Se09

,~-d)

82EI07

(=-,t) 4°Ca(~-,t),E

at

rest;

measured

energy

spectra.

82Ra15

(~-,pd) e~Li(Tr-,pd),E a t 7Li(w-,pd),E at 12C(rr-,pd),E a t

rest; rest; rest;

measured measured measured

inclusive inclusive

cr(Ep), a(Ep),

SgCo(~-,pd),E

8aSe08 82Se08 82Se09

iSVAu(~-,pd),E

103

at rest; measured at rest; measured

82Se09 82Se09

REACTION

INDEX

(~-,3He)

~°Ca(~v-,3He),E at rest; m e a s u r e d

energy

spectra.

82Ra15 (~-,~-t)

~Ue(~r-,~r-t),E=160 .... MeV; m e a s u r e d

G(O(~r),Od),

82E107

(~-,pt) eLi(~r-,pt),E a t r e s t ; m e a s u r e d 7Li(~r-,pt),E a t r e s t ; m e a s u r e d ~ZC(~-,pt),E a t r e s t ; m e a s u r e d

inclusive inclusive

G(Ep), a(Ep),

82Se08 82Se08 82Se09

59Co(~-,pt),E a t r e s t ; m e a s u r e d lSTAu(~-,pt),E at rest; measured

82Se09 82Se09

59Co(~-,2d),E a t r e s t ; m e a s u r e d l~TAu(~-,2d),E at rest; m e a s u r e d

82Se09 82Se09

(~-,2d) eLi(~r-,2d),E a t VLi(rr-,2d),E a t ZZC(~T-,2d),E a t

rest; measured rest; measured rest; measured

inclusive inclusive

~°Ca(~-,a),E at

rest;

energy

measured

G(Ep), a(Ep),

spectra.

82Se08 82Se08 82Se09

82Ra15 (x-,paHe)

12C(~r-,p3He),E at rest; m e a s u r e d SSCo(~r-,p3He),E at rest; m e a s u r e d

82Se09 82Se09

lSVAu(~-,pSHe),E a t

rest;

measured

82Se09

(~-,dt)

eLi(Tr-,dt),E at rest; m e a s u r e d 7Li(~r-,dt),E at rest; m e a s u r e d 12C(vr-,dt),E at rest; m e a s u r e d

inclusive a(Ep), inclusive a(Ep),

82Se08 82Se08 82Se09

5SCo(~-,dt),E a t r e s t ; m e a s u r e d lgVAu(x-,dt),E at rest; measured

82Se09 82Se09

(x-,pa) 82Se09 82Se09

12C(lr-,pa),E a t r e s t ; m e a s u r e d S°Co(w-,pa),E a t r e s t ; m e a s u r e d

lS~Au(~-,pa),E at

rest;

measured

82Se09

(~-,daHe) ~UC(Ir-,dSHe),E at rest; m e a s u r e d 5gCo(Tr-,d3He),E at rest; m e a s u r e d

82Se09 82Se09

19~Au(~-,d3He),E a t

rest;

measured

82Se09

(~-,2t)

eLi(~r-,2t),E at rest; m e a s u r e d ~Li(Tr-,2t),E at rest; m e a s u r e d 12C(Ir-,2t),E at rest; m e a s u r e d

inclusive a(Ep), inclusive a(Ep),

82Se08 82Se08 82Se09

SSCo(~-,2t),E a t r e s t ; m e a s u r e d tSTAu(~-,2t),E a t r e s t ; m e a s u r e d

82Se09 82Se09

(~-,d~) iZC(Tr-,da),E a t r e s t ; m e a s u r e d ~SCo(Tr-,d(x),E a t r e s t ; m e a s u r e d

82Se09 82Se09

197Au(~-,da),E at

rest;

measured

82Se09

(~-,t3He) 12C(~r-,t3He),E a t r e s t ; m e a s u r e d 59Co(w-,tSHe),E a t r e s t ; m e a s u r e d

82Se09

IgTAu(~-,tSHe),Eat rest; measured

825e09

lg~Au(~-,ta),E at

82Se09

82Se09

(~-,ta) tSC(w-,ta),E a t r e s t ; m e a s u r e d 5SCo(~r-,ta),E a t r e s t ; m e a s u r e d

82Se09 82Se09

104

rest;

measured

REACTION

INDEX

(~-,2a) *ZC(=-,2a),E a t r e s t ; m e a s u r e d SgCo(rr-,2a),E a t r e s t ; m e a s u r e d

82Se09

19VAu(w-,2a),E a t

rest;

measured

l°5Ho(~-,xn),E Ta0r-,xn),E ~ ia~Ta(~-,xn),E P b ( ~ r - , x n ) , E ,~

rest; measured 7n-coin. measured a(En),yields. rest; measured 7n-coin. measured a(En),yJelds.

82Le16

at at at at at

82Bu07 82Bu07 82Bu07 82Bu07 82Bu97

82Se09

82Se09

w-,xn) O; m e a s u r e d a(En),yields. N(~r-,xn),E ~ 0; m e a s u r e d a(En),yields. O 0 r - , x n ) , E ~ 0; m e a s u r e d q(En),yields. A l ( ~ - , x n ) , E ~ 0; m e a s u r e d a(En),yields. C u ( ~ r - , x n ) , E ~ O; m e a s u r e d ~r(En),yields.

82Ma22 82Ma22 82Ma22 82Ma22 82Ma22

C(~r-,xn),E ~

at O; at 0;

82Ma22 82Le16 82Ma22

(rr-,xnyp) *:~aBa(Tr-,xnyp),E ~:~SLa(~r-,xnyp),E ~'~°Ce0r-,xnyp),E *~Pr0r-,xnyp),E l~aNd0r-,xnyp),E :~SNd(vr-,xnyp),E

at at at at at at

rest; rest; rest; rest; rest; rest;

measured measured measured measured measured measured

E7,17. E7,I7. E7,I7. ET,IT. E7,17. E7,17.

82Bu07 82Bu07 82Bu07 82Bu07 82Bu07 82Bu07

144Nd(Tr-,xnyp),E 145Nd(Tr-,xnyp),E 14aNd(Tr-,xnyp),E *4BNd(Tr-,xnyp),E ~°Nd(w-,xnyp),E

rest; measured rest; measured rest; measured rest; measured rest; measured

E7,I7. E7,I7. E'y,IT. E7,t7. E7,I7.

(~-,pX) aLi(~r-,pX),E a t

rest;

measured

inclusive

a(Ep),

828e0B

7Li(~r-,pX),E a t r e s t ;

measured

inclusive

a(Ep),

82Se08

7Li(w-,dX),E a t r e s t ;

measured

inclusive

a(Ep),

82Se08

measured

inclusive

q(Ep),

82Se08

(~-,dX) st, i(~r-,dX),E a t

rest;

measured

inclusive

cr(Ep),

828e08

(.-,tx) %i(~r-,tX),E

at

rest;

measured

inclusive

a(l~p),

82Se08

7Li(Tr-,tX),E a t

rest;

(w+,~ - )

i S o ( ~ + , w - ) , E = 8 0 - 2 9 2 Me'g; m e a s u r e d a ( e ) v s E. iso(~r+,~r-),E=164 MeV; m e a s u r e d a(E(~r-)) a t 0=50 . t a O ( ~ r + j r - ) , E = 8 0 - 2 9 2 Me'Y; m e a s u r e d a ( O ) v s E.

zsSi(Tr*,Tr-),E=164 MeV; m e a s u r e d 4°Ca(lr+,Ir-),E=164 MeV; m e a s u r e d

82Gr02

82Mo12

tr(E(~r-)) a t 0 = 5 °. cr(E(Tr-)) a t 0=50 .

8~Mo1~ 82Mo12

82Gr02

Tr + -n 0

7Li(~r+,~r°),E=70 .... MeV; m e a s u r e d t~(0),a(E(~r°)). ~ZC(~r+,~r°),E=70 .... MeV; m e a s u r e d a(0),a(E(~r°)). laC(Tr+jrO),E=164 MeV; m e a s u r e d a(0).

82Do02 82Do02

lSN(~r+,~°),E=164 MeV; m e a s u r e d a(O). 40Ca(~r+,~rS),E=164 MeV; m e a s u r e d a(0,EOr°)).

82Doi0 8~BaSO

82Boi0

(Tr +,Tr + ) iH(~r+,~r+),E=510 .... MeV; m e a s u r e d polarization aH(~r+,w+),E=65 MeV; m e a s u r e d a(0). aH(~r+,~r+),E=219 .... MeV; m e a s u r e d i T n ( 0 ). sH(~r÷,Tr*),E=120,138 MeV; m e a s u r e d recoil ~He(~r÷,~r+),E=51 MeV; m e a s u r e d g(0).

81Be62 82Ba16 82Bo18 82Gr12 82Ba16

7Li(Tr+jr+),E=143 MeV; m e a s u r e d o'(0),cr(E~r). teC(Tr+Jr+),E=13.9 MeV; m e a s u r e d or(0). leC(~r+jr+),E=29 .... MeV; m e a s u r e d a(0). 4 ° C a ( ~ + J r + ) , E = 6 4 . 8 MeV; m e a s u r e d a(0).

8~GiOl 82Gi08 8ZGu08

82DaI3

(~r+,= +,) 4 H e ( ~ r + , r , + ' ) , E = 9 0 - 3 2 0 MeV; m e a s u r e d a(0,E(~r')). 7Li,(w+,~r+'),E=143 MeV; m e a s u r e d a(O),~(Ew), ~ZC(~r+,~r+'),E=80 MeV; m e a s u r e d tr(O),a(~r').

82Ba19 82Gi0t 82Bl09

teC(~r+Jr+'),E=100 .... MeV; m e a s u r e d cr(0,E(Tr)). 13C(Tr+,Tr+'),E=162 Me¥; m e a s u r e d a(0). 4°Ca(Tr+,vr+'),E=80 MeV; m e a s u r e d cr(O),a(~r').

82Mo01 82Se04

82BI09

(Tr÷,p) aHe(~r+,p),E=50-300 3He(~r+,p),E=400,475 4HeOr*,p),E=50-300 *He(Tr+,p),E=400,475 *~C(Tr+,p),E=400,475

MeV; m e a s u r e d MeV; measured MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

t~(0,Ep). yields. a(0,Ep). yields. yields.

8IKa4t 81Ka43 8lKa41 81Ka43 81Ka43

12C(vr+,p),E=32-81 MeV; m e a s u r e d G(Ep),cr(Ed),o'(O). taC(Tr+,p),E=32-81 MeV; m e a s u r e d a(Ep),cr(Ed),a(0). 1 8 0 ( ~ + , p ) , E = 3 2 - 8 1 MeV; m e a s u r e d a(Ep),a(Ed),a(0). eTAl(Tr+,p),E=50-300 MeV; m e a s u r e d c(O,Ep). 2~Al(Tr+,p),E=400,475 MeV; m e a s u r e d yields.

105

82Do01 82D001 82Do01 81KB4t 81Ka43

REACTION

INDEX

(~T +, 7F+ r i ) teC(Tr+,~r+n),E=30-1O0 MeV; m e a s u r e d

or(E),

82Bu20

l~TI0r+,~r+n),E=60-350

MeV; m e a s u r e d

production

820h07

t ~ ? l ( ~ r + j r ° p ) , E = 6 0 - 3 5 0 MeV; m e a s u r e d

production

820h07

(~r+,p~r ° ) XeC(~r+,~r°p),E=30-100 MeV; m e a s u r e d

a(E).

82Bu20

(~r+,~r+p) C(~r+,rr+p),E=245 MeV; m e a s u r e d a(Ep,Op,O(~r)), C(w+,~r+p),E=165 MeV; m e a s u r e d a(0w,0n),cr(0~r,0p). ~eC(~r+,~r+p),E=130-E00 MeV; m e a s u r e d o'(00r),0p) vs Fe(~r+,~r÷p),E=845 MeV; m e a s u r e d o'(Ep,Op,O(~-)), F e ( ~ ÷ j r * p ) , E = 1 6 5 MeV; m e a s u r e d a(O~r,0n),a(0~r,0p).

82Pi03 82Pi04 81Zi01 82Pi03 82Pi04

BrOr*,~r+p),E=6O MeV; m e a s u r e d a(reaction),a(0p), Ag(~r+,~r+p),E=60 MeV; m e a s u r e d cr(reaction),a(0p), t~TI(~r÷,~r÷p),E=60-350 MeV; m e a s u r e d production B i ( ~ r + j r + p ) , E = 2 4 5 MeV; measured a(Ep,Op,O(~r)), Bi(w+,~r+p),E=165 MeV; m e a s u r e d a(O~r,On),a(Ow,Op).

82Gi03 82Gi03 820h07 82Pi03 82Pi04

(~+,d) 7Li(~r+,d),E=32-81 MeV; m e a s u r e d ~°B(Tr+,d),E=3~-81 MeV; m e a s u r e d ieC(~r+,d),E=32-81 MeV; m e a s u r e d

c~(Ep),a(Ed),a(0). a(Ep),a(Ed),a(0). a(Ep),a(Ed),a(0).

82Do01 82Do01 82Do01

13C(w+,d),E=32-81 MeV; m e a s u r e d ~SO(Tr+,d),E=32-81 MeV; m e a s u r e d iSO(~r+,d),E=32-81 MeV; m e a s u r e d

a(Ep),a(Ed),cr(0). a(Ep),c~(Ed),a(0). a(Ep),cr(Ed),a(0).

82Do01 8~DoO1

82Do01

(n+,2p) Z H ( ~ r ÷ , 2 p ) , E = 8 0 - 4 1 7 MeV; m e a s u r e d

~(0).

82Bo17

a H ( w + , 2 p ) , E = 2 5 6 MeV; m e a s u r e d

iTl~(0 ).

82Sm05

(~+m+d) ~ C ( w + J r + d ) , E = 1 6 0 .... MeV; m e a s u r e d

~(O(~r),Od),

82E107

(~r+,~r+t) ~ZC(~r+,~r+t),E=160 .... MeV; m e a s u r e d

cr(0(~r),Od),

82E107

(n.~) ~H(n,-~),E=fission spectrum; measured E'~,I% ~H(n,7),E=thermal; measured E-/. ZH(n,'~),E=thermal; measured E%t'y,~. 3He(polarized n , 7 ) , E = 9 MeV; m e a s u r e d a ( 0 ) , A ( 0 ) . l~C(n,-~),E=thermal; measured E~/,l'~,a. ~ N ( n , ' y ) , E = 5 . 6 - 1 3 MeV; m e a s u r e d a(0,E),'~(0). ~4Mg(n,7),E=thermal; measured E 7. e°Mg(n,7),E=thermal; measured E 7. ~SMg(n,7),E=thermal; measured ET. ~TAl(n,~),E=thermal; measured E'~,I'~. 3~Cl(n,~,),E=thermal; measured E3~,I'~. 4SSc(n,~/),E=thermal; measured E~',I% ~SFe(n,~/),E=21-42 keV; m e a s u r e d c a p t u r e y i e l d vs E Se(n,30,E=O.O06-40 k e V ; m e a s u r e d a ( c a p t u r e ) v s E. 7~Se(n,~,),E=thermal,resonance; measured E~',I% ~Se(n,~,),E=thermal,resonance; measured E3,,l';~. 77Se(n,~'),E=thermal,resonance; measured E~,I'~. ~Se(n,3,),E=thermal,resonance; measured ET,17. S°Se(n,?),E=thermal,resonanee; m e a s u r e d E7,I7. a a S e ( n , ~ / ) , E = 0 , 0 0 6 - 4 0 keV; m e a s u r e d a(capture) vs E ~SBr(n,~),E=0.05-10 keV; measured transmission,E3,, 7°Br(polarized n,'~),E=thermal; measured S ~ B r ( n , ' ~ ) , E = 0 . 0 5 - 1 0 keV; m e a s u r e d transmission,ET, S~Br(polarized n,7),E=thermal; measured a°Kr(n,3~),E=reaetor; measured production a. SSSr(n,~),E=3-200 keV; measured a(capture). STSr(n,3'),E=3-200 keV; measured a(capture), 9SNb(n,~),E=i0-70 keV; measured a(capture). SSTc(n,~/).E=2.65-2000 k e V ; m e a s u r e d ~ r ( c a p t u r e ) v s ~°Ru(n,'~),E=10.05,... eV; m e a s u r e d E~',I3'. l ° t R u ( n , ~ / ) , E = l S . 9 .... eV; m e a s u r e d E~,I'~. l ° ~ R h ( n , 7 ) , E = 1 0 - 7 0 keV; m e a s u r e d or(capture). i°VAg(n,T),E n o t g i v e n ; m e a s u r e d ET,]7,77-eoin. ~°°Ag(n,3'),E n o t g i v e n ; m e a s u r e d E-?,l~,,I(ce), C d ( n , 7 ) , E = 0 . t 3 5 - 1 0 . 0 1 MeV; m e a s u r e d production c~

82Hs01 t42Nd(n,~'),E=thermal; measured E3'. 8~Val3 Z43Nd(n,3'),E=thermal; measured E3'. 8~Ju01 145Nd(n,7),E=thermal; measured E-y, 82We05 14SSm(n,~),E=thermal; measured E3,,I% 8~Ju01 152Sm(n,3'),E=thermal; measured E3',13'. 82We01 l~4Sm(n,'y),E=thermal; measured E~/,I-y. 8~HuO2 1 5 4 8 m ( n , ~ ' ) , E = t h e r m a l , - > 100 eV,2,24 keV; m e a s u r e d 8~Hu02 15~Gd(n,-~),E=thermal; m e a s u r e d E~,I7. 8~Hu02 15~Gd(n,-]),E=thermal,resonance; measured E%I-/, 8~Sc14 tSSGd(n,'y),E=thermal; measured E3'. 82Kr12 15VGd(n,'y),E=thermal; measured E% 8~Ti02 2SlDy(n,~),E=thermal; measured E% 81Wi15 16ZDy(n,3'),E=thermal; measured I~7. 8EBrI8 la4Dy(n,3'),E=thermal; measured E~. 81En07 t65Ho(n,7),E=thermal; measured E'y. 81En07 lSSHo(n,3,),E=7-15 MeV; m e a s u r e d ¢7(0),a(total) vs E 81En07 lS~Tm(n,~'),E=3-2000 keV; measured or(capture). 81En07 l?3yb(n,7),E=therma]; measured E 7. 81En07 173yb(n,7),E=0.01-0.86 keV; measured E3',13'. 8EBrl8 17~Yb(n,7),E=thermal; measured E3'. 810h09 l?SLu(n,3'),E=thermal; measured 7~/(t). 82VelO Z~SHf(n,3'),E=2.6-2000 keV; measured a(E). 810h09 l~SHf(n,7),E=2.6-20O0 keV; measured a(E). 8EVel0 tS°Hf(n,3,),E=2.6-2000 keV; measured o'(E). 82Ku13 lSiTa(n,~),E=10-70 keV; measured a(eapture). 8EHill leTOs(n,~'),E=thermal; measured l(ce),ET,I% 82Hill lSSpt(n,?),E=thermal; measured I(ce),ET,17. 821~e04 l°~Au(n,'y),E=100-1500 keV; measured a(E) absolute. 8~Ma27 i°VAu(n,~),E=thermal; measured a b s o l u t e I-g. 8aCol5 2 ° s P b ( n , ~ ) , E = O . 8 - 7 . 7 MeV; m e a s u r e d c~(E,0). 82Co15 Z ° o P b ( n , 7 ) , E = 7 - I 3 MeV; m e a s u r e d (7(0). 8~Re04 23~Th(n,T),E=l-408 keV; measured or(E). 81Mi17 ~ 3 ¢ T h ( n , ~ ' ) , E = 1 0 0 - 4 0 0 0 eV; m e a s u r e d capture yield 81Su12 e33U(n,~/),E = 0 . 0 0 2 - 1 MeV; m e a s u r e d a(E). 82Sm06 Z3~U(n,~'),E ~ 0 . 0 0 1 - 1 0 MeV; m e a s u r e d a(E). continued

106

821s05 821s05 821s05 83Ba15 82Bat5 82Ba15 8eSc03 81Be57 82Ba28 821s05 821s05 821s05

82Is05 821s05 82ls05 82Me08 82Ma33 821s05 82Sh04 821s05 81St~8 82Be47 82Be¢7 82Be47 82Re04 82KaE8 82Ka~8 81Ch35 82Ke04 82Jo01 82Ki05 81Ko40 82Pe01 81SulO 81SulO

REACTION

(n,7) t ~ ° C d ( n , 7 ) , E = 0 . 4 - 1 . 5 MeV; m e a s u r e d (;(g) r a t i o s . l*aCd(n,y),E=thermal; measured Ey,IT,yy(0), ~3Cd(n,7),E=thermal; measured ET,IT,I(ce). ~*SCd(n,y),E=2,24 k e V ; m e a s u r e d ET,17,I(ce). nSln(n,y),E=thermal; measured (;,activation nVSn(polarized n,7),E=thermah measured a, ~a3Cs(n,7),E=thermal; measured ET,17,I(ce),77-coin ~aaCs(n,7),E=2.66-600 keV; measured ( ; ( c a p t u r e ) vs laSBa(polarized n,T),E=thermal; measured 7 CP. ~3~Ba(polarized n,7),E=thermal; ~ n e a s u r e d 7 CP. tats(polarized n,7),E=thermal; measured a,

INDEX

continued

82Sm08 82Hu08 82Se09 82Sc09 81St29 81Ko36 81Bo42 82Ma23 78Bo41 78Bo41 81Ko36

2 a e u ( n , y ) , E m O.0Ol-10 MeV; m e a s u r e d atE). 238U(n,T),E ~. 0 . 0 0 1 - 1 0 MeV; m e a s u r e d atE). ZaSU(n,7),E=6.67 .... eV; m e a s u r e d capture yield. ZaSU(n,7),E=thermal; measured capture rate. a a 6 U ( n , y ) , E = 7 - 1 5 MeV; m e a s u r e d ( ; ( 0 ) , a ( t o t a l ) v s E. a a a p u ( n , 7 ) , E ~ 0 . 0 0 1 - 0 . 3 MeV; m e a s u r e d (;(E). z a ° P u ( n , y ) , E m 0 . 0 0 1 - 1 0 MeV; m e a s u r e d atE). Z 4 ° P u ( n , y ) , E m 0 . 0 0 1 - 0 . 3 MeV; m e a s u r e d (;(E). a¢*Am(n,y),E=thermal,3O keV; measured (;(capture), a46Cm(n,7),E=thermah measured ET,IT.

81SulO

1548m(n,e),E=thermat;

82Sc03

81Sul8 82B102 82Di10 82Mc08

81Sul0 81SuI0 81Sul0

82Wi05 82Ho07

(n,e) H3Cd(n,e-),E=thermal;

measured

E%lT,I(ce).

828c09

measured

I(ce).

(n,n) * H ( n , n ) , E = 4 5 - 7 5 MeV; m e a s u r e d ate). * H ( n , n ) , E = 2 1 2 .... MeV; m e a s u r e d a(total),a(O). ~H(n,n),E=0.5,1,2 MeV; m e a s u r e d a(total). 2 H ( n , n ) , E = 1 4 . 7 MeV; m e a s u r e d (;(0). Z H ( n , n ) , E = 2 . 0 1 6 MeV; m e a s u r e d ate). Z H ( p o l a r i z e d n , n ) , E = 1 4 . 1 MeV; m e a s u r e d analyzing Z H ( p o l a r i z e d n , n ) , E = 5 0 MeV; m e a s u r e d At0). Z H ( p o l a r i z e d n , n ) , E = 1 0 MeV; m e a s u r e d analyzing Z H ( p o l a r i z e d n , n ) , E = 5 0 MeV; m e a s u r e d At0). ~ L i ( n , n ) , E = 0 . 1 - 4 . 8 MeV; m e a s u r e d (;(total),(;(0). 7 L i ( n , n ) , E = 1 4 . 7 MeV; m e a s u r e d (;(0). ~Li(n,n),E=2-80 keV; measured (;(E),transmission vs 7Li(polarized n,n),E=0.O02-100 keV; measured (7(E), S B e ( n , n ) , E = 1 4 . 7 MeV; m e a s u r e d (;(0). t ° B ( n , n ) , E = 8 - 1 4 MeV; m e a s u r e d (;tO). H B ( n , n ) , E = 8 .... MeV; m e a s u r e d (;(0). l Z C ( n , n ) , E = 1 4 . 7 MeV; m e a s u r e d ( ; ( E n , 0 ) , i n t e g r a t e d (; ~aC(n,n),E=11.6 MeV; m e a s u r e d (;(0). ~ a C ( n , n ) , E = 2 4 MeV; m e a s u r e d a(En). ~aC(n,n),E=0.5,1,2 MeV; m e a s u r e d a(total). ~ a c ( n , n ) , E = 1 0 - 1 8 MeV; m e a s u r e d (;(0),(;tEn). a s S i ( n , n ) , E = 0 . 6 - 3 . 6 MeV; m e a s u r e d (;(0). 3 a S ( n , n ) , E = 0 . 6 - 3 . 6 MeV; m e a s u r e d (7(0). a a s ( n , n ) , E = 0 . 1 8 - 2 MeV; m e a s u r e d a ( t o t a l ) , ( ; ( 0 ) vs E 4 ° C a ( p o l a r i z e d n , n ) , E = 1 4 MeV; m e a s u r e d Ate). ~ ° C a ( p o l a r i z e d n , n ) , E = 9 . 9 , . . . MeV; m e a s u r e d ATE,0)

5 Z C r ( n , n ) , E = 5 , 6 , 7 MeV; m e a s u r e d ~(O), 5 4 F e ( p o l a r i z e d n , n ) , E = 1 4 MeV; m e a s u r e d At0). Co(n,n),E=slow; measured coherent scattering 5 a N i ( n , n ) , E = 6 , 7 MeV; m e a s u r e d a(0),a(total). 5 6 N i ( n , n ) , E = 0 . 9 - 4 . 5 MeV; m e a s u r e d ( ; ( t o t a l ) v s E, 6 ° N i ( n , n ) , E = 6 , 7 MeV; m e a s u r e d (;(0),a(total). 6 4 N i ( n , n ) , E = 6 , 7 MeV; m e a s u r e d (;(0),a(tota!). 8 S C u ( p o l a r i z e d n , n ) , E = 1 4 MeV; m e a s u r e d At0). Ag(n,n),E=thermal; measured coherent scattering i°VAg(n,n),E=thermal; measured coherent scattering l°SAg(n,n),E=thermal; measured coherent scattering n 3 I n ( n , n ) , E = 6 . 4 7 .... MeV; m e a s u r e d at0), i 1 5 I n ( n , n ) , E = 6 . 4 7 .... MeV; m e a s u r e d (;(0), * l S I n ( n , n ) , E = 5 . 1 9 MeV; m e a s u r e d ( ; ( 0 ) , i n t e g r a t e d (; l Z ° S n ( p o l a r i z e d n , n ) , E = 1 4 MeV; m e a s u r e d At0). P b ( n , n ) , E = l . 5 MeV; m e a s u r e d (;(E,0). a ° s P b ( n , n ) , E = 7 . 2 MeV; m e a s u r e d (;(0). e ° s P b ( p o l a r i z e d n , n ) , E = 1 4 MeV; m e a s u r e d At0). a S g B i ( n , n ) , E = l . 5 MeV; m e a s u r e d (;(E,8). Z 3 a T h ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d (;(e). e S 3 U ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d at0). e a S u ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d at0). 238U(n,n),E=6.67 eV; m e a s u r e d (;,transmission. a a S U ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d (;(0). a a g P u ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d (;(e). 2 4 e P u ( n , n ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d ate).

82Bo15 82Ke02 82Po05 80Ba64 81Wel7 82Br14 82Ro03 82To06 82Wa09 82Sm02 81Ch36 82A116 82A116 81Ch36 82G102 82GI02 81Oul2 81Sa39

82Fi08 82Po05 82Da05 81Si16 81Si16 82Ju02 82F101 82Toll

82Ko30

82F101 82Ki07 81Ko35 82Bu08 81Ko35 81Ko35 82FI01 82Bo12 82Bo12 82Bo12 81Si17

818i17 81Si17 82FI01 820104

82Fi08 82F101 820104 82Ha34 82Ha34 82Ha34 8lSel6 82Ha34 82Ha34

82Ha34

n,n') S L i ( n , n ' ) , E = 3 . 5 - 4 MeV; m e a s u r e d at0). n B ( n , n ' ) , E = 8 .... MeV; m e a s u r e d (;tO). ~aC(n,n'),E=14.9 MeV; m e a s u r e d a(ET,O). l ~ C ( n , n ' ) , E = 1 4 . 7 MeV; m e a s u r e d a(En,e),integrated * e C ( n , n ' ) , E = l t . 6 MeV; m e a s u r e d (;tO). 1 2 C ( n , n ' ) , E = 2 4 MeV; m e a s u r e d (;tEn). l a C ( n , n ' ) , E = 1 0 - 1 8 MeV; m e a s u r e d (~(O),a(En). l~0(n,n'7),E=fission spectrum; measured E7,I7. lSO(n,n'7),E=fission spectrum; measured E7,I7. ~ S F ( n , n ' 7 ) , E = 7 , 1 6 - 2 2 MeV; m e a s u r e d a,ET. l ~ F ( n , n ' ) , E = 1 4 . 9 MeV; m e a s u r e d or(my,0). a ~ M g ( n , n ' ) , E = 1 4 . 9 MeV; m e a s u r e d (;(ET,0). 2 S M g ( n , n ' ) , E = 1 4 . 8 MeV; m e a s u r e d (;(ET,e). a ~ A l ( n , n ' ) , E = 1 4 . 9 MeV; m e a s u r e d (;(E7,0). ~TAl(n,n'7),E=fast; measured Ey,ly,DSA. USSi(n,n'),E=14.9 MeV; m e a s u r e d (;(E7,0). aas(n,n'7),E=fast; measured DSA. 5 a C r ( n , n ' ) , E = 5 , 6 , 7 MeV; m e a s u r e d (;(0). 5 5 M n ( n , n ' 7 ) , E = l - 8 MeV; m e a s u r e d E7,I7. 6 4 F e ( p o l a r i z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d Ate). 5 ~ F e ( n , n ' ) , E = 1 4 . 9 MeV; m e a s u r e d (;(E7,6). 5 e F c ( n , n ' 7 ) , E = 1 4 . 6 MeV; m e a s u r e d E7,I7. 5 6 F e ( p o l a r i z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d Ate). ~SNi(n,n'),E=6,7 MeV; m e a s u r e d (;(8),(;(total). 5 S N i ( n , n ' ) , E = 0 . 9 - 4 . 5 MeV; m e a s u r e d ( ; ( t o t a l ) v s E, 5 S N i ( p o l a r i z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d At0).

1 1 a l n ( n , n ' ) , E = 6 . 4 7 .... MeV; m e a s u r e d ate), ltaln(n,n'),E=fission spectrum; measured average n~ln(n,n'7),E=fast; measured E7,I7. n S l n ( n , n ' ) , E = 0 . 8 8 - 5 . 6 5 , . . MeV; m e a s u r e d atE). n S l n ( n , n ' ) , E = 6 . 4 7 .... MeV; m e a s u r e d ate), n a I n ( n , n ' ) , E = 5 . 1 9 MeV; m e a s u r e d (;(0),integrated a nSIn(n,n'),E=fission spectrum; measured average a 1 2 ° S n ( p o l a r i z e d n , n ' ) , E = t 0 MeV; m e a s u r e d At0). 1528m(n,n'y),E=fast; measured my,IT. 1548m(n,n'y),E=fast; measured Ey,17. 15tEu(n,n'T),E=fast; measured Ey,Iy(E),I?(8). la4Er(n,n'y),E=reaetor spectrum; measured EW,IT. 166Er(n,n'T),E=reactor spectrum; measured Ey,Iy. 166Er(n,n'w),E=reactor spectrum; measured ES',IT. 17°Er(n,n'y),E=reactor spectrum; measured Ey,I7. 18omHf(n,n'),E=thermal; measured or. 79Sh25 1680s(n,n"),),E=0.15-1 MeV; m e a s u r e d a. 82E106 82Ko20 l g ° O s ( n , n ' T ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d (;. 1 9 a O s ( n , n ' 7 ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d (;. 81Ka46 82Gu02 l g 4 P t ( n , n ' T ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d (;. 1 9 6 P t ( n , n ' w ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d a. 79Sh25 1 9 8 P t ( n , n ' y ) , E = O . 1 5 - 1 MeV; m e a s u r e d (;. 82GI06 1 9 8 H g ( n , n ' y ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d or. 82Gu02 199Hg(n,n'),E=fission spectrum; measured average a 81Ko35 a ° ° H g ( n , n ' y ) , E = 0 . 1 5 - t MeV; m e a s u r e d (;. 82Bu08 a ° Z H g ( n , n ' y ) , E = 0 . 1 5 - t MeV; m e a s u r e d or. 82Cu02 continued 82Sm02 82G102 79Sh25 81Gul2 81Sa39 82Fi08 82Da05 82Hs01 82Hs01 78Pr10 79Sh25 79Sh25 79Sh25 798h25 82E104

107

81Si17 82Ko16 78Av08 80Faa0

81Si17 818i17 82Ko18 82Gu02 78De42

78De42 82Bo07 81Bo40 81Bo40 81Bo40 81Bo40 81Ko32

82Po07 82Po07 82Po07 82Po07 82Po07 82Po07 82Po07 81Ko43 82Po07 82Po07

REACTION

( n , n ~) a ° N i ( n , n ' ) , E = 6 , 7 MeV; m e a s u r e d a ( 0 ) , a ( t o t a l ) . 9 ° N i ( p o l a r i z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). S~Ni(n,n'),E=6,7 MeV; m e a s u r e d c t ( 0 ) , a ( t o t a l ) . SSCu(n,n'),E=14.9 MeV; m e a s u r e d a(ET,0). SSCu(n,n'),E=14.0 MeV; m e a s u r e d a(ET,0). ~°Ge(n,n'),E -< 1300 keV; m e a s u r e d a(E). 7eGe(n,n'),E <- 1300 keV; m e a s u r e d a(E). 7~Ge(n,n'),E ~ 1300 keV; m e a s u r e d a(E). 7 ° G e ( n , n ' ) , E -< 1300 keV; m e a s u r e d a(E). ~ a N b ( n , n ' T ) , E = r e a c t o r ; m e a s u r e d ET,IT,T(0). C d ( n , n ' ) , E = 0 . 1 3 5 - 1 0 . 0 1 MeV; m e a s u r e d p r o d u c t i o n ~ n C d ( n , n ' ) , E = 0 . 4 - 1 . 5 MeV; m e a s u r e d a ( E ) r a t i o s .

a

INDEX

continued

81Ko35 82Gu02 81Ko35 79Sh25 79Sh25 78Ef02 78Ef02 78Ef02 78Ef02 82Av05 8~Sm06 82Sm08

a ° 4 H g ( n , n ' T ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d a. 2 ° s p b ( n , n ' T ) , E = 0 . 1 5 - 1 MeV; m e a s u r e d o'. Z ° s p b ( n , n ' ) , E = 7 . 2 MeV; m e a s u r e d (7(0). S ° s p b ( p o l a r i z e d n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 2 S 2 T h ( n , n ' T ) , E = 0 . 8 - 2 . 5 MeV; m e a s u r e d T - y i e l d s . 2 3 e T h ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d a ( 0 ) . e a a U ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d a ( 0 ) . e a S U ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d a ( 0 ) . 2 3 e U ( n , n ' T ) , E = 0 . 8 - 2 . 5 MeV; m e a s u r e d , ) ' - y i e l d s . e g S U ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d a ( 0 ) . Z a S p u ( n , n ' ) , E = 0 . 6 - 3 . 4 MeV; m e a s u r e d a(O). 2 4 e p u ( n , n ' ) , E = 0 . 6 - 3 , 4 MeV; m e a s u r e d a ( 0 ) .

82Ch21 82Ha34 82Ha34 82Ha34 82Ch21 82Ha34 82Ha34 82Ha34

3 a S ( n , p ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e (r. SOV(n,p),E=thermal; measured a(Ea),a(Ep). 51V(n,p),E=fission s p e c t r u m ; m e a s u r e d a v e r a g e a. SlV(n,p),E=14.2 MeV; m e a s u r e d a . S4Fe(n,p),E=fission s p e c t r u m ; m e a s u r e d a v e r a g e a. 5°Fe(n,p),E=fission s p e c t r u m ; m e a s u r e d a v e r a g e a. 5 S N i ( n , p ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e a. S 4 Z n ( n , p ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e a. aaMo(n,p),E=14.2 MeV; m e a s u r e d p r o d u c t i o n cr f o r gTMo(n,p),E=14.2 MeV; m e a s u r e d p r o d u c t i o n t7 f o r gSMo(n,p),E=14.2 MeV; m e a s u r e d p r o d u c t i o n a f o r l°°Mo(n,p),E=14.2 MeV; m e a s u r e d p r o d u c t i o n a f o r

82Ko16 81Wa31 82Ko16 82Wa15 82Ko16 82Ko16 82Ko16 82Ko16 81Sr02 81Sr02 81Sr02 81Sr02

a a Y ( n , 2 n ) , E = 1 2 . 8 - 1 8 MeV; m e a s u r e d a(E). S ° Z r ( n , 2 n ) , E = 1 4 . 5 MeV; m e a s u r e d aOZr(n,2n),E=12.3-1g.5 MeV; m e a s u r e d a. a3Nb(n,2n),E=14.2 MeV; m e a s u r e d a ( E n ) . a2Mo(n,2n),E=14.2 MeV; m e a s u r e d p r o d u c t i o n a f o r a2Mo(n,2n),E=14.5 MeV; m e a s u r e d a4Mo(n,2n),E=14.2 MeV; m e a s u r e d p r o d u c t i o n a f o r C d ( n , 2 n ) , E = 0 . 1 3 5 - 1 0 . 0 1 MeV; m e a s u r e d p r o d u c t i o n a 137Ba(n,2n),E=14.4 MeV; m e a s u r e d p r o d u c t i o n tr f o r l a T A u ( n , 2 n ) , E = 1 4 . 2 MeV; m e a s u r e d a ( E n ) . 1 9 7 A u ( n , 2 n ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e t7

80Hul5 82Fa08 82Pa15 82HaO1 81Sr02 82Fa08 81Sr02 82Sm06 82Ch14 82HaOl 82Ko16

eTZn(n,np),E=14.7 SaZn(n,n'p),E=14.7 °SZn(n,np),E=14.7 °~Zr(n,n'p),E=14.7 a2Zr(n,np),E=14.7 aTMo(n,n'p),E=14.7 97Mo(n,np),E=14.7 aSMo(n,n'p),E=14.7 aaMo(n,np),E=14.7

82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03

82Po07 82Po07 82Fi08 82Gu02

(n,p) 3 H e ( n , p ) , E = 0 . 1 5 - 1 5 0 keV; m e a s u r e d a(E). 6Li(n,p),E=60 MeV; m e a s u r e d a ( E p ) , a ( 0 ) . 12C(n,p),E=60 MeV; m e a s u r e d a ( E p ) , a ( 0 ) . 12C(polarized n,p),E=18 MeV; m e a s u r e d d - a s y m m e t r y . 14N(n,p),E=60 MeV; m e a s u r e d a ( 0 ) . l ° O ( n , p ) , E = 6 0 MeV; m e a s u r e d ~(0). ~2Na(n,p),E=O.02-1000 eV; m e a s u r e d a(E). 24Mg(n,p),E=12-19 MeV; m e a s u r e d a(E). 2 4 M g ( n , p ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e a. aTAl(n,p),E=14.2 MeV; m e a s u r e d a ( E n ) . a ~ A l ( n , p ) , E = f i s s i o n s p e c t r u m ; m e a s u r e d a v e r a g e (~. eaSi(n,p),E=60 MeV; m e a s u r e d a(Ep),a(O). eaSi(n,p),E=59.6 MeV; m e a s u r e d a ( 0 ) .

82Bo19 82Br04 82Br04 82De16 82Ne04 82Ne04 82G107 81Li27 82Ko16 82Ha01 82Ko16 82Br04 82U101

(n,2n) 2 H ( n , 2 n ) , E = 1 4 . 7 MeV; m e a s u r e d a ( 0 ) . 1 a F ( n , 2 n T ) , E = 7 , 1 6 - 2 2 MeV; m e a s u r e d cr,E T. l a F ( n , 2 n ) , E = 1 4 . 9 MeV; m e a s u r e d a(ET,0). 45Sc(n,2n),E=13.15-18.26 MeV; m e a s u r e d a , i s o m e r i c 5 5 M n ( n , 2 n ) , E = 1 2 . 3 - 1 8 . 3 MeV; m e a s u r e d a(E). 56Fe(n,2n),E=14.9 MeV; m e a s u r e d a(ET,0). 5eFe(n,2nT),E=14.6 MeV; m e a s u r e d ET,IT. 5 a c o ( n , 2 n ) , E = 1 2 . 4 9 - 1 8 . 2 6 MeV; m e a s u r e d a ( E ) 5aNi(n,2n),E=14.2 MeV; m e a s u r e d a ( E n ) . 7 4 G e ( n , 2 n ) , E = 1 4 . 4 MeV; m e a s u r e d p r o d u c t i o n a f o r 74Se(n,2n),E=14.5 MeV; m e a s u r e d aSSr(n,2n),E=14.5 MeV; m e a s u r e d

80Ba64 78Pr10 79Sh25 80Ma47 80Lu09 79Sh25 82G106 81Hull 82Ha01 81Ch41 82Fa08 82Fa08

(n,np) 44Ca(n,n'p),E=14.7 44Ca(n,np),E=14.7 49Ti(n,n'p),E=14.7 4STi(n,np),E=14.7 5°Cr(n,n'p),E=14.7 5°Cr(n,np),E=14.7 SaCu(n,np),E=14.9 SSCu(n,np),E=14.9 SVZn(n,n'p),E=14.7

MeV; MeV; MeV; MeV; MeV; MeV; MeV; MeV; MeV;

m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a(ET,0). m e a s u r e d a(ET,0). m e a s u r e d a.

82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 79Sh25 79Sh25 82Qa03

MeV; MeV; MeV; MeV; MeV; MeV; MeV; MeV; MeV;

m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d cr. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a. m e a s u r e d a.

(n,d) t H ( n , d ) , E = 7 9 5 MeV; m e a s u r e d a ( 0 ) v s d e u t e r o n 4 H e ( p o l a r i z e d n , d ) , E = 5 0 MeV; m e a s u r e d a n a l y z i n g SLi(n,d),E=14.1 MeV; m e a s u r e d a(O),a(Ed,0). SLi(n,d),E=14.1 MeV; m e a s u r e d a ( E d ) , a ( E t ) , a ( E a ) , l a F ( n , d T ) , E = 7 , 1 6 - 2 2 MeV; m e a s u r e d cr,ET. t a F ( n , d ) , E = 1 4 . 9 MeV; m e a s u r e d a(ET,0). STAl(n,d),E=14.9 MeV; m e a s u r e d a(ET,0). 44Ca(n,d),E=14.7 MeV; m e a s u r e d a .

4STi(n,d),E=14.7 5°Cr(n,d),E=14.7 67Zn(n,d),E=14.7 Sezn(n,d),E=14.7 aeZr(n,d),E=14.7 07Mo(n,d),E=14.7 SeMo(n,d),E=14.7

82Ho08 82Sa05 82Hi06 82Sh19 78PrlO 79Sh25 79Sh25 82Qa03

MeV; MeV; MeV; MeV; MeV; MeV; MeV;

measured measured measured measured measured measured measured

~. a. or. ~. a. cr. or.

82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03 82Qa03

(n,t) aLi(n,t),E=14.1 MeV; m e a s u r e d ° L i ( n , t ) , E = 1 4 . 1 MeV; measured

~(0),a(Ed,O).

o(Ed),tT(Et),a(Ea),

82Hi06 2 7 A l ( n , t ) , E = 1 6 - 2 0 MeV; m e a s u r e d 82Sh19 SSCo(n,t),E=16-20 MeV; m e a s u r e d continued

108

a(E). ~(E).

82QaO1 82QaOl

REACTION

(n,t) SBe(n,t),E~14.1

MeV; m e a s u r e d

a(Ed),cr(Et),ff(Etx),

INDEX

continued

82Sh19

9SNb(n,t),E=16-20

MeV; m e a s u r e d

tx(E).

82QaOI

(n,aHe) 4 ° C a ( n , S H e ) , E = 1 4 . 6 MeV; m e a s u r e d

~(0).

81Mi16

(n,~) g B e ( n , a ) , E = 1 4 . 1 MeV; m e a s u r e d a(Ed),o'(Et),ff(Ea), ~ F ( n j x ) , E = 1 4 . 9 MeV; m e a s u r e d a(E%0). M g ( n , a ) , E = 1 4 . 1 , 1 4 . 7 MeV; m e a s u r e d production cr f o r S 4 M g ( n , a ) , E = 1 4 . 9 MeV; m e a s u r e d ~r(E7,0). S a S i ( n , a ) , E = 1 4 . 9 MeV; m e a s u r e d ~(E7,0). S ~ p ( n , a ) , E = 1 3 - 1 8 MeV; m e a s u r e d c r ( t o t a l ) v s E. 5 * V ( n , a ) , E = 1 3 - 1 8 MeV; m e a s u r e d a ( t o t a l ) v s E. ~ l V ( n , a ) , E = 1 4 . 2 MeV; m e a s u r e d a. ~ S M n ( n , a ) , E = t 3 - 1 8 MeV; m e a s u r e d ~ r ( t o t a l ) v s E. S a C o ( n , a ) , E = 1 3 - 1 8 MeV; m e a s u r e d a ( t o t a l ) v s E.

82Sh19 79Sh25 79Re09 79Sh25 79Sh25 80Zu02 80Zu02 82Wa15 BOZu0Z 80Zu02

5 9 C o ( n , a ) , E = 1 2 . 4 9 - 1 8 . 2 6 MeV; m e a s u r e d or(E) 5SCo(n,et),E=fission spectrum; measured a v e r a g e or. 7 5 A s ( n , a ) , E = 1 3 - 1 8 MeV; m e a s u r e d a ( t o t a l ) vs E. SSNb(n,a),E=14.1 MeV; m e a s u r e d (x(Etx),a(O). 9 a N b ( n , a ) , E = 1 4 . 2 MeV; m e a s u r e d o ( E n ) . 9 2 M o ( n , a ) , E = 1 4 . 2 MeV; m e a s u r e d production cr f o r l S g L a ( n , a ) , E = 1 3 - 1 8 MeV; m e a s u r e d o r ( t o t a l ) vs E. 143Nd(n,a),E=12.3 .... MeV; m e a s u r e d ff(O),a(O,EoO. 14SNd(n,~J,E=2 k e Y ; m e a s u r e d a(E~). tSSGd(n,a),E=thermal; measured cr(Ea),cr(Ep).

81Hull 82Kot6 80Zu02 82Fi12 8ZHa0{ 81Sr02 80Zu02 81Au09 82Ce01 81Wa31

(n,nc¢) 12C(n,na),E=14.7

MeV; m e a s u r e d

¢(En,O),integrated

81Gu12

(n,2~) 9Be(n,2a),E=14.1

MeV; m e a s u r e d

a(Ed),cr(Et),a(Ect),

82Sh19

(n,F) S°aBi(n,P),E=14.7 MeV; m e a s u r e d o'(fission). aaaTh(n,P),E=thermal; measured fragment kinetic eaaTh(n,F),E=thermal; measured E7,17. ~ 3 2 T h ( n , F ) , E = 0 . 7 - 3 0 MeV; m e a s u r e d a(fission) ratio a32Th(n,F),E=reactor spectrum; measured a33U(n,F),E=thermal; measured independent yield of eZSU(n,F),E=reaetor spectrum; measured SaaU(n,F),E=thermal; measured independent isomeric aSSU(n,F),E=thermal; measured 17,13am,lS4rnl,lSSmXe Z~U(n,F),E=O.17,... MeV; m e a s u r e d y i e l d s vs E f o r ~SSU(n,F),E=thermal; measured independent y i e l d o f e35U(n,F),E=thermal; measured cumulative fission e 3 5 U ( n , F ) , E = O . 0 2 - 3 0 MeV; m e a s u r e d a(fission) ratio S S ~ U ( n , F ) , E = 0 . 7 - 3 0 MeV; m e a s u r e d ~(fission) ratio aaSu(n,F),E=thermal; measured fragment mass, *3~U(n,F),E=thermal; measured 17,~SSm,la4rnl,ts~mXe S~SU(n,F),E=IO-200 keV; m e a s u r e d a(total), eS~U(n,F),E=thermal,600 keV; measured proton, ZSSU(n,F),E=13.5-14.8 MeV; m e a s u r e d ~ ( f i s s i o n ) eSSU(n,F),E=14.1 MeV; m e a s u r e d a . z : ~ U ( n , F ) , E = 0 . 2 - 1 . 2 MeV; m e a s u r e d a(absolute).

81Ba60 82As02 82Di03 82Be31 82Er03 81Jo04 82Be07 82DaOl 82Fu08 81GI04 81Jo04 82Au05 82Be08 82Be31 82Fa05 82Fu08 82Go08 82Si08 82Va12 82WaO1 82Wa08

2 3 S U ( n , F ) , E = 0 . 5 5 - 1 . 2 5 MeV; m e a s u r e d o ~ ( f r a g m e n t 9), a S S U ( n , F ) , E = 0 . 8 5 - 3 . 2 3 MeV; m e a s u r e d c T ( f r a g m e n t 0), aSSU(n,F),E=0.86,1.8 MeV; m e a s u r e d a(fragment 0). 2 3 a U ( n , F ) , E ~ 1 2 . 7 5 - 1 6 . 0 3 MeV; m e a s u r e d 2 3 a U ( n , F ) , E = 1 3 . 5 - 1 4 . 8 MeV; m e a s u r e d o'(fission) aSTNp(n,F),E=reactor spectrum; measured 2 3 ~ N p ( n , F ) , E = 0 . 0 2 - 3 0 MeV; m e a s u r e d or(fission) a 3 7 N p ( n , F ) , E = 1 3 . 5 - 1 4 . 8 MeV; m e a s u r e d or(fission) 2aBpu(n,F),E=reactor spectrum; measured e a g P u ( n , F ) , E = 0 . I - I . 5 MeV; m e a s u r e d average prompt 2agPu(n,F),E=thermal; measured independent yield aaSpu(n,F),E=thermal; measured 17,1sem,lS4mI, S S a P u ( n , F ) , E = 1 3 . 5 - 1 4 . 8 MeV; m e a s u r e d a(fission) S 3 a p u ( p o l a r i z e d n , F ) , E = 0 . O I - 0 . 3 eV; m e a s u r e d s~SPu(n,F),E=reactor spectrum; measured S41Pu(n,F),E=thermal; measured complementary a41Pu(n,F),E=reactor spectrum; measured Z4*Am(n,F),E=reaetor spectrum; measured 245Cm(n,F),E=thermal; measured absolute fission 24sCf(n,F),E=thermal; measured absolute yields for

81Sh23 81Sh23 81Ye0E 81Zh05 82Va12 82Be07 82Be08 82Vale 82BED7 80Zh04 BIJo04 82Fu08 82ValE 82Va17 82BeO7 82AI13 82BeO7 82Be07 82Ra09 81GuI3

(n,X) ~Li(n,X),E=2-80 keY; measured c~(E),transmission vs S ~ S ( n , X ) , E = 0 . 1 8 - 2 MeV; m e a s u r e d a(total),a(0) vs E Ti(n,X),E=thermal; measured a(total),t;(absorption) 7~JBr(n,X),E=0.05-10 k e V ; m e a s u r e d transmission,ET, ~Br(polarized n,X),E=thermal; measured aIBr(n,X),E=0.05-10 keV; measured transmission,ET, SlBr(polarized n,X),E=thermal; measured H S S n ( n , X ) , E = 0 . 3 - 5 MeV; m e a s u r e d transmission. i l T S n ( p o l a r i z e d n,X),E = 0 . 7 5 - 2 . 3 eV; m e a s u r e d HTSn(polarized n,X),E~thermal; measured o, ~ S S n ( n , X ) , E = 0 . 3 - 5 MeV; m e a s u r e d transmission. *S°Sn(n.X),E=0.3-5 MeV; m e a s u r e d transmission. ~ a a S n ( n , X ) , E = 0 . 3 - 5 MeV; m e a s u r e d transmission.

BaAII6 82Ju02 82Ga14 810h09 82VelO 810h09 82VelO 82Ha47 81A128 8t/o36 82Ha47 82Ha47 82Ha47

l a 4 S n ( n , X ) , E = O . 3 - 5 MeV; m e a s u r e d transmission. *SSLa(polarized n,X),E=thermah measured ~, L S S L a ( p o l a r i z e d n , X ) , E = 0 . 7 5 eV; m e a s u r e d ~3%a(n,X),E ~ 0 . 7 3 4 eV; m e a s u r e d transmission. * 4 * P r ( p o l a r i z e d n,X),E=O.O01-100 keV; m e a s u r e d l S ° T b ( p o l a r i z e d n , X ) , E = O . 0 0 1 - l O 0 keY; m e a s u r e d l S S H o ( p o l a r i z e d n,X),E=O.O01-1OO k e V ; m e a s u r e d lSTEr(polarized n,X),E=0.O01-100 keV; measured 1 S a T i n ( p o l a r i z e d n,X),E=O.O01-100 k e V ; m e a s u r e d ZSSTh(n,X),E=O.O07-15 e V , O . O l S - 4 k e V ; m e a s u r e d aaSU(n,X),E=6.67 eV; m e a s u r e d a,transmission. 2 4 S C m ( n , X ) , E = 0 . 4 - 6 6 eV; m e a s u r e d transmission.

109

82Ha47 81Ko36 82Algl 82Ve07 82A103 82AI03 82AI03 82Al03 82AI03 820106 81SeI6 BiAn25

REACTION INDEX

(P,7) SH(p,7),E=8-30 MeV; m e a s u r e d a(E,0). aBe(p,7),E=320 keY; m e a s u r e d t~(ET),IT. lZB(p,T),E=5-14 MeV; m e a s u r e d ET,absolute ltB(p,v),E=0.82-2.83 MeV; m e a s u r e d a(O) vs E,T(0). l~B(p,T),E=23-60 MeV; m e a s u r e d a(E). r i B ( p o l a r i z e d p,T),E=28.7 MeV; m e a s u r e d a(0),A(0). HB(p,v),E=2.9-4.6 MeV; m e a s u r e d Ev,lT,cr(0) vs E. ~aC(p,T),E=l.75 MeV; m e a s u r e d a(E,Bp,0). ~ZNe(p,7),E=70-355 keV; m e a s u r e d a(ET,E),E7, e~Ne(p,7),E=70-355 keV; m e a s u r e d a(ET,E),ET, 65Mg(p,7),E=l.716 MeV; m e a s u r e d ")'(0). ZSMg(p,T),E=resonance; m e a s u r e d ET,IT, eSMg(p,T),E=600-1730 keV; m e a s u r e d a(E). ~SMg(p,v),E=774,880 keV; m e a s u r e d ET,17,Doppler eSMg(p,T),E=l.2 MeV; m e a s u r e d cr(E,ET,0),DSA.

82Mc03 82Ri04 82Coll 82Ha12 82We08 82We08 82WrO1 81Bi17 82Goll 82Goll 81Ko38 82Al19 82An01 82De15 82Ke08

2SMg(p,7),E=l.4-2.2 MeV; m e a s u r e d ET,DSA. 2SMg(p,7),E=0.29-2.2 MeV; m e a s u r e d cr(E,E(7)),ET, 2~Al(p,7),E=2.16,2.312 MeV; m e a s u r e d ET,17,DSA. 4ZK(p,7),E=0.68-2.48 MeV; m e a s u r e d "},,neutron 4eCa(p,7),E=0.63-3.01 MeV; m e a s u r e d 7 - r a y , n e u t r o n 44Ca(p,7),E=0.775-5.05 MeV; m e a s u r e d 7 - r a y , n e u t r o n 5°Cr(p,7),E=3.2-3.3 MeV; m e a s u r e d cr(ET,E). ~Cr(p,T),E=4.14-4.2 MeV; measured ET,/T,T(8),a(8) 5aCr(p,7),E=0.88-2.4 MeV; m e a s u r e d a(E). 5eNi(p,7),E=2839 .... keV; m e a s u r e d 7(0). aeKr(p,7),E=2.8 MeV; m e a s u r e d ET,17,DSA. 84Kr(p,7),E=l.85-2.87 MeV; m e a s u r e d ET,IT,77-coin, aSsr(p,7),E=2.2-3.7 MeV; m e a s u r e d a(E). aay(p,7),E=2.6-3.3 MeV; m e a s u r e d a(E).

82Anll 82Sm04 81G105 82Se02 82Mi06 82Mi06 82Br03 82K106 8 1 G a3 8 82Sz01 82Fa12 82Fa09 82DyO1 82Dy01

(p,=) H ( p o l a r i z e d p,~r),E=515,578 MeV; m e a s u r e d s p i n

82ApOl

(p,.-) aBe(polarized p,vr-),E=200,... MeV; m e a s u r e d lZC(polarized p,vr-),E=183 MeV; m e a s u r e d a(E(~r)), laC(polarized p,~r-),E=183 MeV; m e a s u r e d cr(E(~r)), *~C(polarized pJr-),E=183 MeV; m e a s u r e d a(E(~r)), Z~C(pjr-),E=183 MeV; m e a s u r e d a(O,E(vr)),tr(O).

82Lo02 82Ja05 82Ja05 82Ja05 82Vi05

'80(p,~r-),E=191 MeV; m e a s u r e d ty(e,E(vr)),a(e). 4eCa(p,~v-),E=206 MeV; m e a s u r e d a(O,E(~r)),a(e). 4eCa(p,~r-),E=206 MeV; m e a s u r e d a(O,E(~r)),a(e). aaY(p,~r-),E=206 MeV; m e a s u r e d a(8,E(~r)),a(O). 9SZr(p,vr-),E=206 MeV; m e a s u r e d a(O,E(Ir)),a(O).

82Vi05 82Vi05 82Vi05 82Vi05 82Vi05

(pjr +) 1H(polarized ill(polarized ZH(polarized aBe(polarized

p,~r+),E=515-583 MeV; measured (7(8), pjr÷),E=400,450 MeV; m e a s u r e d pjr+),E=305 .... MeV; m e a s u r e d or(E,0), p,~r+),E=200-250 MeV; m e a s u r e d A(0).

81Fo13 82Fa07 82Lo17 82Au02

leC(polarized p,~r+),E=200-250 MeV; m e a s u r e d g(e), lSO(p,Tr+),E=149--166 MeV; m e a s u r e d or(O). eaSi(pjr+),E=149-166 MeV; m e a s u r e d a(@).

82Lo03 81Sj03 8lSj03

(p,n) ZH(p,n),E=800 MeV; m e a s u r e d P(On). SH(p,n),E=l.3,1.8 MeV; m e a s u r e d or(0). SH(p,n),E=9.77-14.77 MeV; m e a s u r e d or(0=0 s) vs E. 7Li(p,n),E=60-200 MeV; measured ~(0=0°). 7Li(p,n),E=60-200 MeV; m e a s u r e d total ¢7(reaction) 12C(p,n),E=62-160 MeV; m e a s u r e d ~(0=0 °) vs E. laC(p,n),E=60-200 MeV; m e a s u r e d if(O=0°). 14C(p,n),E=60-200 MeV; m e a s u r e d ¢7(0=0°). l°0(p,n),E=62-160 MeV; m e a s u r e d ~(O=0 °) vs E. 160(p,n),E=99.1,135.2 MeV; m e a s u r e d ~(En) vs 0. leO(polarized p,n),E=134 MeV; m e a s u r e d o'(O),tT(En), 160(p,n),E=35 MeV; m e a s u r e d a(En),a(0). laO(p,n),E=35 MeV; m e a s u r e d a(En),a(0). la0(p,nT),E=4.4-4.62,... MeV; m e a s u r e d y i e l d s , a ( E ) 24Mg,(p,n),E=62-160 MeV; m e a s u r e d cr(O=Os) vs E. a4Mg(p,n),E=35 MeV; m e a s u r e d cr(En),a(0). 2~Mg(p,n),E=62-160 MeV; m e a s u r e d a(O=O°) vs E. a°Mg(p,n),E=60-200 MeV; m e a s u r e d cr(O=OS). a~Al(p,n),E=~ MeV; measured a(En). ~aSi(p,n),E=62-160 MeV; m e a s u r e d cr(O=O°) vs E. avCl(p,n),E=60-200 MeV; m e a s u r e d or(0=0°). ~lK(p,n),E=D.68-2.48 MeV; m e a s u r e d 7 , n e u t r o n 42Ca(p,n),E=160 MeV; m e a s u r e d a(0,En). 4aCa(p,n),E=60-200 MeV; m e a s u r e d a(O=O°). ~4Ca(p,n),E=0.775-5.05 MeV; m e a s u r e d 7 - r a y , n e u t r o n ~aCa(p,n),E=62-160 MeV; m e a s u r e d a(O=Os) vs E. 4SSe(p,n),E=2.9-4 MeV; m e a s u r e d 7 - r a y , n e u t r o n ~Cr(p,n),E=22 MeV; m e a s u r e d a(En). ~SCr(p,n),E-0.88-2.4 MeV; m e a s u r e d a(E). ~aCr(p,n),E=22 MeV; m e a s u r e d a(En). S4Fe(p,n),E=28-35 MeV; m e a s u r e d or(0). 5eFe(p.n),E=22 MeV; m e a s u r e d cr(En). 5SFe(p,n),E=28-35 MeV; m e a s u r e d a(0). ~aNi(p,n),E=22 MeV; measured t~(En).

82BhO1 81Ch37 82Th07 82Ta03 82Wa02 82An08 82Ta03 82Ta03 82An08 82Fa06 82Mall 820h03 8fiOr04 82Dill 82An08 820r01 82An08 82Ta03 82Bi04 82An08 82Ta03 82Se02 81Go18 82Ta03 82Mi06 82An08 82Mi 06 82Bi04 81Ga38 82Bi04 820h02 82Bi04 820h02 82Bi04

°°Ni(p,n),E=22 MeV; m e a s u r e d a(En). eZNi(p,n),E=22 MeV; m e a s u r e d a(En). SSCu(p,n),E=5-7.8 MeV; m e a s u r e d ET,IT(e),TT-coin. 76Se(p,n),E=6.7 MeV; m e a s u r e d ET,Iv,77-coin,a(E7), 76Se(p,n),E=19,20,22,25 MeV; m e a s u r e d a(En),a(O). aOSe(p,n),E=la,20,22,25 MeV; m e a s u r e d a(En),cr(O). SZSe(p,n),E=19,20,22,25 MeV; m e a s u r e d cr(En),a(O). aaKr(p,n),E=2.8 MeV; m e a s u r e d ET,IT,DSA. S°Kr(p,n),E=2.8 MeV; m e a s u r e d ET,17,DSA. SSy(p,n),E=5-9 MeV; m e a s u r e d 9°Zr(p,n),E=22 MeV; m e a s u r e d a(E.n). S°Zr(p,n),E=7.8 MeV; m e a s u r e d I(ce),Tl/z. 91Zr(p,n),E=22 MeV; m e a s u r e d cr(En). S4Zr(p,n),E=22 MeV; m e a s u r e d a(En). 9aZr(p,nT),E=l.3-5.1 MeV; m e a s u r e d ET,17,a(ET). aSZr(p,n),E=2-6.5 MeV; m e a s u r e d t o t a l or(E). aVMo(p,nT),E=2-5.2 MeV; m e a s u r e d E T , 1 7 , n T - , 7 7 - c o i n "8Mo(p,n),E=2.4-4 MeV; m e a s u r e d ET,17,I(ce), la°Mo(p,nT),E=l.2-3.6 MeV; m e a s u r e d ET,17,a(ET). l°°Mo(p,n),E=2-6.5 MeV; m e a s u r e d t o t a l a(E). l°sPd(p,nT),E=6.05 MeV; m e a s u r e d I(ce). l°aAg(p,nT),E=3.4,3.9 MeV; m e a s u r e d ET,IT,DSA. Jl°Cd(p,n),E=Z5 MeV; m e a s u r e d ~(8). llsCd(p,n),E=22 MeV; m e a s u r e d a(En). l*4Cd(p,n),E=25 MeV; m e a s u r e d a(O). naCd(p,n),E=e5 MeV; m e a s u r e d or(O). 1151n(p,n),E=22 MeV; m e a s u r e d a(En). 12eSn(p,n),E=22 MeV; m e a s u r e d cr(En). 124Te(p,n),E=3.9-6 MeV; m e a s u r e d ET,IT,77-eoin, *2aTe(p,n),E=2.8-5 MeV; m e a s u r e d ET,17,77-coiin, lS°Hf(p,n),E=6.5-9 MeV; m e a s u r e d ET,IT,E(X-ray), *alTa(p,n),E=22 MeV; m e a s u r e d cr(En). aS2Th(p,n),E=8-22 MeV; m e a s u r e d a ( f i s s i o n ) ,

110

82Bi04 82Bi04 82PaOl 82Doll 82Wo06 82Wo06 82Wo06 82Fa12 82Fa12 81Sk04 82Bi04 82Hu01 82Bi04 82Bi04 81Ar24 82FI03

82Ka26 82Ar12 81Ar24 82F103 78Za12 82Av07 82MuOl 82Bi04 82Mu01 82MuOI 8~Bi04 82Bi04 82Bu12

81Bu22 8ZNo09 82Bi04 82Ku07

REACTION

INDEX

(P,P) ~H(polarized p,p),E=579 MeV; m e a s u r e d P(0), *H(polarized p,p),E=550-950 MeV; m e a s u r e d ~H(polarized p,p),E=950 MeV; m e a s u r e d a s y m m e t r y , *H(p,p),E=515-583 MeV; m e a s u r e d at(0=90°). *H(polarized p,p),E=5.05,9.85 MeV; m e a s u r e d ~H(p,p),E=529,556,582 MeV; m e a s u r e d a(0). *H(polarized p,p),E=500-800 MeV; m e a s u r e d s p i n *H(p,p),E=516-58Z MeV; m e a s u r e d at(0=90°). ~H(p,p),E=796 MeV; m e a s u r e d (~(O),A(0). %[(polarized p,p),E=796 MeV; m e a s u r e d a(O),A(O). ~H(polarized p,p),E=800 MeV; m e a s u r e d s p i n ~I=[(polarized p,p),E=643 MeV; m e a s u r e d a n a l y z i n g *H(polarized p,p),E=647 MeV; m e a s u r e d s p i n *H(p,p),E at 0.846-1.99 GeV/c; m e a s u r e d a(0). ZH(p,p),E=l GeV; m e a s u r e d P(0). eH(p,p),E=0.6-2.7 GeV; m e a s u r e d at(0) vs E. all(polarized p,p),E=10 MeV; m e a s u r e d at(0),A(0). ell(polarized p,p),E=64.8 MeV; m e a s u r e d A(0). aHe(p,p),E=700-1700 MeV; m e a s u r e d a(0). 4He(p,p),E=992 MeV; m e a s u r e d at(0). °Li(p,p),E=136 MeV; m e a s u r e d at(0). SLi(p,p),E=24.4 MeV; m e a s u r e d (~(Ep'),at(0). ~Li(p,p),E=24.4 MeV; m e a s u r e d (r(Ep'),at(0). tZC(p,p),E=l GeV; m e a s u r e d P(6). ~ZC(p,p),E=l.5-l.9 MeV; m e a s u r e d or(E). ~SC(p,p),E=l.75 MeV; m e a s u r e d cr(E,Ep,0). ~SC(p,p),E=135 MeV; m e a s u r e d at(0). 160(p,p),E=l GeV; m e a s u r e d a(O). ~0(p,p),E=l GeV; m e a s u r e d P(0). *SO(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). *~0(polarized p,p),E=6.461-6.487 MeV; m e a s u r e d ~¢Mg(p,p),E=0.8 GeV; m e a s u r e d at(0). ZaMg(polarized p,p),E=3.89-4.17 MeV; m e a s u r e d Z4Mg(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). ZdMg(polarized p,p),E=134.7 MeV; m e a s u r e d at(e), ZSMg(p,p),E=0.8 GeV; m e a s u r e d G(0). eaSi(p,p),E=~ GeV; m e a s u r e d or(O). ZSSi(polarized p,p),E=65 MeV; m e a s u r e d cr(0),A(0), ZSSi(polarized p,p),E=134.5 MeV; m e a s u r e d at(0), aZS(p,p),E=l GeV; m e a s u r e d at(O). 4~Ar(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). SaK(p,p),E=l GeV; m e a s u r e d at(O). a~Ca(polarized p,p),E=497 MeV; m e a s u r e d s p i n 4°Ca(p,p),E=l GeV; m e a s u r e d o'(0). ~aCa(p,p),E=l GeV; m e a s u r e d P(O). 4°Ca(p,p),E~0.8 GeV; m e a s u r e d at(Ep'),a(0),A(0). ~°Ca(polarized p,p),E=0.8 GeV; m e a s u r e d (~(Ep'), ¢°Ca(polarized p,p),E=65 MeV; m e a s u r e d G(0),A(0). ~°Ca(polarized p,p),E=80.2,181.5 MeV; m e a s u r e d 4~Ca(polarized p,p),E=65 MeV; m e a s u r e d at(O),A(0). *SCa(p,p),E~l GeV; m e a s u r e d a(0).

aaCa(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). 46Ti(polarized p,p),E=800 MeV; m e a s u r e d a(0), 4aTi(polarized p,p),E=65 MeV; m e a s u r e d o'(O),A(0). 4aTi(polarized p,p),E=800 MeV; m e a s u r e d a(0), ~aTi(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). 5°Ti(polarized p,p),E=65 MeV; m e a s u r e d ~(O),A(O). ~tV(p,p),E=8.O5 MeV; m e a s u r e d at(O). ~lV(p,p),E=5.39-6.05 MeV; m e a s u r e d or(E). SOCr(p,p),E=5.20-6.05 MeV; m e a s u r e d at(E). 5ZCr(p,p),E=5.20-6.05 MeV; m e a s u r e d tr(E). SaCr(p,p),E=4.59-4.72 MeV; m e a s u r e d at(0) vs E. SSCr(p,p),E=5,20-6.05 MeV; m e a s u r e d cr(E). SdCr(p,p),E=5.20-6.05 MeV; m e a s u r e d tr(E). SdFe(p,p),E=5.20-6.05 MeV; m e a s u r e d at(E). 54Fe(polarized p,p),E=65 MeV; m e a s u r e d at(0),A(0). 56Fe(p,p),E=5.20-6,05 MeV; m e a s u r e d or(E). 56Fe(p,p),E=3.1-4.2 MeV; m e a s u r e d cr(IE,O). 56Fe(polarized p,p),E=65 MeV; m e a s u r e d a(O),A(0). 57Fe(p,p),E=5.20-6.05 MeV; m e a s u r e d or(E). 5aFe(p,p),E=5.20-6.05 MeV; m e a s u r e d at(E). aaNi(polarized p,p),E=65 MeV; m e a s u r e d (r(0),A(0). ~QNl(polarized p,p),E=65 MeV; m e a s u r e d cr(0),A(O). 6aNi(polarized p,p),E=65 MeV; m e a s u r e d cr(O),A(0). 6aNi(polarized p,p),E=65 MeV; m e a s u r e d ¢(0),A(0). SdZn(p,p),E=2.88-5.02 MeV; m e a s u r e d a(0). SaSr(p,p),E=6.06 MeV; m e a s u r e d at(0),K-shell Say(polarized p,p),E=65 MeV; m e a s u r e d G(0),A(0). aOZr(polarized p,p),E=800 MeV; m e a s u r e d or(0), g°Zr(p,p),E=l GeV; m e a s u r e d or(O). 9°Zr(p,p),E=l GeV; m e a s u r e d P(O). 9aZr(polarized p,p),E=65 MeV; m e a s u r e d ~(8),A(O). g%r(polarized p,p),E=79.6 .... MeV; m e a s u r e d a(8), aaZr(polarized p,p),E=80O MeV; m e a s u r e d q(0), S2Zr(polarized p,p),E=104 MeV; m e a s u r e d at(0), SaMo(polarized p,p),E=65 MeV; m e a s u r e d a(e),A(0). i°°Mo(polarized p,p),E=65 MeV; m e a s u r e d o'(0),A(O). ~aCRu(p,p),E=29 MeV; m e a s u r e d q(O). Ag(p,p),E=150-400 keV; m e a s u r e d at(E). lZ°Sn(polarized p,p),E=104 MeV; m e a s u r e d a(e), i44Sm(polarized p,p),E=65 MeV; measured at(O),A(O). 14~Sm(p,p),E=l.04 GeV; m e a s u r e d ~(0), i~sSm(p,p),E=l.04 GeV; m e a s u r e d at(0). iSZSm(p,p),E=l.04 GeV; m e a s u r e d at(0). Au(p,p),E=150-400 keV; m e a s u r e d a(E). easPb(p,p),E=l GeV; m e a s u r e d at(0). 26aPb(p,p),E=[ GeV; m e a s u r e d P(O). eOaPb(polarized p,p),E=65 MeV; m e a s u r e d ~r(O),A(0). a°aPb(polarized p,p),E=79.8 .... MeV; m e a s u r e d at(0) e°sBi(polarized p,p),E=65 MeV; m e a s u r e d O(0),A(O). USaTh(p,p),E=26 MeV; m e a s u r e d at(0). 2SSU(p,p),E=26 MeV; m e a s u r e d a(O).

81Ap01 81Bo41 8[Bo43 8tFa08 82Ba09 82Be37 82Bh03 82Chlt 821r01 821r01 82Me04 82Mc05 82Mc07 82Sh22 82A118 82Be30 82Do07 82Sh13 81Be52 82~eQ3 81He21 82Pe06 82Pe06 82A118 82Tall 8IBi17 82C008 82A118

82A118 82Sa19 82Se01 82B101 82Pr03 82Sa19 82Sc17 82B101 82AI18

82Sa19 82Se17 82All8

82Sa19 82A118 81Ra21 82A118 82Al18 82Blt0

82B110 82Sa19 82Se17 82Sa19 82A118

82Sa19 81Pa22 82Sa19 81Pa22 82Sa19 82Sal9 78An29 78An29 78An28 78An28 82KI06 78An28 78An28 78AnZ8 82Sa19 78An28 82Ar04 82Sat9 78An28 78Anti8 82Sa19 82Sa19

82Sa19 82Sa19

81Ra23 82Ch24 82Sai9

81Ba54 82AIl8 82AII8 82Sa19

82Sc17 81Ba54 82Se17 8~SaI9 82Sa19 82Be19 82WetO 82Se17

82Sa19 8-2T;1'7 82Ta17 82TaI7 82We10

82A118 82A118 82Sa19 82Sc17 82Sa19 82Ha02

82Ha02

(p,p') 6Li(p,p'),E=136 MeV; m e a s u r e d at(0). SLi(p,p'),E=24.4 MeV; m e a s u r e d at(Ep'),at(0). VLi(p,p'7),E~2.4 MeV; m e a s u r e d E'/,I7. 7Li(p,p'),E=24.4 MeV; m e a s u r e d a(Ep'),at(0). ~C(polarized p,p'),E=22-29 MeV; m e a s u r e d P(0), lZC(polarized p,p'),E=150 MeV; m e a s u r e d ~C(p,p'T),E~41.1 MeV; m e a s u r e d at(Ep',Op',~T=90°), tZC(p,p'),E:t2 MeV; m e a s u r e d (e+)(e-)-coin. ~2C(p,p'7),E~24-44 MeV; m e a s u r e d E7,17,7(0). tZC(p,p'),E=0.8 GeV; m e a s u r e d at(O).

~C(p,p'7),E~591,696,796 keV; m e a s u r e d p T - e o i n , tZC(p,pT),E=l.594 .... MeV; m e a s u r e d at(O), ~C(]p,p'7),E~1700-1835 keV; m e a s u r e d ~(OT,ET,0p'), ~ZC(p,p'),E=l.7 .... MeV; m e a s u r e d at(Ep'), l~C(p,p'),E=135 MeV; m e a s u r e d at(0). ~aC(p,p'),E=:[35 MeV; m e a s u r e d at(0). tdN(polarized p,p'),E=21 MeV; m e a s u r e d at(O),veetor ~aN(p,p'),E=0.8 OeV; m e a s u r e d at(0),at(Ep'). ~O(p,p'7),E~23.7,44.6 MeV; m e a s u r e d 7(0),or(total) ~SO(p,p'7),E~4.4-4.62 .... MeV; m e a s u r e d yields, ~aO(polarized p,p'),E=800 MeV; m e a s u r e d at(0),

5SCr(p,p'),E=5,20-6.05 MeV; m e a s u r e d a(E). 5aCr(p,p'),E=0.88-2.4 MeV; m e a s u r e d o'(E). 54Cr(p,p'),E=5.20-6.05 MeV; m e a s u r e d or(E). 80Ha55 54Fe(p,p'),E= 5.20- 6.05 MeV; m e a s u r e d a(E). 82Pe06 5SFe(p,p'),E=5.20- 8.05 MeV; m e a s u r e d cr(E). 81Ful2 5r Fe(p,p'),E=5.20-6.05 Me'V; m e a s u r e d (~(E). 82Ca08 5aFe(p,p'),E=5.20-6.05 MeV; m e a s u r e d G(E). 82De02 5SNi(p,p'),E=27 Me'g; m e a s u r e d G(0). 82En01 5SNi(p,p'),E=200 MeV; m e a s u r e d a(O). 82Gu03 eaNi(p,p'),E=200 MeV; m e a s u r e d a(0). 82Ba26 6eNi(p,p'),E=200 MeV; m e a s u r e d a(0). 82Le03 eZNi(p,p'),E=7.08 MeV; m e a s u r e d I(ee),(ce)(t). 82Li12 eCZn(p,p'T),E=3.24-3.£6 MeV; m e a s u r e d E7,17,7(0). 82Ta09 6aZn(p,p'),E=200 MeV; m e a s u r e d at(0). 82Tall 7ZGe(p,p'e),E=3-4.34 MeV; m e a s u r e d p'e-coin, 82Co08 74Ge(p,p'),E=22 MeV; m e a s u r e d a(E,O). 82Ri05 eSY(polarized p,p'),E=Zt.l MeV; m e a s u r e d c~(E,e), 82Ao05 S°Zr(polarized p,p'),E=800 MeV; m e a s u r e d at(O), 82B108 90Zr(p,p'),E=200 MeV; m e a s u r e d at(0). 81Nal4 9°Zr(p,p'),E=200 MeV; m e a s u r e d at(0). 82Dill 9°Zr(p,p'),E=800 MeV; m e a s u r e d ~(0). 82G108 continued 8tHe21

82Pe06

iii

78An28 81Ga38 78An28 78An28 78An28 78An28 78An28

82Bl16

~'2Di_9_~. 82Dj04 82D~04 82Ka22 82Raft 82Dj04 82~e03

82Ta16 82Me02 81Ba54 82Cr02 82Dj04 82Ga02

REACTION

(p,p') Na(p,p'),E=6.~7 .... MeV; m e a s u r e d a(O). ZSNa(p,p'v),E=500-17D0 keV; m e a s u r e d a(E). Z~Mg(p,p'),E=5.0-6.0 MeV; m e a s u r e d s p i n - f l i p Z4Mg(p,p'),E=0.8 GeV; m e a s u r e d a(O). UaMg(p,p'v),E=14.5-41.1 MeV; m e a s u r e d e4Mg(polarized p,p'),E=65 MeV; m e a s u r e d a(0),A(0). e°Mg(p,p'),E=0.8 GeV; m e a s u r e d G(0). Si(p,p'),E=ll5 MeV; m e a s u r e d or(0). ~aSi(p,p'),E=5.6-6.O MeV; m e a s u r e d s p i n - f l i p ZaSi(p,p'v),E=35.3,40.9 MeV; m e a s u r e d ZSSi(polarized p,p'),E=65 MeV; m e a s u r e d a(0),A(0). eaSi(p,p'),E=ll5 MeV; m e a s u r e d G(0). ZOSi(polarized p,p'),E=650,800 MeV; m e a s u r e d or(0). aeS(p,p'v),E=15.5-40.9 MeV; m e a s u r e d 3~S(p,p'),E=7.5 MeV; m e a s u r e d p v - c o i n , p v ( 0 ) , E v , I % a*S(polarized p,p'),E=650 MeV; m e a s u r e d G(0). a°Ca(p olarized p,p'),E=497 MeV; m e a s u r e d p r o t o n ~°Ca(p,p'),E=0.8 GeV; m e a s u r e d (y(Ep'),ct(0),A(0). *°Ca(polarized p,p'),E=0.8 GeV; m e a s u r e d a(Ep'), ~°Ca(polarized p,p'),E=65 MeV; m e a s u r e d cr(0),A(O). ~°Ca(p,p'),E=5.9-6.5 MeV; m e a s u r e d G(Ep',E),ct(O), ~°Ca(polarized p,p'),E=5.9-6.5 MeV; m e a s u r e d 4aCe(polarized p,p'),E=650 MeV; m e a s u r e d a(0). ~aCa(p,p'v),E=0.63-3.01 MeV; m e a s u r e d v - r a y , 4~Ca(p,p'v),E=0.775-5.05 MeV; m e a s u r e d " / - r a y , ~Ca(p,p'v),E=2.315-2.9903 MeV; m e a s u r e d a(0p'), ~aCa(p,p'),E=44.4 MeV; m e a s u r e d a(O),proton ~Ca(p,p'),E=65 MeV; m e a s u r e d a(O). ~SCa(polarized p,p'),E=159.8 MeV; m e a s u r e d cr(Ep'), 4~Sc(p,p'),E=l.2-2.5 MeV; m e a s u r e d G(E). S~V(p,p'),E=6.05 MeV; m e a s u r e d a(O). aZV(p,p'),E=200 MeV; m e a s u r e d or(0). ~SCr(p,p'),E=5.20-6.05 MeV; m e a s u r e d of(E). ~Cr(p,p'),E=5.20-~.05 MeV; m e a s u r e d a(E). ~eCr(p,p'T),E=4.14-4.2 MeY; m e a s u r e d E"/,Iv,v(O),

INDEX

continued

82Va16 81Tr08 78Vi04 83Bl01 82De03 82Ho13 8~BI01 8~Ka0¢ 78Vi04 83De02 82Ho13 82Ka04 82Be3~ 82De0~ 82Go13 82B e 3~ 82Aa04 82B]10 82B 110 82Ho13 82Wal~ 82Wa l ~

~°Zr(polarized p,p'),E=500 MeV; m e a s u r e d a n a l y z i n g SZZr(polarized p,p'),E=800 MeV; m e a s u r e d or(e), ~eZr(p,p'),E=7.08 MeV; m e a s u r e d I(ee),Ev,Iv,TI/e g2Zr(p,p'),E=200 MeV; m e a s u r e d a(0). a2Zr(p,p'),E=200 MeV; m e a s u r e d or(0). °2Zr(p,p'),E=7.08 MeV; m e a s u r e d l(ce),(ce)(t). gZZr(p,p'),E=ll5 MeV; m e a s u r e d a(Ep'),G(0). a4Zr(p,p'),E=8.11 MeV; m e a s u r e d I(ee),E%l%%/a a4Zr(p,p'),E=200 MeV; m e a s u r e d G(0). a4Zr(p,p%E=200 MeV; m e a s u r e d a(O). aaZr(p,p'),E=200 MeV; m e a s u r e d tr(0). aeZr(p,p'),E=200 MeV; m e a s u r e d ct(0). a2Mo(p,p'),E=200 MeV; m e a s u r e d a(O). a4Mo(p,p'),E=200 MeV; m e a s u r e d G(0). gaMo(p,p'),E=200 MeV; m e a s u r e d G(0). aaMo(p,p'),E=200 MeV; m e a s u r e d a(0), l°°Mo(p,p'),E=200 MeV; m e a s u r e d a(0). n a S n ( p o l a r i z e d p,p'),E=800 MeV; m e a s u r e d a(0,1~p), 12°Sn(p,p'),E=~00 MeV; m e a s u r e d a(0). ~a°Sn(p,p'),E=800 MeV; m e a s u r e d ~r(0). ~Z4Sn(p,p'),E=~00 MeV; m e a s u r e d a(O). i4SCe(p,p'),E=E00 MeV; m e a s u r e d cr(0). 144Sm(p,p'),E=800 MeV; m e a s u r e d G(O). 144Sm(p,p'),E=l.04 GeV; m e a s u r e d G(0). 15aSm(p,p'),E=l.04 GeV; m e a s u r e d G(0). 152Sm(p,p'),E=l.04 GeV; m e a s u r e d or(0). Za6Pb(p,p'),E=35 MeV; m e a s u r e d (7(0). Z°vPb(p,p'),E=95 MeV; m e a s u r e d o'(Ep',O). Z°aPb(polarized p,p'),E=497 MeV; m e a s u r e d p r o t o n 2°aPb(p,p'),E=201 MeV; m e a s u r e d a(0). 2°apb(p,p'),E=800 MeV; m e a s u r e d o'(0). Z°sPb(polarized p,p'),E=400 MeV; m e a s u r e d eaaTh(p,p'),B=26 MeV; m e a s u r e d a(0). 2aaU(p,p'),E=26 MeV; m e a s u r e d G(0).

82Be3~ 8~Mi06 82Mi 06 82Sh12 82Be14 82FuOR

82Re07 81An23 78An29 82Dj04 78An28 78Ao28 82K106

82Mo02 81Ba54 81Ju03 82Cr02 82Dj04 82Ka22 82Ka~7 81Ju03 82Cr02 82D~04 82Cr02 82Dj04 82Dj04 82DJ04 82Dj04 82Dj04 82Dj04 82Mo02 82Dj04 82Ga02 82Dj04 82Dj04 8 2 G a0 2 82Ta17 82Ta17 82Ta17 81Fi07 82Ba38 82Aa04 82DjO1 82Ga02 82Mo02

82Ha02 82Ha02

(p,2n) aaY(p,2n),E=0.059-24 GeV; m e a s u r e d p r o d u c t i o n (7 of ~°Zr(p,~n),E=18-26 MeV; m e a s u r e d EV,Iv(E),vV-coin. ~7Sn(p,2nv),E=15-25 MeV; m e a s u r e d EV,Iv,vv-eoin,

82Re13 82Di09 82Va07

laaBa(p,2n),E=17,1-20.3 MeV; m e a s u r e d EV,Iv(E), aaaTh(p,2n),E=8-22 MeV; m e a s u r e d a ( f i s s i o n ) ,

82Ko05 82Ku07

(p,np) e l l ( p o l a r i z e d p,pn),E=65 MeV; m e a s u r e d 4°Ca(p,np),E=149.5 MeV; m e a s u r e d cr(0p,0n,Ep), 4aCa(p,np),E=149.5 MeV; m e a s u r e d a(Op,On,Ep), aeKr(p,np),E=600 MeV; m e a s u r e d p r o d u c t i o n or.

82Sh07 82Wa17 82Wa17 82Ku13

8aKr(p,np),E=600 MeV; measured production ~. a4Kr(p,np),E=600 MeV; m e a s u r e d p r o d u c t i o n a. eSKr(p,np),E=600 MeY; m e a s u r e d p r o d u c t i o n G. laaCs(p,np),E=36.4-67 MeV; m e a s u r e d r e s i d u a l s

82Ku13 82Ku13 82Ku13 82La15

UaSn(p,d),E=R0 MeV; m e a s u r e d o'(Ep),G(O). nVSn(p,d),E=20 MeV; m e a s u r e d q(Ep),G(0). ~JaSn(p,d),E=~0 MeV; m e a s u r e d cr(Ep),cr(0). naSn(p,d),E=;~0 MeV; m e a s u r e d G(Ep),G(0). le°Sn(p,d),E=26.3 MeV; m e a s u r e d q(E(d),0). lZaSn(p,d),E=20 MeV; m e a s u r e d a(Ep),a(0). lZeSn(p,d),E=20 MeV; m e a s u r e d a(Ep),G(0). JZ4Sn(p,d),E=20 MeV; m e a s u r e d q(Ep),cr(0). 12eTe(p,d),E=42 MeV; m e a s u r e d a(0). le4Te(p,d),E=42 MeV; m e a s u r e d a(0). la°Te(p,d),E=42 MeV; m e a s u r e d a(0).

82F102 82Fl02 82FLO2 8~F102 8~Di04 82F102 8~F102 8~Fl02 8~Ga18 8~Gal8 82Ga18

(p,d) ~H(polarized p,d),E=10 MeV; m e a s u r e d v e c t o r to ~He(polarized p,d),E=200,400 MeV; m e a s u r e d 4He(polarized p,d),E=32,50 MeV; m e a s u r e d a n a l y z i n g aBe(p,d),E=14.3,26.2 MeV; m e a s u r e d G(0,Ed). UB(polarized p,d),E=ll.34-11.94 MeV; m e a s u r e d ~aC(polarized p,d),E=13.79-14.39 MeV; m e a s u r e d ~ N ( p o l a r i z e d p,d),E=21 MeV; m e a s u r e d o'(0),vector l°~Ru(p,d),E=29 MeV; m e a s u r e d (~(0). H~Sn(p,d),E=20 MeV; m e a s u r e d a(Ep),cr(O). U~Sn(p,d),E=20 MeV; m e a s u r e d cr(Ep),a(0). ~ S n ( p , d ) , E ~ 2 0 MeV; m e a s u r e d a(Ep),a(0).

82Sp03 82Ka21 82Sa05 81Be53 82Bu03 82Bu03 82Ao05 82Be19 82F102 82F102 82F102

(p,2p) ~H(polarized p,2p),E=65 MeV; m e a s u r e d ~He(polarized p,ap),E=250,500 MeV; m e a s u r e d ~He(p,ap),E=250,350,550 MeV; m e a s u r e d

82Sh07 82Ma19 82Va01

°Li(p,2p),E=0.8 GeV; measured pp-coin,a(0p0~) vs SLi(p,2p),E=50-100 MeV; measured o(el,O2,E1). aBe(p,2p),E=0.8 GeV; measured pp-coin,cr(Ot,0z) vs

112

81Fr24 81Pa25 81Fr24

REACTION

INDEX

(p,3n) ~SSCs(p,3n),E=36.4-67 MeV; m e a s u r e d r e s i d u a l s ~7sYb(p,3n),E n o t g i v e n ; m e a s u r e d ET,IT.

82La15 81Do14

232Th(p,3n),E=8-22 MeV; m e a s u r e d

or(fission),

82Ku07

(p,2np) s;"Kr(p,Snp),E=600 MeV; m e a s u r e d p r o d u c t i o n a, 83Kr(p,gnp),E=600 MeV; m e a s u r e d p r o d u c t i o n ~.

82Ku13 BZKul3

S4Kr(p,2np),E=600 MeV; m e a s u r e d p r o d u c t i o n a. SSKr(p,2np),E=6OO MeV; m e a s u r e d p r o d u c t i o n ~.

82Ku13 82Ku13

l°°Mo(p,t),E=52 MeV; m e a s u r e d l ° ° R u ( p o l a r i z e d p,t),E=22 MeV; l ° 2 R u ( p o l a r i z e d p,t),E=22 MeV; l ° 4 R u ( p o l a r i z e d p,t),E=22 MeV; l ° a P d ( p o l a r i z e d p,t),E=22 MeV; l ° s P d ( p o l a r i z e d p,t),E=22 MeV; l ° s p d ( p o l a r i z e d p,t),E=22 Me'Y; l l ° P d ( p o l a r i z e d p,t),E=22 MeV; l°sCd(p,t),E=42 MeV; m e a s u r e d 11°Cd(p,t),E=42 MeV; m e a s u r e d 11~Cd(p,t),E=42 MeV; m e a s u r e d l14Cd(p,t),E=43 MeV; m e a s u r e d lisCd(p,t),E=42 MeV; m e a s u r e d lS4Te(p,t),E=52 MeV; m e a s u r e d laSBa(polarized p,t),E=22 MeV; 13SBa(p,t),E=52 MeV; m e a s u r e d 14ZCe(p,t),E=52 MeV; m e a s u r e d 140Nd(p,t),E=52 MeV; m e a s u r e d 1S°Sm(p,t),E=52 MeV; m e a s u r e d lSlTa(p,t),E=19 MeV; m e a s u r e d lSSHg(p,t),E=25 MeV; m e a s u r e d 23ZTh(p,t),E=52 MeV; m e a s u r e d

82Na06 82Ao01 82Ao01 82Ao01 82Ao01 82Ao01 82Ao01 82Ao01 82Cr01 83Cr01 82Cr01 82Cr01 82Cr01 B2Na06 83Ao01 82Na06 82NaO6 82Na06 82Na06 82Wa10 82Be21 82Na06

(p,t) 13C(p,t),E=65 MeV; m e a s u r e d a(0),A(0). SSZn(p,t),E=52 MeV; m e a s u r e d a(Et,0). ~aGe(p,t),E=13 MeV; m e a s u r e d at0). VeGe(p,t),E=13 MeV; m e a s u r e d cr(E(t),0). 74Ge(p,t),E=13 MeV; m e a s u r e d at0). 7'~Ge(p,t),E=13 MeV; m e a s u r e d atE(t),0). 7e~Ge(p,t),E=13 MeV; m e a s u r e d at0). 7~Ge(p,t),E=13 MeV; m e a s u r e d cr(E(t),~). 7t~Kr(p,t),E=51.9 MeV; m e a s u r e d at0). e°Kr(p,t),E=51.9 MeV; m e a s u r e d at0). s~:Kr(p,t),E=51.9 MeV; m e a s u r e d at0). aCKr(p,t),E=5t.9 MeV; m e a s u r e d at0). 9%r(p,t),E=52 MeV; m e a s u r e d a(Et,0). a~Zr(polarized p,t),E=22 MeV; m e a s u r e d 9ZZr(p,t),E=52 MeV; m e a s u r e d a(Et,0). 9~Zr(p,t),E=52 MeV; m e a s u r e d a(Et,0). SaMo(polarized p,t),E=22 MeV; m e a s u r e d 9aMo(p,t),E=52 MeV; m e a s u r e d a(Et,0). 9°Ms(polarized p,t),E=22 MeV; m e a s u r e d 9SMo(p,t),E=52 MeV; m e a s u r e d cr(Et,0). 9eMo(polarized p,t),E=E2 MeV; m e a s u r e d ~eMo(p,t),E=52 MeV; m e a s u r e d a(Et,0).

a(0),A(0).

a(0),A(0).

o'(O),A(O). q(0),A(0).

82Ka01 82Na06 82Be13 82Be45 82Be13 82Be45 82Be13 82Be45 82Ma18 82Ma18 82Ma18 82Ma18 82Na06 82Ao01 82Na06 82Na06 82AoOI 82N a 06 82AoOl 82N a 06 82A s 01 B2Na06

q(Et,0). measured measured measured measured measured measured measured a(Et),Q.

a(O),A(O). a(0),A(O). a(0),A(0). a(0),A(0). a(0),A(0). a(0),A(0).

a(O),A(O).

o(Et). a(Et).

~(Et). a(Et).

a(Et,o). m e a s u r e d u(0),A(0).

a(Et,o). a(Et,0). a(Et,0). a(Et,0). (~(0),a(Et). cr(Et),Q. ct(Et,e).

(p,pd) 7Li(p,pd),E=670 MeV; m e a s u r e d a ( E ( m i s s i n g ) , E p ) . leC(p,pd),E=670 MeV; m e a s u r e d a ( E ( m i s s i n g ) , E p ) .

81Erl0 81Erl0

lSO(p,pd),E=101.3 MeV; m e a s u r e d a(Ei,Ez,61,02).

82Sa24

(p,3He) 13C(p,SHe),E=65

MeV; m e a s u r e d cr(O),A(O).

B2Ka01

A s ( p o l a r i z e d p,SHe),E=237,445 MeV; m e a s u r e d

82Gr01

(p,anp) 8ZKr(p,3np),E=600 MeV; m e a s u r e d p r o d u c t i o n a. aSKr(p,3np),E=600 MeV; m e a s u r e d p r o d u c t i o n a. S4Kr(p,3np),E=600 MeV; m e a s u r e d p r o d u c t i o n a.

82Ku13 82Ku13 82Ku13

a°Kr(p,3np),E=600 MeV; m e a s u r e d p r o d u c t i o n a. eSY(p,3np),E=0.059-24 GeV; m e a s u r e d p r o d u c t i o n a

82Ku13 82Re13

(p,pt) 160(p,pt),E=101.3 MeV; m e a s u r e d a(Ej,Ea,OI,O~).

82Sa24

(p,2d) SLi(p,2d),E=670 MeV; m e a s u r e d (7(0j,0z)

vs m i s s i n g

82Er06

7Li(p,2d),E=670 MeV; m e a s u r e d cr(01,0a) vs m i s s i n g

82Er06

(p,~) l°B:(p,aT),E=2.4 MeV; m e a s u r e d ET,IT. 12C(polarized p,a),E=72 MeV; m e a s u r e d at0), l~N(p,a),E=78-810 keV; m e a s u r e d atE,0). 180(p,aT),E=4.4-4.62 .... MeV; m e a s u r e d y i e l d s , a t E ) lSF(p,a),E=7.4 MeV; m e a s u r e d E-/,l~l,a~,-eoin. Na(p,a),E=6.27,6.37,6.52 MeV; m e a s u r e d at0). 23Na(p,a~),E=500-1700 keV; m e a s u r e d atE). ZaNa(p,a),E=500-1700 keV; m e a s u r e d atE). 27Al(p,a),E=632,... keV; measu}'ed Ea. 27AI(p,~),E=1365 .... keV; m e a s u r e d ey(Oa).

80H a 55 41K(p,a),E=0.68-2.48 MeV; m e a s u r e d 7 , n e u t r o n 8IDol3 46Ti(polarized p,a),E=79.2 MeV; m e a s u r e d a(0),A(0) 82Re06 4STi(p,a),E=40.35 MeV; m e a s u r e d ry(0). 82Dill 48Ti(polarized p,a),E=79.2 MeV; m e a s u r e d a(0),A(0) 82Ve04 4aTi(p,a),E=40.35 MeV; m e a s u r e d ate). 82Va16 50Ti(p,a),E=40.35 MeV; m e a s u r e d at0). 81Tr08 SSNi(polarized p,a),E=72 MeV; m e a s u r e d o'(0), 81Tr08 74Ge(p,a),E=36.25 MeV; m e a s u r e d a(Ea),a(0). 81Erl2 A s ( p o l a r i z e d p,a),E=237,445 MeV; m e a s u r e d 81Vo09 lSeEr(p,a),E=t7 MeV; m e a s u r e d a(Ea),a(0). continued

113

82Se02 81Bo37 82Ab03 81Bo37 82Ab03 82Ab03 8IDol3 82Pe07 82Gr01 82Ha17

REACTION

(p,a)

3°Si(p,a),E=4.9-6.08 MeV; m e a s u r e d o'(E,E(a),O).

INDEX

continued

ze4Er(p,a),E=17 MeV; measured ~(Ea),a(0).

82C h09

82Ha17

(p,n3p) S°y(p,n3p),E=O.059-24 GeV; m e a s u r e d p r o d u c t i o n a

82Re13

(p,4p) 89y(p,4p),E=0.059-24 GeV; m e a s u r e d

p r o d u c t i o n G of

82Re13

(p,5n)

lSSCs(p,5n),E=36.4-67 MeV; m e a s u r e d r e s i d u a l s

82La15

(p,3n2p) SgY(p,3nEp),E=0.059-24 GeV; measured p r o d u c t i o n a

82Re13

(p,n4p) agy(p,n4p),E=O.059-24 GeV; m e a s u r e d

production a

82Re13

(p,6n) 133Cs(p,6n),E=36.4-67 MeV; m e a s u r e d

residuals

82La15

(p,5np)

e2Kr(p,5np),E=600 MeV; m e a s u r e d p r o d u c t i o n G. e3Kr(p,5np),E=600 MeV; m e a s u r e d p r o d u c t i o n a.

82Ku13 82Ku13

S4Kr(p,5np),E=600 MeV; measured 88Kr(p,5np),E=600 MeV; m e a s u r e d

(p,3n3p) egy(p,3n3p),E=0.059-24 GeV; m e a s u r e d

production a

83Re13

(p,da) 9Be(p,da),E=30 MeV; m e a s u r e d ¢r(0d,Ed,0a).

82Loll

(p,2n4p) 8eY(p,2n4p),E=0.059-24 GeV; m e a s u r e d p r o d u c t i o n G

82Re13

(p,4n3p) egy(p,4n3p),E=0.059-24 GeV; m e a s u r e d p r o d u c t i o n a

82Re13

(p,3n4p) 89y(p,3n4p),E=O.059-24 GeV; m e a s u r e d p r o d u c t i o n a

82Re13 (p,4n4p)

egY(p,4n4p),E=0.059-24 GeV; m e a s u r e d

production

82Re13 (p,5n4p)

egY(p,Sn4p),E=0.059-24 GeV; m e a s u r e d

production G

82Re13

114

production a. p r o d u c t i o n a.

82Ku13 82Ku13

REACTION

INDEX

(p,6ndp) 8aY(p,6n4p),E=0.059-24

GeV; m e a s u r e d

82Re13

production

(p,8ndp) aSY(p,8n4p),E=0.059-24

GeV; m e a s u r e d

82Re13

production

(p,xnyp)

aaZTh(p,xnyp),E=6.8-20.2 MeV; m e a s u r e d

81Ce06

(7(E) f o r

(p,F) 82Shi0 82Sh10 82Sh10 82Sh10 82Pall 82Pall

A g ( p , F ) , E = 1 5 5 , 2 0 0 MeV; m e a s u r e d a(fission), I n ( p , F ) , E = 1 5 5 , 2 0 0 MeV; m e a s u r e d (7(fission), S n ( p , F ) , E = 1 5 5 , 2 0 0 MeV; m e a s u r e d a(fission), S m ( p , F ) , E = 1 5 5 , 2 0 0 MeV; m e a s u r e d a(fissien), 1 a q r ( p , F ) , E = 6 8 , 8 5 , 1 0 0 MeV; m e a s u r e d independent 193Ir(p,F),E=68,85,100 MeV; m e a s u r e d independent

Z°aBi(p,F),E=60 MeV; m e a s u r e d fission fragment 23ZTh(p,F),E=15 MeV; m e a s u r e d o r ( f r a g m e n t 0). 2 a Z T h ( p , F ) , E = 8 - 2 2 MeV; m e a s u r e d or(fission), Z S e T h ( p , F ) , E = 4 - 1 1 MeV; m e a s u r e d a ( f i s s i o n ) v s E, 232Th(p,F),E=140 .... MeV; m e a s u r e d

82No10 82KuOl 82Ku07 82Ku12 82Sa08

L a ( p , X ) , E = 4 0 0 GeV; m e a s u r e d production (7(0) f o r L u ( p , X ) , E = 4 0 0 GeV; m e a s u r e d production a(O) f o r Ta(p,X),E=0.125-4 MeV/nucleon; measured L-shell T a ( p , X ) , E = 0 . 6 6 , 8 GeV; m e a s u r e d y i e l d s f o r 7971, Ta(p,X},E=B G e ¥ ; m e a s u r e d Rb,Cs i s o t o p e y i e l d s . T a ( p , X ) , E = 5 GeV; m e a s u r e d Ea,Tl/2 of spaliation, Au(p,X),E=0.125-4 MeV/nucleon; measured L-shell Au(p,X),E=l,2.5,24 GeV; m e a s u r e d p r o d u c t i o n (y f o r A u ( p , X ) , E = 5 GeV; m e a s u r e d Ea,%/2 of spallation, A u ( p , X ) , E = 4 0 0 GeV; m e a s u r e d production ~(0) f o r P b ( p , X ) , E = 6 6 0 MeV; m e a s u r e d cumulative cr f o r Bi(p,X),E=660 MeV; m e a s u r e d cumulative (7 f o r Th(p,X),E=I,g.5,g4 GeV; m e a s u r e d p r o d u c t i o n a f o r T h ( p , X ) , E = 5 GeV; m e a s u r e d Ea,TI/2 of s p a l l a t i o n , a S 2 T h ( p , X ) , E = 0 . 1 5 - 2 4 GeV; m e a s u r e d production a(E) U ( p , X ) , E = 6 0 0 MeV; m e a s u r e d absolute,comparative U(p,X),E=5 GeV; m e a s u r e d Ea,Tl/e of spallation,

828t0I 828t01 81Ba56 82Av01 82Av03 82Bo04 81Ba56 81Sa34 82Bo04 82St01 80Ad08 80ADO8 81Sa34 82Bo04 82Sa01 81BjO4 82Bo04

C(polarized

82Rag0

(p,X) ~"dMg(p,X),E=400 MeV; m e a s u r e d pT-coin,a(0p),proton aI7AI(p,X),E=16-70 MeV; m e a s u r e d production a(E) e:TAl(p,X),E=600 MeV; m e a s u r e d production (7 f o r ~:VAI(p,X),E=400 MeV; m e a s u r e d p y - c o i n , ( 7 ( 0 p ) , p r o t o n ~:aSi(p,X),E=400 MeV; m e a s u r e d pT-eoin,(7(Op),proton e'aNi(p,X),E=400 MeV; m e a s u r e d pT-eoin,o'(Op),proton Cu(p,X),E a t 225 G e V / c ; m e a s u r e d residuals yields, S a C u ( p , X ) , E = l S - 7 0 MeV; m e a s u r e d production a(E) ~SCu(p,X),E=16-70 Me'q; m e a s u r e d production (7(E) ~SAs(p,X),E=593,540 MeV; m e a s u r e d production (7 for Br(p,X),E=800 MeV; m e a s u r e d production or, Br(p,X),E=593,540 MeV; m e a s u r e d production a for R b ( p , X ) , E = 8 0 0 MeV; m e a s u r e d production a, R b ( p , X ) , E = 5 9 3 , 5 4 0 MeV; m e a s u r e d production (7 f o r 8 9 Y ( p , X ) , E = 5 9 3 , 5 4 0 MeV; m e a s u r e d production (7 f o r Z r ( p , X ) , E = 0 . 0 5 9 - 2 4 GeV; m e a s u r e d production (r o f Ag(p,X),E=O.125-4 M e V / n u c l e o n ; m e a s u r e d L - s h e l l A g ( p , X ) , E = 4 0 0 GeV; m e a s u r e d production cr(0) f o r

82La13 82Gr09 82Gr19 82La13 8ZLaI3 82La13 828a18 82Gr09 82Gr09 82Gr19 8gGr06 82Gr19 82Gr06 82Gr19 82Gr19 82Re13 81Ba56 82St01

(p,pX) Be(polarized

p,pX),E=780

MeV; m e a s u r e d

analyzing

82Ra20

p,pX),E=100-750

MeV; m e a s u r e d

(p,aHeX) l e e ( p o l a r i z e d p , a H e X ) , E = 7 2 MeV; m e a s u r e d a(O,E), 2 7 A l ( p o l a r i z e d p , a H e X ) , E = 7 2 MeV; m e a s u r e d a(0,E), 5 a N i ( p o l a r i z e d p,aHeX),E=72 MeV; m e a s u r e d a(0,E),

82Legl 82Le21 8gLe21

9 ° Z r ( p o l a r i z e d p , a H e x ) , g = 7 2 MeV; m e a s u r e d a ° a B i ( p o l a r i z e d p,SHeX),E=72 MeV; m e a s u r e d

(7(0,E), ~(0,E),

82Le21 82Le21

cr(0,E), analyzing (7(0,E), analyzing (7(8,E),

82Legl 81Ko33 82Le21 8tKo33 82Le21

(p,aX) lZC(polarized p,aX),E=72 leC(polarized p,aX),E=72 aTAl(pelarized p,aX),E=72 aTAl(polarized p,aX),E=72 S S N i ( p o l a r i z e d p,c~X),E=T2

MeV; m e a s u r e d analyzing MeV; m e a s u r e d (7(O,E), MeV; m e a s u r e d analyzing MeV; m e a s u r e d (7(0,E), MeV; m e a s u r e d analyzing

5 8 N i ( p o l a r i z e d p , a X ) , E = 7 2 MeV; m e a s u r e d a ° Z r ( p o l a r i z e d p , ~ X ) , E = 7 2 MeV; m e a s u r e d 9 ° Z r ( p o l a r i z e d p,(~X),E~72 MeV; m e a s u r e d 2 ° 9 B i ( p o l a r i z e d p , a X ) , E = 7 2 MeV; m e a s u r e d e ° S B i ( p o l a r i z e d p , a X ) , E = 7 2 MeV; m e a s u r e d

81Ko33 82Le21 8iKo33 83Le21 81Ko33

(d,7) 1 5 4 8 m ( d , 7 ) , E = 7 . 5 - 1 7 . 5 MeV; m e a s u r e d (7(capture) Z ° S B i ( d , 7 ) , E = 8 - 1 1 . 5 MeV; m e a s u r e d a(E),

vs

82Gi06 82Ze03

2 3 8 U ( d , 7 ) , E = 7 . 5 - 1 7 . 5 MeV; m e a s u r e d

(7(capture)

vs E

l°B(d,~r-),E=300,600 MeV; m e a s u r e d

(7(0) vs p i o n

82Gi06

(d,rr-) SLi(d,Tr-),E=300,600 MeV; m e a s u r e d SBe(d,Tr-),E=300,600 MeV; m e a s u r e d

(7(0) v s p i o n (7(0) vs p i o n

82As01 82As01

115

82As01

REACTION

INDEX

(d,n) UH(d,n),E=3-6 MeV; m e a s u r e d a(O=O°) vs E. e l l ( p o l a r i z e d d,n),E=8 MeV; m e a s u r e d P(0n). °Li(d,n3'),E=48,170 keV; m e a s u r e d t h i c k t a r g e t ~Li(d,n),E=13.~ MeV; m e a s u r e d (r(En). 7Li(d,n),E=400,680,1020 keV; m e a s u r e d a(En). aBe(d,n'~),E=48,170 keV; m e a s u r e d t h i c k t a r g e t

81Pa26 81To15 82Ce02 80Ma48 80Yall 82Ce02

B(d,n),E=8 MeV; m e a s u r e d a(En). laB(d,n-y),E=48,170 keY; m e a s u r e d t h i c k t a r g e t 12C(d,n),E=7-10 MeV; m e a s u r e d a(0=0e,E). 2SSi(d,n),B=ll MeV; measured G(0p,0n,En), 74Ge(d,n),E=7 MeV; m e a s u r e d 5'T-coin.

82Fi08 82Ce02 81Sh22 80Jal8 80Joll

~SSi(d,p),E=ll MeV; m e a s u r e d a(Op,0n,En), 2SSi(d,p),E=l-2.5 MeV; m e a s u r e d a(0,Ep,E). V4Ge(d,ps'),E=6 MeV; m e a s u r e d E%I3,,Tt/2,p-y-coin. 7aKr(polarized d,p),E=ll MeV; m e a s u r e d a(0),A(0). aSMo(polarized d,p),E=16 MeV; m e a s u r e d a(O),a(Ep), ~°eRu(d,p),E=45 MeV; m e a s u r e d a(0). 14SNd(d,p),E=12.1 MeV; m e a s u r e d a(Ep),a(Et),a(0). tSaw(d,p),E=7-15.7 MeV; m e a s u r e d a(E).

80Jal8 80Li21 82is07 82Bu01 82Ha41 82Be19 82Ja09 81Ta26

(d,p) e l l ( p o l a r i z e d d,p),E=l-13 MeV; SHe(polarized d,p),E=14.6-39.9 ~Li(d,p),E=9.05 MeV; m e a s u r e d 7Li(d,p),E=9.05 MeV; m e a s u r e d

m e a s u r e d a(O),vector MeV; m e a s u r e d a(0).

a(O). ~Li(d,p),E=0.684-0.896 MeV; measured

~r(~d,O).

~Li(d,p),E=0.6-1.2 MeV; m e a s u r e d d - d e l a y e d Ea,I(~. aBe(polarized d,p),E=l.4-E.2 MeV; m e a s u r e d a(0), t~C(d,p),E=9 MeV; m e a s u r e d a(0).

81Gr23 81R o13 81YuO1 80Y e 62 82E]03 82Fi03 80De45 79Wa24

(d,2n) 7eSe(d,2n),E=13.5 MeV; m e a s u r e d ET,I%7"~-eoin, ~eaSb(d,2n),E=12.5 MeV; m e a s u r e d ~/(t),'~(0,H,t). ~aeW(d,Sn),E=7-15.7 MeV; m e a s u r e d a(E).

82Doll 811o05 81Ta26

tSsW(d,Sn),E=7-15.7 MeV; m e a s u r e d or(E). la4W(d,2n),E=7-15,7 MeV; m e a s u r e d a(E). lssw(d,Sn),E=7-15.7 MeV; m e a s u r e d a(E).

81Ta26 81Ta26 81Ta26

(d,np) SHe(polarized d,np),E=lS,21 MeV; m e a s u r e d iTu(0), aa°U(d,np),E=26 MeV; m e a s u r e d l(ce),

821s06 82Go02

ZasU(d,np),E=20 MeV; m e a s u r e d

l(ce),

82Go02

(d,d) I H ( p o l a r i z e d d,d),E=20 MeV; m e a s u r e d v e c t o r , t e n s o r SHe(polarized d,d),B=14.6-39.9 MeV; m e a s u r e d 7Li(d,d),E=9.05 MeV; m e a s u r e d a(0). laC(d,d),E=9 MeV; m e a s u r e d a(O). l a 0 ( p o l a r i z e d d,d),E=lS-23 MeV; m e a s u r e d a(0), tS0(polarized d,d),E=20 MeV; m e a s u r e d ~(0),iTlt(0 ) ~aO(polarized d,d),E=18-23 MeV; m e a s u r e d a(0), a4Mg(polarized d,d),E=18-23 MeV; m e a s u r e d ~(0), a a s i ( p o l a r i z e d d,d),E=lS-23 MeV; m e a s u r e d a(0), aSS(polarized d,d),E=lS-23 MeV; m e a s u r e d ~(0), a~Ar(polarized d,d),E=18-23 MeV; m e a s u r e d a(0), ~°Ca(polarized d,d),E=18-23 MeV; m e a s u r e d a(0), 4aCa(polarized d,d),E=20 MeV; m e a s u r e d (~(0), aeCa(polarized d,d),E=20 MeV; m e a s u r e d a(0), a~Se(d,d),E=13.6 MeV; m e a s u r e d a ( 0 ) , t o t a l aaTi(d,d),E=13.6 MeV; m e a s u r e d a ( 0 ) , t o t a l 51V(d,d),E=13.6 MeV; m e a s u r e d q(0),totaI SZCr(d,d),E=13.6 MeV; m e a s u r e d a ( 0 ) , t o t a l

82Do07 81Ro13 80Y e 02 79Wa~4 82ClOt 82C103 82C101 82C101 82C101 82C101 82C101 82C101 82C 103 82C103 8lBil6 81Bi16 81Bit6 81Bi16

5aCr(d,d),E=13.6 MeV; m e a s u r e d (7(0),total 54Cr(d,d),E=13.6 MeV; m e a s u r e d a(O),total 54Cr(polarized d,d),E=18-23 MeV; m e a s u r e d a(O), 7eKr(polarized d,d),E=ll MeV; m e a s u r e d a(O),A(0). e ° Z r ( p o l a r i z e d d,d),E=20 MeV; m e a s u r e d a(0), lSeRu(d,d),E=45 MeV; m e a s u r e d a(0). l ¢ 4 S m ( p o l a r i z e d d,d),E=lS-23 MeV; m e a s u r e d a(O), 144Sm(polarized d,d),E=20 MeV; m e a s u r e d a(O), l~SSm(polarized d,d),E=18-23 MeV; m e a s u r e d a(e), l~ZSm(polarized d,d),E=20 MeV; m e a s u r e d a(8), l ~ 4 S m ( p o l a r i z e d d,d),E=18-23 MeV; m e a s u r e d a(O), t ~ 4S m(pol a ri z e d d,d),E=20 MeV; m e a s u r e d a(O), e ° s p b ( p o l a r i z e d d,d),E=18-23 MeV; m e a s u r e d a(O), Z° s pb(pol a ri z e d d,d),E=20 MeV; m e a s u r e d a(O), 2°epb(d,d),E=3-7 MeV; m e a s u r e d a(O) vs E, ZaSTh(polarized d,d),E=18-23 MeV; m e a s u r e d a(O), eaZTh(polarized d,d),E=20 MeV; m e a s u r e d a(0),

81Bi16 81Bi16 82C101 82BuO1 82C103 82Be19 82C101 82C103 82C101 82CI03 88C101 82C103 82C101 8 2 C1 0 3 82Ro15 82C101 82C103

54Cr(polarized d,d'),E=18-23 MeV; m e a s u r e d a(0), S°Zr(polarized d,d'),E=20 MeV; m e a s u r e d iT(O), l a 4 S m ( p o l a r i z e d d,d'),E=18-23 MeV; m e a s u r e d a(e), t 4 4 S m ( p o l a r i z e d d,d'),E=2O MeV; m e a s u r e d a(0), tSSSm(polarized d,d'),E=lS-23 MeV; m e a s u r e d a(e), 152Sin(polarized d,d'),E=20 MeV; m e a s u r e d a(O), l ~ 4S m(pol a ri z e d d,d'),E=18-23 MeV; m e a s u r e d a(O), t ~ 4S m(pol a ri z e d d,d'),E=20 MeV; m e a s u r e d a(O), z°Spb(polarized d,d'),E=18-23 MeV; m e a s u r e d a(0), 2°spb(polarized d,d'),E=20 MeV; m e a s u r e d iv(e), 232Th(polarized d,d'),E=lS-23 MeV; m e a s u r e d o'(0), 232Th(polarized d,d'),E=20 MeV; m e a s u r e d o'(O),

82C101 82C103 82C101 8 2 C1 0 3 82C101 82C103 82C101 82C103 83C101 82C103 82C101 82C103

(d,d') LH(d,d'),E=l.62 GeV; m e a s u r e d a(0). tzC(d,d'),E=9 MeV; m e a s u r e d a(0). taO(polarized d,d'),E=18-23 MeV; m e a s u r e d a(0), l a 0 ( p o l a r i z e d d,d'),E=20 MeV; m e a s u r e d a(O), teO(polarized d,d'),E=18-~3 MeV; m e a s u r e d a(O), 24Mg(polarized d,d'),E=lS-23 MeV; measured t~(O), ZSSi(polarized d,d'),E=18-23 MeV; m e a s u r e d or(0), 32S(polarized d,d'),E=lS-23 MeV; m e a s u r e d a(0), SeAr(polarized d,d'),E=18-23 MeV; m e a s u r e d a(O), 4°Ca(polarized d,d'),E=18-23 MeV; m e a s u r e d ~(0), 4°Ca(polarized d,d'),E=20 MeV; m e a s u r e d or(e), 4aCa(polarized d,d'),E=20 MeV; m e a s u r e d a(0),

82Ba23 79Wa~4 82C101 82C103 82C101 82C101 82C101 82C101 82C101 82C101 82C 103 82C103

(d,2p) 12C(d,2p),E=99.2 MeV; m e a s u r e d a(E(SHe)),a(0).

82Be33

116

REACTION

INDEX

(d,t) ;'Li(d,t),E=9.05 MeV; m e a s u r e d or(O). 91Zr(polarized d,t),E=5 MeV; m e a s u r e d Ta6(O), l°°Mo(polarized d,t),E=16 MeV; m e a s u r e d a(O),a(Ep) UUSn(polarized d,t),E=40 MeV; m e a s u r e d cr(Et),(r(O)

146Nd(polarized d,t),E=16 MeV; m e a s u r e d cr(Et),cr(O) 148Nd(d,t),E=12.1 MeV; m e a s u r e d cr(Ep),cr(Et),cr(O). 147Sm(polarized d,t),E=6.5 MeV; m e a s u r e d Tao(O),

80Y e 02 82Se03 82Ha41 82Ga17

82Ar13 82Ja09 82Se03

(d,aHe) 59Co(d,3He),E=33.3 MeV; m e a s u r e d

cr(E(3He),7).

82Ni01

lS3lr(d,3He),E=40 MeV; m e a s u r e d or(0).

82Bl17

(d,2d) SLi(d,2d),E=9 MeV; m e a s u r e d

momemtum

spectra.

79Su14

(d,c~) ~Li(d,a),E(cm)=35-110 keY; m e a s u r e d a(E). SLi(d,a),E=9.05 MeV; m e a s u r e d a(O). leC(d,a),E=9 MeV; m e a s u r e d a(O). laC(polarized d,a),E=52 MeV; m e a s u r e d a(O),iTn(O) ~SO(polarized d,a),E=52 MeV; m e a s u r e d cr(O),iTu(O) 3zS(d,a),E=4O MeV; m e a s u r e d a(O). :~eS(d,a),E=4-14 MeV; m e a s u r e d or(E).

3aS(polarized d,~),E=16 MeV; m e a s u r e d cr(O),iTi1(O) 34S(polarized d,c[),E=52 MeV; m e a s u r e d (x(0),iTl~(0) a ° A r ( p o l a r i z e d d,~x),E=16 MeV; m e a s u r e d at(0), aSAr(polarized d,a),E=16 MeV; m e a s u r e d or(0), SSNi(polarized d,a),E=80 MeV; m e a s u r e d v e c t o r I°4Ru(d,~),E=20 MeV; m e a s u r e d Ea.

81Go19 81Yu01 79Wa24 82Ma25 82Ma25 82De29 82Qa02

82Ta04 82Ma25 82Ta04 82Ta04 82Na05 82De03

(d,6Li) LaC(d,nLi),E=12.7 .... MeV; m e a s u r e d

(r(E(6Li)),

81Dol5

154Sm(d,SLi),E=33 MeV; m e a s u r e d a(E(6Li)),~(O).

82Ja04

(d,ta) 9Be(d,ta),E=2.5 MeV; m e a s u r e d a(Et,Ot,Oa).

82La09 (d,TLi)

~L3C(d,TLi),E=13.6 MeV; m e a s u r e d (7(E(SLi)),

81Do15

(d,2a) 7Li(d,2a),E=9-13.5 MeV; m e a s u r e d cr(En).

80Ma48 (d,9Be)

:LSF(d,SBe),E=13.6 MeV; m e a s u r e d a(0).

81Go16

(d,F) ~:32Th(d,F),E=70,...

MeV; m e a s u r e d

82Sa08

(d,pF) :"33U(d,pF),E=I3.5 MeV; m e a s u r e d E p , f r a g m e n t

82Pa14

(d,X) 45Sc(d,X),E=13.6 MeV; m e a s u r e d t o t a l a ( r e a c t i o n ) . Ti(d,X),E=13.6 MeV; m e a s u r e d t o t a l a ( r e a c t i o n ) . SIV(d,X),E=13.6 MeV; m e a s u r e d t o t a l a ( r e a c t i o n ) . :i2Cr(d,X),E=13.6 MeV; m e a s u r e d t o t a l q ( r e a c t i o n ) .

82Bi03 82Bi03 82Bi03 82Bi03

53Cr(d,X),E=13.6 MeV; m e a s u r e d t o t a l or(reaction). 54Cr(d,X),E=13.6 MeV; m e a s u r e d t o t a l a ( r e a c t i o n ) . Ta(d,X).E=8 GeV; m e a s u r e d y i e l d s f o r 7981,sz,ss

(d,pX) 93Nb(polarized d,pX),E=56 MeV; m e a s u r e d c o n t i n u u m

81Sa35

117

82Bi03 82Bi03 82Av01

REACTION

INDEX

(d,d'X) g3Nb(polarized d,d'X),E=56 MeV; measured c o n t i n u u m

81Sa35

(t,p) l°B(t,p),E=0.9,1.1 MeV; m e a s u r e d or(O). teC(t,p),E=18 MeV; m e a s u r e d ey(8). 3°Si(t,p),E=15 MeV; m e a s u r e d G(Ep,8). 9SMo(t,p),E=17 MeV; m e a s u r e d G(0). °4Mo(t,p),E=17 MeV; m e a s u r e d a(O).

81Ci06 82F o01 82Fo02 81F106 81F106

97Mo(t,p),E=17 MeV; m e a s u r e d G(8). 9eMo(t,p),E=17 MeV; m e a s u r e d a(0). iS°Sm(t,p~'),E=15 MeV; m e a s u r e d ET,I~,,p'),-coin. lvsyb(t,p),E=15 MeV; m e a s u r e d G(Ep),a(8). a°4Hg(t,p),E=16 MeV; m e a s u r e d 7 ( 0 , H ) , 7 - y i e l d s .

81F106 81F106 82Ka07 82Zu02 82Be38

eSSi(polarized t,t),E=17 MeV; m e a s u r e d G(0),A(8). 32S(polarized t,t),E=17 MeV; m e a s u r e d a(0),A(6). a°sPb(t,t),E=O.5,9,10,t2 MeV; m e a s u r e d a(0),a(Ea).

82ScRi

(t,2n) a°¢Hg(t,2n),E=16 MeV; m e a s u r e d 3'(8,H,t).

82Ma05

(t,2p) IH(t,2p),E at 2.5 GeV/c; m e a s u r e d

particle

82Ch06

(t,t) IH(t,t),E at 2.5 GeV/c; m e a s u r e d p a r t i c l e m o m e n t u m aSMg(polarized t,t),E=17 MeV; m e a s u r e d a(0),A(O). eTAl(polarized t,t),E=17 MeV; m e a s u r e d a(0),A(0).

82Ch06 82Sc21 82Se21

8gBa45 82Wo08

(t,t') 32S(polarized t,t'),E=17 MeV; m e a s u r e d a(O),A(8).

82Ba45 (t,pd)

tH(t,pd),E at 2.5 GeV/c; m e a s u r e d p a r t i c l e

82Ch06 (t,3He)

tH(t,3He),E at 2.5 OeV/c; m e a s u r e d

particle

82C h06

(t,a) 3eS(polarized t,(x),E=17 MeV; m e a s u r e d G(O),A(O). aaSe(t,(x),E=18 MeV; m e a s u r e d a(Ec~),a(0).

82Ba45 82Mo04

lSTEr(t,a),E=17 MeV; m e a s u r e d G(O),G(Ea). 2°8Pb(t,a),E=8.5,9 MeV; m e a s u r e d G(O),cr(Ea).

82De37 82Wo08

(t,da) ~Li(t,da),E=2.5,5 MeV; m e a s u r e d a(0d,Oa) vs a r e

82Ar08 ( 3 H e , ~ +)

3He(SHe,Tr+),E=268.5,282

MeV; m e a s u r e d a(0),a(E*r).

4

81Le24

He( 3 He,~r+ ),E=266.5,280.5 MeV; m e a s u r e d cr(ETr),a(8)

8~Bi06

(SHe,n) laC(SHe,n),E=3.2 MeV; m e a s u r e d E7. a4Mg(SHe,n),E=13 MeV; m e a s u r e d G(En,8). a4Mg(3He,n),B=18.9-41 MeV; m e a s u r e d a ( r e a c t i o n ) vs asMg(3He,n),E=13 MeV; m e a s u r e d G(En,0). 27Al(SHe,n),E=15 MeV; m e a s u r e d a(0),G(En). 27Al(SHe,n),E=18.9-41 MeV; m e a s u r e d or(reaction) vs

eSsi(SHe,n),E=13 MeV; m e a s u r e d a(En,0). aesi(SHe,n),E=18.9-41 MeV; m e a s u r e d ~ ( r e a c t i o n ) vs eOsi(SHe,n),E=15 MeV; m e a s u r e d a(0),a(En). lOTAg(SHe,n),E=threshold-46 MeV; m e a s u r e d a(E). l ° 9 A g ( S H e , n ) , E = t h r e s h o l d - 4 6 MeV; m e a s u r e d G(E). 144Sm(3He,n),E=lS.3 MeV; m e a s u r e d I(ce),(ce)(t).

82Wa16 82Bo14 82Fr03 82Bo14 82A128 82Fr03

82Bo14 82Fr03 83A128 800m01 800m01 82Ka23

(SHe,p) 3He(SHe,p),E=14 MeV; m e a s u r e d A(0). 7Li(3He,p),E=14 MeV; m e a s u r e d P(8). 9Be(3He,p),E=14 MeV; m e a s u r e d P(8). 9Be(3He,p),B=13.6 MeV; m e a s u r e d P(8).

81Ko34 27AI(SHe,p),E=34.8 MeV; m e a s u r e d 81S103 aSsi(SHe,p),E=12-36 MeV; m e a s u r e d 81S103 S~Fe(SHe,p),E=23,35 MeV; m e a s u r e d 82H a 06 ~90o(3He,p),E=34.8 MeV; m e a s u r e d continued

118

cr(0),angle G(E). a(0,Ep),a(0,Ed), G(0),angle

82Bu15 8 2 Q a0 3 8 1 Bu 2 6 82Bu15

REACTION

(3He,p) SBe(3He,p),E=38 MeV; m e a s u r e d a(E(p),0),a(E(d)). ~5Mg(SHe,p),E=8.05-20,425 MeV; m e a s u r e d o-(Ep), z6Mg(SHe,p),E=18.9-41 MeV; m e a s u r e d a ( r e a e t i o n eTAl(aHe,p),E < 14.5 MeV; m e a s u r e d er(Ep).

INDEX

continued

82Zw02 82Bo03 82Fr03 81Sh26

61Ni(aHe,p),E=23,35 MeV; m e a s u r e d (x(O,Ep),cr(0,Ed), l°°Mo(SHe,p),E=25 MeV; m e a s u r e d q(Ep,0). nZSn(SHe,p),E=34.8 MeV; m e a s u r e d (r(0),angle

81Bu26 82De03 82Bu15

(3He,2n) 46Ti(aHe,2n),E=22 MeV; m e a s u r e d 7 7 - c o i n , 7 7 ( t ) . ~°eMo(aHe,2n),E=10-18 MeV; m e a s u r e d a(E,ET), S~Ru(SHe,2n),E ~ 20 MeV; m e a s u r e d ET,17,77-cotn.

82H a 36 82K102

l ° e A g ( a H e , 2 n ) , E = t h r e s h o l d - 4 6 MeV; m e a s u r e d a(E). 144Sm(SHe,2n),E=12.6-27 MeV; m e a s u r e d ET,I7(E),

800m01

82Pa04

82Fe01

(3He,np) 28Si(SHe,np),E=9.5 MeV; m e a s u r e d a(E(n),E(p),0).

82Yo02

(SHe,d) ZaMg(SHe,d),E=18.9-41 MeV; m e a s u r e d a ( r e a e t i o n ) vs e~Al(SHe,d),E=34.8 MeV; m e a s u r e d a ( 0 ) , a n g l e eTAl(aHe,d),E=130 MeV; m e a s u r e d a(0),a(Ed). 27Al(~He,d),E=35 MeV; m e a s u r e d a(Ed,0). ZSSi(aHe,d),E=130 MeV; m e a s u r e d a(0),a(Ed). aSSi(SHe,d),E=lS.9-41 MeV; m e a s u r e d a ( r e a e t i o n ) vs eSSi(aHe,d),E=90 MeV; m e a s u r e d or(0). ~Sca(aHe,d),E=16 MeV; m e a s u r e d a b s o l u t e a(O). 4~Sc(3He,d),E=16 MeV; m e a s u r e d (x(Ed,O). "%Fe(3He,d),E=90 MeV; m e a s u r e d a(0).

STFe(SHe,d),E=23,35 MeV; m e a s u r e d (z(O,Ep),a(O,Ed), 5SCo(SHe,d),E=34.8 MeV; m e a s u r e d a(0),angle 58Ni(SHe,d),E=90 MeV; m e a s u r e d a(0). 81Ni(SHe,d),E=23,35 MeV; m e a s u r e d (;(O,Ep),ct(O,Ed), 9°Zr(3He,d),E=89.3 MeV; m e a s u r e d a(0). gZMo(3He,d),E=16 MeV; m e a s u r e d a b s o l u t e or(6). nZsn(aHe,d),E=34.8 MeV; m e a s u r e d a(0),angle le4Sn(3He,d),E=89.8 MeV; m e a s u r e d a(0). 144Sm(aHe,d),E=240 MeV; m e a s u r e d a(0),a(Et),a(Ed). lSalr(3He,d),E=40 MeV; m e a s u r e d a(e).

82Fr03 82B u15 82Dj03 82Na02 82Dj03 82Fr03 82Ma04 82Fi14 82Hall 82Ma04

81Bu26 82Bu15 82Ma04 81Bu26 82Ma04 82Fi14 82Bu15 82Ma04 82Ga12 82B117

(UHe,2p) lH(SHe,2p),E=69 MeV; m e a s u r e d a(0),~r(0p,0d,Ep),pp~Mg(SHe,2p),E=t8.9-41 MeV; m e a s u r e d a ( r e a c t i o n )

82Wi07 82Fr03

27Al(SHe,2p),E=lS.9-41 MeV; m e a s u r e d

or(reaction)

82Fr03

(SHe,3n) ~SAs(3He,3n),E=25-36 MeV; m e a s u r e d t h i c k t a r g e t e~Sy(SHe,3n),E=33-43 MeV; m e a s u r e d ET,IT(E,t), ~*°Zr(SHe,3nT),E=33-43 MeV; m e a s u r e d ET,17(07,t), l ° S A g ( 3 H e , 3 n ) , E = t h r e s h o l d - 4 6 MeV; m e a s u r e d ~r(E). ~tSb(SHe,3n),E=24.3 .... MeV; m e a s u r e d E(7),1(7),

82B107 82Di09 82De34 800mO1 82Ha46

12ZTe(3He,3n),E=20-27 MeV; m e a s u r e d ET,17,1(ce), ~S4Te(SHe,3n),E=20-27 MeV; m e a s u r e d ET,17,l(ce), 126Te(UHe,3n),E=20-27 MeV; m e a s u r e d ET,IS',l(ce), 2°aTl(SHe,3n),E=20-26.6 MeV; m e a s u r e d ET,IT,a(E7), ~°aTl(3He,3n),E=20-26.6 MeV; m e a s u r e d ET,1T,a(ET),

82Ha44 82Ha44 82Ha44 82Lo14 82Lo14

(3He,2np) ~'6Se(SHe,2np),E=32 MeV; m e a s u r e d

ET,17,TT-coin,

82Doll

(3He,t) 12c(SHe,t),E=130,170 MeV; m e a s u r e d a(Et),a(E(aHe)) 160(3He,t),E=130,170 MeV; m e a s u r e d a(Et),cr(E(SHe)) e4Mg(3He,t),E=18.9-41 MeV; m e a s u r e d a ( r e a c t i o n ) vs ~:TAl(SHe,t),E=34.8 MeV; m e a s u r e d a ( 0 ) , a n g l e ZTAl(ZHe,t),E=18.9-41 MeV; m e a s u r e d a ( r e a c t i o n ) vs eTAl(aHe,t),E=130,170 MeV; m e a s u r e d a(Et), ZSSi(aHe,t),E=130,170 MeV; m e a s u r e d cr(Et), 4"°Ca(3He,t),E=130,170 MeV; m e a s u r e d ¢r(Et), ~'STi(SHe,t),E=130,170 MeV; m e a s u r e d a(Et),

82Ta05 82Ta05 82Fr03 82Bu15 82Fr03 82Ta05 82Ta05 82Ta05 82Ta05

51V(SHe,t),E=24.7 MeV; m e a s u r e d a(Et),Q. SSCo(aHe,t),E=34.8 MeV; m e a s u r e d cr(0),angle SlBr(SHe,t),E=24.7 MeV; m e a s u r e d a(Et),Q. 85Rb(3He,t),E=24.7 MeV; m e a s u r e d cr(Et),Q. 8~Rb(3He,t),E=24.7 MeV; m e a s u r e d a(Et),Q. g°Zr(SHe,t),E=43.4 MeV; m e a s u r e d a(0). 9°Zr(aHe,t),E=130,170 MeV; m e a s u r e d a(Et), UeSn(3He,t),E=34.8 MeV; m e a s u r e d a(0),angle

82Ko06 82Bu15 82Ko06 82Ko06 82Ko06 82Fi09 82Ta05 82Bu15

(SHe,pd) IH(SHe,pd),E=69 MeV; m e a s u r e d cr(0),G(Op,0d,Ep),pp-

82Wi07

(SHe,SHe) 1H(SHe,SHe),E=69 MeV; m e a s u r e d c;(0),(r(0p,0d,Ep), 12C(3He,3He),E=40.9 MeV; m e a s u r e d ¢;(0). 160(SHe,SHe),E=40.9 MeV; m e a s u r e d (r(0). ~8si(SHe,3He),E=90 MeV; m e a s u r e d a(0).

82Wi07 5~Fe(SHe,3He),E=23,35 MeV; m e a s u r e d cr(0,Ep), 82A114 5SNi(3He,3He),E=90 MeV; m e a s u r e d ~(0). 82A114 SlNi(aHe,SHe),E=23,35 MeV; m e a s u r e d cr(0,Ep), 82Ma04 90Zr(3He,aHe),E=89.3 MeV; m e a s u r e d or(0). continued

119

81Bu26 82Ma04 81Bu26 82Ma04

REACTION

(SHe,3He) S4Fe(SHe,SHe),E=90 MeV; m e a s u r e d

or(O).

INDEX

continued

82Ma04

124Sn(SHe,3He),E=89.8 MeV; m e a s u r e d

a(0).

82Ma04

(3He,3He') ZZC(SHe,3He'),E=130,170 l°O(3He,3He'),E=130,170 ZTAI(3He,SHe'),E=130,170 ZSsi(SHe,3He'),E=130,170

MeV; m e a s u r e d cr(Et), MeV; m e a s u r e d cr(Et), MeV; m e a s u r e d cr(Et), MeV; m e a s u r e d G(Et),

82Ta05 82Ta05 82Ta05 82Ta05

4°Ca(SHe,ZHe'),E=130,170 MeV; m e a s u r e d G(Et), 4STi(3He?He'),E=130,170 MeV; m e a s u r e d cr(Et), 3SNi(3He,SHe'),E=130 MeV; m e a s u r e d or(0). g°Zr(SHe,ZHe'),E=130,170 MeV; m e a s u r e d a ( E t ) ,

82Ta05 82Ta05 82Dj02 82Ta05

(SHe,3p) Z4Mg(3He,3p),E=18.9-41 MeV; m e a s u r e d ZTAl(SHe,3p),E=lS.9-41 MeV; m e a s u r e d

a(reaction) a(reaction)

82Fr03 82Fr03

ZeSi(SHe,3p),E=18.9-41

MeV; m e a s u r e d

o(reaction)

82Fr03

(3He,3np) 9°Zr(3He,3np),E=43

MeV; m e a s u r e d

ET,lT(O),Tq,-coin.

82Di09

(3He,a) 7Li(SHe,a),E=42.9 MeV; m e a s u r e d a ( E a ) v s e. lZC(SHe,a),E=99.4 .... MeV; m e a s u r e d cr(E,e). 13C(SHe,a),E=16-23 MeV; m e a s u r e d (r(e),aT(e). 1 7 0 ( p o l a r i z e d 3He,a),E=33 MeV; m e a s u r e d a(0), Z4Mg(3He,a),E=18.9-41 MeV; m e a s u r e d o r ( r e a c t i o n ) v s eSMg(SHe,a),E=8.05-20.425 MeV; m e a s u r e d cr(Ep), eVAl(3He,a),E=34.8 MeV; m e a s u r e d a ( 0 ) , a n g l e ~TFe(3He,a),E=23,35 MeV; m e a s u r e d a(O,Ep),G(O,Ed), SgCo(SHe,a),E=34.8 MeV; m e a s u r e d a ( 0 ) , a n g l e

81An24 81Ta25 82Gu12 82Ka12 82Fr03 82Bo03 82Bu15 81Bu26 82Bu15

elNi(SHe,a),E=23,35 MeV; m e a s u r e d cr(O,Ep),cr(0,Ed), 76Se(SHe,a),E=10-36 MeV; m e a s u r e d or(E). °ZMo(SHe,a),E=25 MeV; m e a s u r e d G(Ea,O). l ° 7 A g ( 3 H e , a ) , E = t h r e s h o l d - 4 6 MeV; m e a s u r e d or(E). 11ZSn(SHe,a),E=34.8 MeV; m e a s u r e d cr(O),angle 11eSn(SHe,a),E=283 MeV; m e a s u r e d cr(Ea),cr(e). lZ4Te(ZHe,a),E=70 MeV; m e a s u r e d a(Ea,0). 13°Te(3He,a),E=70 MeV; m e a s u r e d a ( E a , e ) . Z°epb(3He,a),E=283 MeV; m e a s u r e d cr(Ea),cr(O).

81Bu26 82He01 82Ma07 800m01 82Bu15 82La12 82Ga18 82Ga18 82La12

(3He,ncx)

Z4Mg(SHe,na),E=18.9-41 MeV; m e a s u r e d ZSSi(ZHe,na),E=18.9-41

MeV; m e a s u r e d

a(reaction) or(reaction)

82Fr03 82Fr03

77Se(SHe,na),E=14-36 MeV; measured or(E). 1°~Ag(SHe,na),E=threshold-46 MeV; measured

or(E).

82He01 800m01

(3He,2n~) log

3

Ag( H e , 2 n a ) , E = t h r e s h o l d - 4 6

MeV; m e a s u r e d

if(E).

800m01 (3He,SHe)

ZTAl(ZHe,eHe),E=18.9-41 MeV; m e a s u r e d

or(reaction)

82Fr03 (3He,2pa)

ZeMg(SHe,2pa),E=18.9-41

MeV; m e a s u r e d

a(reaction)

82Fr03

ZTAl(SHe,2pa),E=18.9-41

MeV; m e a s u r e d

a(reactien)

82Fr03

(3He,VLi) ZTAI(ZHe,TLi),E=I8.9-41 MeV; m e a s u r e d

or(reaction)

82Fr03 (SHe,2a)

2ssi(SHe,2a),E=32-41

MeV; m e a s u r e d

(r(reaction)

vs

82Fr03

(SHe,xn) 7SAs(SHe,xn),E=threshold - 70 MeV; measured Se(SHe,xn),E=threshold-36 MeV; measured production 7VSe(SHe,xn),E=threshold-36 MeV; measured 9SNb(3He,xn),E=14-36 MeV; measured c,(E) for x=2,3.

82A120 02He01 82He01 81AulO

Z24Sn(SHe,xn),E=33 MeV; m e a s u r e d z24Sn(SHe,xn),E=43 MeV; m e a s u r e d 15°Nd(SHe,xn),E=33 MeV; m e a s u r e d

120

inclusive inclusive inclusive

82Fi07 82Fi07 82Fi07

REACTION

INDEX

(3He,xnyp) 7SSe(aHe,xnyp),E=threshold-36 7~Se(aHe,xnyp),E=threshold-36

MeV; m e a s u r e d MeV; m e a s u r e d

a(E) a(E)

77Se(aHe,xnyp),E=threshold-36

82He01 82HeOl

MeV; m e a s u r e d

or(E)

82He01

(3He,X) U(aHe,X),E=890

MeV; m e a s u r e d

absolute,comparative

81Bj04

(3He,rr-X) aH(aHe,~r-X),E=910 MeV; m e a s u r e d

g(O(Tr)) v s

pion

82As05

12C(aHe,Tr-X),E=910 MeV; m e a s u r e d

g(0(w))

vs p i o n

82As05

(r(0(w)) vs p i o n

82As05

(SHe,st+X) ~H(aHe,~r+X),E=910 MeV; m e a s u r e d aH(aHe,Tr+X),E=91O MeV; m e a s u r e d

a(e(rr)) v s p i o n a(0(~r)) v s

pion

laC(aHe,Tr+X),E=St0 MeV; m e a s u r e d

82As05 82As05

(~,v) a H ( a , y ) , E ( c m ) = l .... MeV; m e a s u r e d a(eapture) v s E. 3He(a,T),E(cm)=107-1266 keV; measured cr(E,E%OT), aHe(a,7),E(cm)=165-1170 keV; measured or(absolute) 14N(a,7),E ~ 1 5 1 7 . 5 - 1 5 3 5 k e V ; m e a s u r e d ~r(O,E), ~ a 0 ( a , ~ ) , E = 3 . 0 2 0 , 3 . 0 3 6 MeV; m e a s u r e d ET,17. a4Mg(a,'7),E=3.7-5.1 MeV; m e a s u r e d a ( E ) , a ( E T , 8 ) .

81Ro12 82KP05 820s02 82Ev01 82Ev01 82Cs01

a v C l ( a , y ) , E = 2 . 9 - 5 . 2 3 MeV; m e a s u r e d a(E). a S A r ( c ~ , 7 ) , E = 5 . 4 9 5 - 5 . 5 0 5 MeV; m e a s u r e d ET,tT,T 4 ° C a ( a , y ) , E = 4 . 4 6 - 4 . 6 2 MeV; m e a s u r e d , E T , l % Q . 8 e N i ( a , T ) , B = 5 . 0 7 - 8 . 6 4 MeV; m e a s u r e d a(E). e 4 N i ( a , 7 ) , E = 4 . 5 - 7 . 4 5 MeV; m e a s u r e d a(E).

79Zy04 82Pr05 82Di05 79Zy04 79Zy04

K(a,rr-),E=977,772 MeV/nucteon;

82St13

(~,~-) Cl(u,~r-),E=977,772

MeV/nucleon;

measured

pion

828t13

measured p i o n

(a,n) l a C ( a , n ) , E = 5 . 4 9 8 MeV; m e a s u r e d E%l-y. l S F ( a , n ) , E = 5 MeV; m e a s u r e d TT-coin. 24Mg(a,n),E=20-37 MeV; m e a s u r e d a ( r e a c t i o n ) v s E. a S M g ( a , n T ) , E = 1 4 , 1 5 . 5 MeV; m e a s u r e d nT-coin,nT(0), 2 7 A l ( a , n ) , E = 2 0 - 3 7 MeV; m e a s u r e d o r ( r e a c t i o n ) v s E. 2 7 A l ( a , n ) , E = l O - 3 0 MeV; m e a s u r e d a(E). s a S i ( a , n ) , P . = 2 0 - 3 7 MeV; m e a s u r e d a(reaction) v s E. a l P ( a , n T ) , E = l l . 7 , 1 6 . 3 MeV; m e a s u r e d a(ET,E), 4 3 C a ( a , n ) , E = 1 2 - 1 7 MeV; m e a s u r e d o(E),yT-coin. S ° T i ( a , n ) , E = l l MeV; m e a s u r e d ET,IT,linear C r ( a , n ) , E = l l MeV; m e a s u r e d ET,I%linear 5 8 N i ( a , n T ) , E = 1 0 . 7 5 - 1 6 MeV; m e a s u r e d Ty-,nT-eoin,

82Al19 8aVe05 82Fr03 81G105 82Fr03 82Qa02 82Fr03 82Va02 82Ra01 82By01 82By01 82Sm0I

4 H e ( a , p ) , E = 3 7 - 4 3 MeV; m e a s u r e d a ( 0 ) v s B,cr(Ep). 1 2 C ( a , p ) , E = 1 0 . 5 - 2 0 MeV; m e a s u r e d a(Ea),a(Ep),a(0) a S M g ( a , p ) , E = 2 0 - 3 7 MeV; m e a s u r e d c r ( r e a c t i o n ) v s E. a e M g ( a , p ) , E = 2 0 - 3 7 MeV; m e a s u r e d a(reaction) v s E. A l ( a , p ) , E = 3 1 . 2 MeV; m e a s u r e d a(Ep). A l ( a , p ) , E = 1 8 MeV; m e a s u r e d a(O),a(Ep). saSi(a,pT),E=7.95,8 MeV; m e a s u r e d pT(e,H) i n

82SI01

6 S N i ( a , n ) , E = 6 . 9 5 - 8 . 7 6 MeV; m e a s u r e d a(E). 6 4 N i ( a , n ) , E = 5 . 3 - 7 . 4 5 MeV; m e a s u r e d a(E). e°Se(¢x,ny),E=10,... MeV; m e a s u r e d ET,IT,TT-coin, lOaRh(a,n),E=14-42 MeV; m e a s u r e d t h i c k t a r g e t HTSn(a,n),E=16,18,20 MeV; m e a s u r e d 7 T - c o i n , T ( e ) , n ~ S n ( a , n ) , E = 1 8 MeV; m e a s u r e d 7~/-coin,3'(e),a(ET). l a S S n ( a , n ) , E = 2 5 MeV; m e a s u r e d T(t),7(0,H,t). ~ z l S b ( a , n ) , E = l l . 5 - 2 7 MeV; m e a s u r e d a(E). 1 3 ° T e ( a , n ) , E = 1 0 - 5 3 . 5 MeV; m e a s u r e d a b s o l u t e or(E). l S V A u ( a , n ) , E = 1 1 . 5 - 2 7 MeV; m e a s u r e d or(E). a ° ~ B i ( a , n ) , E = l S - 2 8 MeV; m e a s u r e d TT-,(X-ray)T-coin

79Zy04 79Zy04 82Es01 81Dm01 82Ch01 82Ch01 811005 82Ca10 82Wa14 82Ca10 82Lo0I

4 a T i ( a , p ) , E = 8 MeV; m e a s u r e d Ty(0),py-coin,recoit, 4STi(a,p),E ~ 24 MeV; m e a s u r e d cr(0),a(Ea'),a(Ep). V ( a , p ) , E = 3 1 . 2 MeV; m e a s u r e d a(Ep). F e ( a , p ) , E = 3 1 . 2 MeV; m e a s u r e d a(Ep). C o ( a , p ) , E = 3 1 . 2 MeV; m e a s u r e d (~(Ep). C o ( a , p ) , E = 1 8 MeV; m e a s u r e d cr(0),ex(Ep). S a c u ( a , p T ) , E = 1 6 . 7 MeV; m e a s u r e d ET,13,,DSA,pT-coin.

810h08 82An07 80Yal2 80Yal2 80Yal2 81Zh04 81Zh07

(a,P) 82Am02 82Fr03 82Fr03 80Yal2 81Zh04 82Ho06

(~,an) 6SZn(a,2n),E=23 74Ge(a,2n),E=27

MeV; m e a s u r e d l(ce). MeV; m e a s u r e d 7T(t),y(0),linear 7SGe(a,2n),E=27 MeV; m e a s u r e d 7 T ( t ) , ~ ( O ) , l i n e a r 7SAs(a,Rn),E=14-28 MeV; m e a s u r e d t h i c k t a r g e t 7 S S e ( a , 2 n ) , E = 2 7 MeV; measured E 3 , , 1 7 , D S A , T T - c o i n . a S s e ( a , 2 n ) , E = 1 6 . 5 - 2 7 . 3 MeV; m e a s u r e d E%IT,7(t), S S R b ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-eoin,IT,(x(On), 8 S y ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,IT,cr(en), S ° Z r ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,ly,cr(0n), tOaRh(a,2n),E=14-42 MeV; m e a s u r e d t h i c k t a r g e t I°4Pd(a,2n),E=35 MeV; m e a s u r e d nT-coin,IT,~r(On), I ° s p d 0 x , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,17,(r(On),

79Ne09 l l S S n ( a , 2 n ) , E = 2 2 - 3 3 MeV; m e a s u r e d E%IT,YT(8), laOSn(a,2n),E=35 MeV; m e a s u r e d c¢(En). 81Ma39 81Ma39 t a O S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,I'y,a(On), 1 2 4 S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d ¢x(En). 82B107 82An06 1 2 4 S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d n~-eoin,13',a(On), 1 2 1 S b ( a , 2 n ) , E = 2 6 MeV; m e a s u r e d la3I yield~ 82Za04 82Fi02 1 a i S b ( a , 2 n ) , E = l l . 5 - 2 7 MeV; m e a s u r e d a(E). 82Fi02 1 3 9 L a ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,IT,cr(On), 82Fi02 1 4 a N d ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,Iy,a(On), 81Dm01 1 4 a N d ( a , 2 n ) , E = 2 8 , 3 2 MeV; m e a s u r e d nT-coin,IT,cr(0n) 82Fi02 ~ 5 ° N d ( a , 2 n ) , E = 3 2 MeV; m e a s u r e d a(En). 82Fi02 lSSNd(a,2nT),E=Sl-26 MeV; m e a s u r e d ET,IT,I(ee), continued

121

82Va10 81Fi06 82Fi02 81Fi06 82Fi02 81Vel7 82Ca10 B2Fi02 82Fi02 82Fi02 81Fi06 82K003

REACTION

(a,an) ~ o 8 p d ( a , 2 n ) , E = 3 2 MeV; m e a s u r e d a(En). Z ° e p d ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d n'y-coin,17,a(en), l ° e P d ( a , 2 n ) , E = 3 2 MeV; m e a s u r e d nT-coin,l'~,a(On), n ° P d ( a , 2 n ) , E = 3 5 Me¥; m e a s u r e d n'y-eoin,17,~(Sn), n ° P d ( a , 2 n ) , E = 2 8 , 3 2 MeV; m e a s u r e d nT-coin,IT,a(0n) i t s C d ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d 7(8,H,t). U a S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d a(En). n e S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,l'y,a(en), U 4 S n ( a , 2 n ) , E = 2 2 , 2 4 MeV; m e a s u r e d "yT-coin,~/(O), n a S n ( a , 2 n ) , E = 2 2 MeV; m e a s u r e d 77-coin,7(e),a(ET). naSn(a,2n),E=22-33 MeV; m e a s u r e d E'y,I%77(0), U e S n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d a(En). n e s n ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,IT,a(On),

INDEX

continued

81Fi06 82Fi02 82Fi02 82Fi02 82Fi02 81Go17 81Fi06 82Fi02 82Ch01 82Ch01 82Va10 81Fi06 82Fi02

t S 2 S m ( a , a n ) , E = 1 9 . 5 MeV; m e a s u r e d ET,l~,,linear t S O G d ( a , 2 n ) , E = 2 4 , 2 8 MeV; m e a s u r e d E(7),I(7)(E,t,e) z S 2 D y ( a , 2 n ) , E = 2 4 MeV; m e a s u r e d E%lT(0,t),77-coin. l S S H o ( a , 2 n ) , E = 2 6 . 5 MeV; m e a s u r e d "y(e). l S S H o ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d n'y-coin,17,a(0n), 1 2 e E r ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d 7"Y-coin,'y(0). 1 7 5 L u ( a , 2 n ) , E = 2 9 . 5 MeV; m e a s u r e d 7(0),E7,I7, l ~ S L u ( a , 2 n ) , E = 2 9 . 5 MeV; m e a s u r e d E'y,IT,a(ET,O), l S X A u ( a , 2 n ) , E = l l . 5 - 2 7 MeV; m e a s u r e d a(E). I ° ~ A u ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,17,a((~n), Z o e p b ( a , 2 n ) , E = 3 5 MeV; m e a s u r e d n~'-coin,I%a(en), a a S U ( a , 2 n ) , E = 2 5 . 2 MeV; m e a s u r e d "7(0,H,T).

82Da12 82Fi15 82Fi06 811o06 82Fi02 82Wa19 82Ao02 82Ao04 82Ca10 82Fi0~ 82Fi02 82Ra04

2 e s i ( a , d ) , E = 1 6 - 2 8 MeV; m e a s u r e d a(E). 3 2 S ( a , d ) , E = 5 0 MeV; m e a s u r e d a(8).

82Qa02 82De29

(a,np) 74Se(a,np),E=37

MeV; m e a s u r e d

E~',lT,7"y-coin,a(E'y),

82Doll

(a,d) S B e ( a , d ) , E = 4 8 MeV; m e a s u r e d a(E(p),0),a(E(d)). a a S i ( a , d ) , E = 5 0 MeV; m e a s u r e d a(0). 2 a S i ( a , d ) , E = 2 8 - 3 7 MeV; m e a s u r e d a(reaction) v s E.

82Zw02 82De29 82Fr03

(~,ap) ~Mg(a,2p),E=20-37 ~Al(a,2p),E=20-37

MeV; m e a s u r e d MeV; m e a s u r e d

a(reaction) a(reaction)

v s E. v s E.

2eSi(a,2p),E=20-37

82Fr03 82Fr03

MeV; m e a s u r e d

a(reaction)

v s E.

83Fr03

(a,3n) 7 S S e ( a , 3 n ) , E = 3 0 - 5 5 MeV; m e a s u r e d cr(ET,E),T(e),ET, l ° ° M o ( a , 3 n ) , E = 3 4 - 4 6 MeV; m e a s u r e d a(E,ET),a(ET,O), u ° p d ( a , 3 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,I'7,a(On), U 3 1 n ( a , 3 n T ) , E = 3 6 - 4 8 MeV; m e a s u r e d E'y,IT,'y'y-coin, USln(a,3n7),E=36-48 MeV; m e a s u r e d ET,IT,TT-coin, U a S n ( a , 3 n ) , E = 3 5 MeV; m e a s u r e d nT-coin,lT,a(0n),

82Be48 82K102 82Fi02 82Va07 82Va07 82Fi02

ta°Sn(c~,3n),E=35 124Sn(a,3n),E=35 t4eNd(a,3n),E=35 14SNd(a,3n),E=32 lSSHo(a,3n),E ~ tgTAu(a,3n),E=35

MeV; MeV; MeV; MeV; 34-46 MeV;

measured nT-eoin,17,a(en), measured nT-coin,l'y,a(en), measured n~/-coin,IT,a(On), measured n~/-coin,l%a(0n), MeV; m e a s u r e d a(E'y),'yT(0), measured nT-coin,IT,a(0n),

144Sm(a,t),E=80

MeV; m e a s u r e d

82Fi02 82Fi02 82Fi02 82Fi02 82E102 82Fi02

(a,2np) 77Se(a,3np'~),E=40-50

MeV; m e a s u r e d

a(E,E~'),E'7,1~,,

82Be03

(~,t) 4 e C a ( a , t ) , E = 2 6 - 3 0 MeV; m e a s u r e d 9 e M o ( a , t ) , E = 2 6 - 3 0 MeV; m e a s u r e d

absolute absolute

82Fi14 82Fi14

a(0). a(0).

a(t)),a(Et),cr(Ed).

82Ga12

(a,3He) a T A l ( a , a H e ) , E = 2 8 - 3 7 MeV; m e a s u r e d

a(reaetion)

vs E

82Fr03

(a,4n) 2°4Pb(a,4n),E=50

MeV; m e a s u r e d

82Ha16

ce(0,H,t).

(~,2d) eLi(a,2d),E=18

MeV; m e a s u r e d

momemtum

spectra.

79Su14

(a,a) ~ H ( a , a ) , E = 6 - 1 4 MeV; m e a s u r e d a(Ed),ad-coin,a(E), 3 H e ( a , a ) , E = 0 . 2 3 MeV; m e a s u r e d y i e l d v s E. 9 B e ( a , a ) , E = 3 5 . 5 MeV; m e a s u r e d ~(8). ZaC(c~,a),E=10.5-20 MeV; m e a s u r e d o-(Ea),a(Ep),cr(O) 12C(a,a),E=3.5-3.63 MeV; measured 0"(8) vs E.

82Br09 SSNi(a,a),E=480 82Kr05 58Ni(a,a),E=25 82Pe03 60Ni(a,a),E=25 82Am02 SZNi(a,a),E=25 82Fr10 S4Ni(a,a).E=fi5 continued

122

MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

a(0). a(0). a(0). a(•). a(0).

81A127 82En04 82En04 82En04 82En04

REACTION

(a,a) ~¢N(c~,a),E ,.~ 1 5 1 7 . 5 - 1 5 3 5 k e Y ; m e a s u r e d a(0,E), t ¢ N ( a , a ) , E = 3 4 . 8 5 MeV; m e a s u r e d a(Ea),a(e). t ~ O ( a , a ) , E = 3 . 5 - 4 . 9 MeV; m e a s u r e d a(e). a 4 M g ( a , a ) , E = 2 . 6 - 4 . 9 MeV; m e a s u r e d a(E,O). atP(a,a),E=27.2 MeY; m e a s u r e d a(O). ~ S S c ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d a(e),total * e T i ( a , a ) , E = 2 7 . 3 MeV; m e a s u r e d a(O),total ~ V ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d a(O),total 5 ~ V ( a , a ) , E = 2 5 MeY; m e a s u r e d a(O). C r ( a , a ) , E = 2 7 . 2 Me'V; m e a s u r e d a(0). 5 0 C r ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). 5 2 C r ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d ¢r(0),total 52Cr(a,a),E=27.2 MeV; m e a s u r e d a ( 0 ) . ~ a C r ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). 5 3 C r ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d a(0),total ~ 3 C r ( a , a ) , E = 2 5 MeV; m e a s u r e d or(0). 5 4 C r ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d a(0),total S 4 C r ( a , a ) , E = 2 7 . 2 MeV; m e a s u r e d (r(O). S 4 F e ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). S ~ F e ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). ~BFe((~,a),E=25 MeV; m e a s u r e d a(O). S g C o ( a , a ) , E = 2 5 MeV; m e a s u r e d a(O).

INDEX

continued SaCu(a,a),E=25 MeV; m e a s u r e d

82EvO1 82Pe05 81Bu27 82CsOl 78Go21 81Bil6 81Bil6 81Bil6 82En04 81Bu25 82En04 81Bi16 81Bu25 82En04 81Bi16 82En04 81Bi16 81Bu25

a(e). S ~ C u ( a , a ) , E = 2 5 MeV; m e a s u r e d a(O). S4Zn(a,(x),E=25 MeV; m e a s u r e d a(e). S S Z n ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). SeZn(a,a),E=25 MeV; m e a s u r e d a(O). 7 B Z n ( a , a ) , E = 2 5 MeV; m e a s u r e d a(8). 7°Ge(a,(x),E=25 MeV; m e a s u r e d a(0). ~ e G e ( a , a ) , E = 2 5 MeV; m e a s u r e d a(0). 73Ge(a,a),E=25 MeV; m e a s u r e d a(O). 74Ge(a,a),E=25 MeV; m e a s u r e d a ( 0 ) . ~SGe(a,a),E=25 MeV; m e a s u r e d a(O). 76Se(a,a),E=25 MeV; m e a s u r e d a(O). 78Se(a,a),E=25 MeV; m e a s u r e d a(O). 8°Se(a,¢t),E=25 MeV; m e a s u r e d a(O). BgY(c~,a),E=25 MeV; m e a s u r e d a(O). 9°Zr(a,c*),E=104 MeV; m e a s u r e d a(8). 9 a Z r ( ~ , ~ ) , E = 1 0 4 MeV; m e a s u r e d a(O). 9 S N b ( a , a ) , E = 2 5 MeV; m e a s u r e d or(0). n S S n ( a , a ) , E = 4 8 0 MeV; m e a s u r e d a(e). a ° e P b ( a , a ) , E = 3 4 0 , 4 8 0 MeV; m e a s u r e d a(O). a4SBk(a,(~),E=17.06 MeV; m e a s u r e d a(Ea,e=1500).

82En04 82En04 82En04 82En04

82En04 82En04 82En04 82En04

82En04 82En04 82En04 82En04 82En04 88END4 82En04 82En04 82En04 82En04 82En04

82Co09 82Co09 82En04

81A127 81A127 8aBel2

(a,~') 9 B e ( a , a ' ) , E = 3 5 . 5 MeV; m e a s u r e d a(0). 12C((~,a'),E=I04 MeV; m e a s u r e d a(Ea),a(e). 1 2 C ( a , a ' ) , E = 1 0 . 5 - 2 0 MeV; m e a s u r e d cr(E(x),a(Ep),a(O) t4N(c~,a'),E=34.85 MeV; m e a s u r e d a(Ea),a(0). ~ O ( a , a ' ) , E = 9 . 5 2 - 9 . B MeV; m e a s u r e d a(E(a),O(al)), 1 7 0 ( a , a ' 7 ) , E = 5 . 4 8 6 MeV; m e a s u r e d E7,17. ~ ° 0 ( a , ~ ' 7 ) , E = 5 . 4 8 6 MeV; m e a s u r e d E7,17. ~ g F ( a , a ' ) , E = 5 MeV; m e a s u r e d "/T-coin. 3OSi(a,a'),E=120 MeV; m e a s u r e d a(O). ~SCa(a,(x'),E=70 MeV; m e a s u r e d a(O). ~ S T i ( a , a ' ) , E ~ 24 MeV; m e a s u r e d a(O),ct(Ea')jy(Ep). C r ( a , a ' ) , E = 2 7 . 2 MeV; m e a s u r e d or(0). 5 2 C r ( a , a ' ) , E = 2 7 . 2 MeV; m e a s u r e d a(O). 5 * C r ( a , a ' ) , E = 2 7 . 2 MeV; m e a s u r e d a(O). 5 S N i ( a , a ' ) , E = 4 8 0 MeV; m e a s u r e d or(0). S S N i ( a , a ' ) , E = 1 2 9 MeV; m e a s u r e d a(O),a(Ea'). °~Rb(a,cx'),E=3 MeV; m e a s u r e d Coulomb excitation.

82Pe03 81Ey02 82Am03 82Pe05 81G235 82Hs01 82Hs01 82Ve05 82Sa15 82Fu02 82An07 81Bu25 81Bu25 81Bu25 81A127 82Ga16 82F209

9 ° Z r ( a , a ' ) , E = 1 0 4 MeV; m e a s u r e d a(0). 9 ° Z r ( a , a ' ) , E = 9 9 . 3 MeV; m e a s u r e d a(Ea'),c~7(O ). 9 a Z r ( a , a ' ) , E = 1 0 4 MeV; m e a s u r e d a(O). U S S n ( a , a ' ) , E = 4 8 0 MeV; m e a s u r e d a(O). l ¢ 4 S m ( a , a ' ) , E = 8 3 . 8 .... MeV; m e a s u r e d ct(0,E). * S S D y ( a , a ' ) , E = l a - 1 6 MeV; m e a s u r e d a. l S e D y ( a , a ' ) , E = 1 2 - 1 6 MeV; m e a s u r e d a. lSaEr(a,a'),E=12-16 MeV; m e a s u r e d ¢r 1 6 4 E r ( a , a ' ) , E = l S - 1 6 MeV; m e a s u r e d a. 1 6 8 Y b ( ~ , a ' ) , E = 1 2 - 1 6 MeV; m e a s u r e d a. 2 ° 8 p b ( a , a ' ) , E = 3 4 0 , 4 8 0 MeV; m e a s u r e d ct(O). 2 ° s P b ( a , a ' ) , E = 8 3 . 8 .... MeV; m e a s u r e d ¢r(0,E). e a a T h ( a , a ' ) , E = 1 0 0 , 1 7 2 MeV; m e a s u r e d a(e). eaSU(a,a'),E=lO0,172 MeV; m e a s u r e d (;(0). Z 4 S A m ( a , a ' ) , E = 1 7 MeV; m e a s u r e d ¢r(Ea',0=150°), a49Bk(a,cz'),E=lT.06 MeV; m e a s u r e d ~(Ea,8=150°).

82Co09

82Ta10 82Co09 81A127 82Ya02 82Ro07 82Ro07 82Ro07 82Ro07 82Ro07 81A127 82Ya02 82Moli 82Moli

81Be54 83Be12

(~,Sn) 14SSm(a,5n),E=76

MeV; m e a s u r e d

E T , I T , 7 7 - c o i n , 7 ( O ).

82Br13

a,na) 119Sn((~,a'n),E=109 MeV; m e a s u r e d

(;(Ea,0a),

820k01

aosPb(a,a'n),E=104

MeV; m e a s u r e d

na-coin,Ea,En.

81St25

MeV; m e a s u r e d

a(reaction) a(reaetion)

82Fr03

(a,pa) aH(a,pa),E=lO.27,11.3,13 MeV; m e a s u r e d

a(Ep,0p,0a) a H ( ~ , p a ) , E = 9 . 8 4 7 - : [ 3 . 9 9 1 MeV; m e a s u r e d cr(Oa,0p) 2H(cx,~p),E=140 MeV; m e a s u r e d cr(Ecx,Ep,Oa,0p). a * M g ( a , p a ) , E = 1 2 0 MeV; m e a s u r e d ap(O),aa(0),a(Ea),

81Br25 82Br17 82La14 82Zw01

29Si(a,pa),E-28-37

3°Si(a,pa),E=28-37 MeV; m e a s u r e d 4°Ca(a,pa),E=la0 5SNi(a,pa),E=140

MeV; m e a s u r e d MeV; m e a s u r e d

v s E. v s E.

ap(O),aa(O),a(Ec~), a(Ol,Oz,EI,E~),

82Fr03 82zwo1 82Be22

(~,6n) a°3Tl(a,6n),E=66,70.77

MeV; m e a s u r e d

ET,IT,7(t),

82Br21 (c¢,6He)

l~SSn(a,SHe),E=218 MeV; m e a s u r e d

a(E(SHe)),a(0).

8aGe06

20sPb(cLSHe),E=218 MeV; m e a s u r e d

123

a(E(SHe)),o-(0).

8aGe06

REACTION

INDEX

(a,da) LSO(a,da),E=139.2 MeV; m e a s u r e d

a(Ei,Ez,Ot,Oz).

82Sa24

(a,ta) lSO(a,ta),E=139.2

o'(Ei,Ez,Ol,0e).

MeV; m e a s u r e d

82Sa24

(a,3Hea) *SO(a?Hea),E=139.2

MeV; m e a s u r e d

a(EI,Ez,Ol,0z).

82Sa24

(a,2~) SLi(a,2a),E=18 MeV; m e a s u r e d S L i ( a , 2 a ) , E = 1 8 MeV; m e a s u r e d 7 L i ( a , 2 a ) , E = 1 8 MeV; m e a s u r e d

momemtum as(0). aa(0).

spectra.

798u14 80Zh05 80Zh05

Z 4 M g ( a , 2 a ) , E = 1 2 0 MeV; m e a s u r e d 4°Ca(a,2a),E=120 MeV; m e a s u r e d 5SNi(a,2a),E=140 MeV; m e a s u r e d

c~p(O),aa(O),a(Ea), ap(O),aa(O),a(Ea), a(01,02,Ei,Ez),

82ZwO1 82Zw01 82Be22

(c(,xn) S g C o ( a , x n ) , E = 2 8 - 3 2 MeV; m e a s u r e d a(En,0n),a(Ep,Op) ° ° N i ( a , x n ) , E = 2 8 - 3 2 MeV; m e a s u r e d a(En,On),a(Ep,Op) ~SAs(a,xn),E=threshold - 1 4 0 MeV; m e a s u r e d t ° s p d ( a , x n ) , E = 3 1 . 5 MeV; m e a s u r e d E7,I7. t 2 4 S n ( a , x n ) , E = 3 5 MeV; m e a s u r e d inclusive * S ° N d ( a , x n ) , E = 3 5 MeV; m e a s u r e d inclusive * S ° N d ( a , x n ) , E = 3 5 MeV; m e a s u r e d a(O). 1 5 4 G d ( a , x n ) , E = 4 0 - 1 1 0 MeV; m e a s u r e d E7,17(0).

* S S G d ( a , x n ) , E = 4 0 - 1 1 0 MeV; m e a s u r e d E7,15'(0 ). * 5 e G d ( a , x n T ) , E = 7 O MeV; m e a s u r e d a(En),a(0n),iT,E7 i S e G d ( a , x n ) , E = 4 0 - 1 1 0 MeV; m e a s u r e d ET,17(O). 1 6 ° G d ( a , x n ) , E = 4 0 - 1 1 0 MeV; m e a s u r e d E7,17(0). 1 7 4 Y b ( a , x n ) , E = 2 7 MeV; m e a s u r e d ET,IT,aT(t). 1 7 6 Y b ( a , x n ) , E = 2 7 MeV; m e a s u r e d ET,Iv,aT(t). Z°3Tl(cx,xn),E=64 MeV; m e a s u r e d 7(O,H,t).

82Sc18 82Sc18 82A120 82Ao02 82Fi07 82Fi07 82Fi07 82Lu03

83Lu03 82De13 82Lu03 82Lu03 82Ko08 82Ko08 82Hu07

(a,xp) 5gCo(a,xp),E=28-32

MeV; m e a s u r e d

a(En,0n),a(Ep,0p)

82Sc18

S°Ni(a,xp),E=28-32

MeV; m e a s u r e d

a(En,en),ar(Ep,ep)

82Sc18

MeV; m e a s u r e d

a(En,0n),a(Ep,Op)

82Sc18

(Ot,X(~) 5SCo(a,xa),E=28-32

MeV; m e a s u r e d

a(En,On),a(Ep,0p)

82Sc18

S°Ni(a,xa),E=28-32

(a,F) 82SAO8 82DroOl

2aZTh(a,F),E=69.2,... MeV; m e a s u r e d 2 3 S u ( a , F ) , E = 2 8 , 3 6 MeV; m e a s u r e d fission

Z37Np(~,F),E=28,36 MeV; m e a s u r e d 2 4 9 C f ( a , F ) , E = 2 8 , 3 6 MeV; m e a s u r e d

fission fission

82DmO1 82DmO1

(a,aF) 2 S 2 T h ( a , a ' F ) , E = 1 2 0 MeV; m e a s u r e d

a(fragment

O),

82Da14

2 S e U ( a , a ' F ) , E = 1 2 0 MeV; m e a s u r e d

a(fragment,~,e),

82De07

(~,x) 4 H e ( a , X ) , E = 6 0 - 1 6 0 MeV; m e a s u r e d a(fragment 0,E), C ( a , X ) , E = l . 5 9 , 4 . 1 9 GeV; m e a s u r e d absolute t2C(a,X),E=94,173 MeV/nucleon; measured total 4SSc(a,X),E=27.2 MeV; m e a s u r e d total a(reaction). T i ( a , X ) , E = 2 7 . 2 MeV; m e a s u r e d total a(reaction). 5JV(a,X),E=27.2 MeV; m e a s u r e d total a(reaction). S2Cr(a,X),E=27.2 MeV; m e a s u r e d total a(reaction). S a C r ( a , X ) , E = 2 7 . 2 MeV; m e a s u r e d total a(reaction). a4Cr(a,X),E=27.2 MeV; m e a s u r e d t o t a l a ( r e a c t i o n ) .

SSCo(a,X),E n o t g i v e n ; m e a s u r e d residuals s a N i ( a , X ) , E = 1 7 2 . 5 MeV; m e a s u r e d a(fragment O;E), Z r ( a , X ) , E <- 55 MeV; m e a s u r e d production a(E) for Ag(a,X),E=0.135-4 MeV/nucleon; measured L-shell Ta(a,X),E=0.125-4 MeV/nucleon; measured L-shell T a ( a , X ) , E = 1 5 . 2 GeV; m e a s u r e d y i e l d s f o r ~gst,sa, Au(a,X),E=0.125-4 MeV/nucleon; measured L-shell 1SVAu(a,X),E=172.5 MeV; m e a s u r e d (;(fragment 0,E),

82G101 83Ge05 82De20 82Bi03 82Bi03 82Bi03 82Bi03 82Bi03 82Bi03

(a,a'X) 54Fe(a,a'X),E=59 .... MeV; m e a s u r e d

a(Ea,Oa).

82Ma28

(°Li,p) 4°Ca(SLi,p),E=156 MeV; m e a s u r e d

o~(O) v e r s u s

82Ne02

124

82Pa19 82LuOl 81De39 81Ba56 81Ba56 82AvOl 81Ba56 82LuOl

REACTION

INDEX

(6Li,np) ~°O(SLi,np),E=7.3,...

MeV; m e a s u r e d

relative

81XeO1

3°Si(SLi,np),E=9.2,...

MeV; m e a s u r e d

relative

8iXeQt

(6Li,d) 14C(SLi,d),E=34 MeV; m e a s u r e d a(Ed),da-eoin,da(O), l°O(SLi,d),E=75 MeV; m e a s u r e d a(O). ~UO(SLi,d),E=7.3 .... MeV; m e a s u r e d r e l a t i v e lSO(~Li,d),E=72 MeV; m e a s u r e d (~(0).

2aSi(SLi,d),E=75 MeV; m e a s u r e d a(8). 3°Si(SLi,d),E=9.2 .... MeV; m e a s u r e d r e l a t i v e ¢°Ca(SLi,d),E=156 MeV; m e a s u r e d a(O) v e r s u s

82CuOl 81Ta23 81XeOl 82Ta15

81Ta23 81XeOl 82Ne02

(SLi,3n) aZSe(~Li,3n),E=27 MeV; m e a s u r e d ET,I-/(O),a(E,E-/), 81Br(~Li,3n),E=19-32 MeV; m e a s u r e d E7,I-/,-/T-coin, 9~Mo(SLi,3n),E=18-34 MeV; m e a s u r e d E%I-/,-/(0),n-/-, 9SMo(~Li,3n),E=18-34 MeV; m e a s u r e d E % l % - / ( 0 ) , n 7 - , ll*Sn(~Li,3n),E=33 MeV; m e a s u r e d E-/,I-/,a(E-/),-/(e),

82Ze02

XSC(SLi,t),E=24-26 MeV; m e a s u r e d cr(O,E),cr(O),a(Et) tSC(~Li,t),E=9-35 MeV, m e a s u r e d a ( f u s i o n , E ) .

82AbO~ 82Ab02

llSSn(aLi,3n),E=33 MeV; m e a s u r e d E-/,IT,cr(E-/),-/(e), naSn(SLi,3n),E=33MeV; measured E-/,IT,o(E-/),-/(0), t a ° s n ( S L i , 3 n ) , E = 3 2 - 3 4 MeV; m e a s u r e d E-/,I-/,-/-/-coin, t2aSn(SLi,3n),E=32-34 MeV; m e a s u r e d Ev,I-/,-/-/-coin, le4Sn(OLi,3n),E=32-34 MeV; m e a s u r e d E-/,IT,-/-/-eoin,

82De05

82Ka15 82Ka15 82Ga21

82Ga21 82Ga21 82Sh20 82Sh20 82Sh20

(6Li,t)

4°Ca(SLi,t),E=156 MeV; m e a s u r e d

~(6) v e r s u s

82Ne02

(eLi,3He) ¢°Ca(SLi,3He),E=156 MeV; m e a s u r e d

a(O) v e r s u s

82Ne02

(SLi,a) *°Ca(~Li,(x),E=156 MeV; m e a s u r e d

cr(O) v e r s u s

82Ne02 (6Li,na)

SeSe(eLi,n~),E=27

MeV; m e a s u r e d

E-/,17(O),a(E,ET),

82Ze02

(aLl,SHe) Z~Mg(eLi,SHe),E=34 MeV; m e a s u r e d a*Mg(°Li,SHe),E=34 MeV; m e a s u r e d

a(E(aHe),0). cr(E(eHe),0).

82Ci01 82Ci01

27AI(~Li,aHe),E=34 MeV; m e a s u r e d

a(E(SHe),O).

82Ci01

(SLi,°Li) 4°Ca(~Li,%i),E=26,30 MeV; m e a s u r e d

a(O).

82Co12

~ l V ( p o l a r i z e d eLi,SLi),E=9.8,12,14 MeV; m e a s u r e d

82Mo17

(SLi,SLi') 4°Ca(SLi,SLi'),E=30 MeV; m e a s u r e d

or(O).

82Co12

(SLi,SB) SLi(SLi?B),E=72 MeV; m e a s u r e d cr(E(SB)),cr(O). IZC(SLi,eB),E=72 MeV; m e a s u r e d cr(E(eB)),a(O). 9°Zr(eLi,SB),E=90 MeV; m e a s u r e d (~(E(SB)),cr(O). SZZr(SLi,SB),E=90 MeV; m e a s u r e d o'(E(aB)),o*(O). g4Zr(eLi,SB),E=90 MeV; m e a s u r e d o'(E(SB)),cT(0).

9eMo(SLi,SB),E=90 S4Mo(aLi,SB),E=90 SSMo(OLi,aB),E=90 9SMo(SLi,eB),E=90 t°OMo(SLi,aB),E=90

82A108 82A108 82TiO1 82TiO1 82TiO1

MeV; MeV; MeV; MeV; MeV;

measured measured measured measured measured

a(E(SB)),a(0). ¢r(E(SB)),(~(O). (7(E(SB)),(7(O). ¢r(E(SB))Jr(O). cr(E(SB)),a(8).

82TiO1 82Ti0I 82TiO1 82Ti01 82Ti01

(SLi,xn) ~asHf(SLi,xn),E=55-124 MeV; m e a s u r e d - / ( X - r a y ) - , l S t T a ( S L i , x n ) , E = 5 5 - 1 2 4 MeV; m e a s u r e d ~ ( X - r a y ) - , 181Ta(SLi,xn),E=74.8 .... MeV; m e a s u r e d K X - r a y IBSW(SLi,xn),E=55--124 MeV; m e a s u r e d - / ( X - r a y ) - , LaSRe(SLi,xn),E=55-124 MeV; measured -/(X-ray)-, IS~Re(6Li,xn),E=55-t24 MeV; measured -/(X-ray)-, 1~4Pt(SLi,xn),E=55-124 MeV; measured -/(X-ray)-, lg4Pt(SLi,xn),E=74.8 .... MeV; m e a s u r e d K X - r a y

tSapt(sLi,xn),E=74.8,... laTAu(OLi,xn),E=55-124 tOTAu(SLi,xn),E=74.8 .... 82Vi02 S°STl(OLi,xn),E=55-124 82Ka05 a°STl(SLi,xn),E=55-124 82Ka05 2°Spb(SLi,xn),E=55-124 82Ka05 2°8Pb(SLi,xn),E=74.8,... 82Ka05 2°sBi(aLi,xn),E=55-124 82Vi02 continued 82Ka05 82Ka05

125

Me¥; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d Me'q; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

K X-ray 7(X-ray)-, K X-ray T(X-ray)-, T(X-ray)-, -/(X-ray)-, K X-ray -/(X-ray)-,

82vio2 82Ks05 82Vi02 82Ka05 82Ka05 82KaO5 82Vi02 82Ka05

REACTION

(eLi,xn) Xaapt(sLi,xn),E=55-124

MeV; m e a s u r e d

7(X-ray)-,

INDEX

continued

82ga05

(SLi,F) IaITa(SLi,F),E=74.8,... MeV; m e a s u r e d t a a p t ( a L i , F ) , E = 7 4 . 8 .... MeV; m e a s u r e d 1aapt(aLi,F),E=74.8,... MeV; m e a s u r e d

82Vi02 82Vi02 82Vi02

IaTAu(aLi,F),E=74.8,... MeV; m e a s u r e d ~ ° s P b ( a L i , F ) , E = 7 4 . 8 .... MeV; m e a s u r e d

82Vi02 82Vi02

(SLi,X) JZC(aLi,X),E=10-36 MeV; m e a s u r e d a(fragment 0,E), I a C ( S L i , X ) , E = 9 . 2 3 - 3 5 . 0 8 MeV; m e a s u r e d S ~ V ( p o l a r i z e d S L i , X ) , E = I 0 - ~ 0 MeV; m e a s u r e d E5',13', l a l T a ( % i , X ) , E = 7 4 . 8 .... MeV; m e a s u r e d

82De30 82De30 82Mo17 8~Vi02

la4pt(sLi,X),E=74.8 .... MeV; ~gsPt(SLi,X),E=74.8 .... MeV; 197A u(SLi,X),E=74.8 .... MeV; a°aPb(aLi,X),E=74.8.... MeV;

measured measured measured measured

82Vi02 82Vi02 82Vi02 82Vi02

(SLi,pX) 181Ta(eLi,pX),E=94.4,74.8 MeV; m e a s u r e d l a 4 P t ( S L i , p X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d t a a P t ( S L i , p X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

inclusive inclusive inclusive

8~Vi02 8~Vi02 82Vi02

l ~ T A u ( S L i , p X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d ~ ° a p b ( S L i , p X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

inclusive inclusive

82¥i02 82Vi02

inclusive inclusive inclusive

82Vi02 82Vi02 82Vi02

inclusive inclusive

82Vi02 82Vi02

inclusive inclusive

82Vi02 82Vi02

77-coin,IT,ET,

82Ba25

(SLi,dX) laC(eLi,dX),E=34 MeV; m e a s u r e d a(O,Ed) i n c l u s i v e . l a l T a ( e L i , d X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d inclusive l g 4 p t ( s L i , d X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d inclusive

82Cu02 82vi02 8~Vi02

1 9 a p t ( s L i , d X ) , E = 9 4 . 4 ; 7 4 . 8 MeV; m e a s u r e d ~eTAu(SLi,dX),E=94.4,74.8 MeV; m e a s u r e d ~ ° e P b ( S L i , d X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

(SLi,tX) lelTa(eLi,tX),E=94.4,74.8 194Pt(%i,tX),E=94.4,74.8 laaPt(SLi,tX),E=94.4,74.8

MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

inclusive inclusive inclusive

8~Vi02 82Vi02 82Vi0~

19VAu(SLi,tX),E=94.4,74.8 MeV; m e a s u r e d Z a s P b ( a L i , t X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

(SLi,aX) lSlTa(eLi,(xX),E=94.4,74.8 MeV; m e a s u r e d l a 4 P t ( S L i , a X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d 1 9 a P t ( a L i , a X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

inclusive inclusive inclusive

82vi02 82Vi0~ 82Vi0~

1 9 7 A u ( a L i , a X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d 2 ° s P b ( e L i , a X ) , E = 9 4 . 4 , 7 4 . 8 MeV; m e a s u r e d

(VLi,n) I H ( T L i , n ) , E = 1 3 . 1 5 - 2 2 MeV; m e a s u r e d

cr(0) v s E.

8~Da21

(TLi,p) Sly(polarized

~Li,p),E=12,20 MeV; m e a s u r e d

er(0),

81K04~

(TLi,2n) 4°Ca(TLi,2n),E=14

MeV; m e a s u r e d

45V y i e l d .

82Holl

S4Ni(~Li,2n),E=14-18

MeV; m e a s u r e d

(TLi,np) t2C(VLi,np),E=10.7.12.3 MeV; m e a s u r e d r e l a t i v e l e O ( ~ L i , n p ) , E = l l . 8 MeV; m e a s u r e d relative

8IXe01 81XeOl

6*Zn(TLi,np),E=16.2 MeV; m e a s u r e d

relative

81Xe01

(TLi,d) J~C(VLi,d),E=10.7,12.3 MeV; m e a s u r e d r e l a t i v e l e 0 ( T L i , d ) , E = l l . 8 MeV; m e a s u r e d relative

81Xe01 81Xe01

a4Zn(TLi,d),E=16.2 MeV; m e a s u r e d

126

relative

81Xe01

REACTION

INDEX

(TLi,nd) t°aMo(~Li,nd),B=48 MeV; m e a s u r e d E3~,I"/,3")'-,

82Ha13 (7Li,2np)

~°°Mo(VLi,2np),E=4B

MeV; m e a s u r e d E'y,I~,~T-,

82Ha13

ffLi,t) ~ V ( p o l a r i z e d 7Li,t),E=12,2O

MeV; m e a s u r e d or(0),

81Ko42

1S°Mo(~bi,t),E=48

MeV; m e a s u r e d E'y,I%~'7-,

82Ha13

(TLi,4n) SZSe(TLi,4n),E=3R.5 MeV; m e a s u r e d E3,,I~(0),a(E,E'y) H~Cd(~bi,4n),E=32-50 MeV; m e a s u r e d E~/,I~,~(t),

82Ze02 B2Dull

llsCd(¢Li,4n),E=32-50 MeV; m e a s u r e d ET,IT,T(t), 176Yb(TLi,4n),E=35-45 MeV; m e a s u r e d t~7,1~,

82Dull 82Ba21

(7Li,2nt) ~54Sm(TLi,2nt),E=41~ MeV; measured E'],17,77-,

B2Hal3 (TLi,3nd)

154Sm(TLi,3nd),E=48 MeV; measured ET,17,qT-,

82Ha13 (TUi,4np)

lS4Sm(TLi,4np),E=413

MeV; m e a s u r e d E~/,I~/,~-/-,

82Ha13 (TLi,2na)

SaSe(TLt,2na),E=32.5 MeV; m e a s u r e d E~/,I~/(O),

82Ze02 (7Li,TLi)

~aSi(~Li,TLi),E=45 MeV; m e a s u r e d (~(0). 4°Ca(TLi,TLi),E=45 MeV; m e a s u r e d a(0). 5iV(polarized 7Li,TLi),E(cm)=8.5-17.5 MeV;

82Ee01 82EeOI 81Ko42

SlV(polarized ~Li,TLi),E=I0--20 MeV; m e a s u r e d ET,]7 ~SNi(polarized 7Li,TLi),E~I4.2,... MeV; m e a s u r e d

82Mo17 82Mo13

(7Li,TLi ') eSSi(TLi,TLi'),E=45 MeV; m e a s u r e d a(0). ~°Ca(VLi,TLi'),E=45 lVIeV; m e a s u r e d a(0).

82EeOI 82EeOl

58Ni(polarized 7Li,TLi'),E=20.3

MeV; m e a s u r e d a(e)

82Mot3

(TLi,SLi) a°aPb(?Li,SLi),E=52 MeV; m e a s u r e d a(0).

82Le14 (TLI,8B)

SBe(?Li.SB),E=83 MeV; m e a s u r e d a(E(SB)),cr(0).

82A108

12C(TLi,SB),•=83 MeV; m e a s u r e d a(E(SB)),cr(O).

82AI08

(7Li,xn) iSOHf(TLi,xn),E=55-124 lalTa(TLi,xn),E=55-1E4 lSSw(~Li,xn),E=55-124 lSSRe(~Li,xn),E=55-124 lSVRe(TLi,xn),E=55-124 lSapt(TLi,xn),E=55-124

MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

3,(X-ray)-, 7(X-ray)-, ~/(X-ray)-, "y(X-ray)-, ~(X-ray)-, -~(X-ray)-,

8gKa05 82Ka05 82KaO5 82Ka05 82Ka05 82Ka05

ISapt(~Li,xn),E=55-124 MeV; m e a s u r e d -y(X-ray)-, 19VAu(TLi,xn),E=55-124 MeV; m e a s u r e d ~ ( X - r a y ) - , Z°aTl(TLi,xn),E=55-124 MeV; m e a s u r e d ~/(X-ray)-, Z°STl(TLi,xn),E=55-/fi4MeV; n~easured ~/(X-ray)-, Z°sPb(~Li,xn),E=55-124 MeV; m e a s u r e d - / ( X - r a y ) - , Z°SBi(~Li,xn),E=55-124 MeV; m e a s u r e d "y(X-ray)-,

(TLi,xnp) S4Zn(TLi,xnp),E=15-1~I MeV; m e a s u r e d ET,I'y(0),DSA.

82Pa03

127

82Ka05 82Ka05 82Ka05 B2Ka05 82Ka05 82Ka05

REACTION INDEX

(TLi,X) *ZC(VLi,X),E=10-38 MeV; m e a s u r e d <7(fragment 0,E), 13C(rLi,X),E=10-34 MeV; m e a s u r e d <7(fragment 0,E), 5~V(polarized 7Li,X),E(cm)=8.5-17.5 MeV; m e a s u r e d

82D e 30 82De30 81Ko42

~lV(polarized 7Li,X),E=IO-20 MeV; m e a s u r e d E7,I7, ~SFe(TLi,X),E n o t given; measured residuals

82Mo17 82Pa19

(~Be,p) 12C(~Be,p),E(em)=5.9-15.4 MeV; m e a s u r e d <7(0) vs E.

82Hu06

(gBe,d) 12C(SBe,d),E(cm)=5.9-15.4 MeV; m e a s u r e d <7(8) vs E.

82Hu06

(gBe,3n) 4°Ar(SBe,3n),E=20 MeV; m e a s u r e d 77-coin,DSA.

82Ra01

(gBe,t) ~eC(SBe,t),E(cm)=5.g-15.4 MeV; m e a s u r e d <7(8) vs E.

82Hu06

(gBe,a) *eC(SBe,cQ,E(em)=5.9-15.4 MeV; m e a s u r e d <7(e) vs E.

82Hu06 (SBe,SBe)

iZC(9Be,SBe),E(em)=5.9-15.4 MeV; m e a s u r e d a(8) vs

82Hu06 (gBe,°Be)

12C(9Be,SBe),E(em)=5.9-15.4 MeV; m e a s u r e d <7(8) vs

82Hu06 (l°B,np)

58Ni(t°B,np),E=31 MeV; measured

E7,17,7(@),

82So04

(~°B,Sn)

ZOSTl(i°B,5n),E ~ 70 MeV; m e a s u r e d 7 ~ / - , n T - c o i n ,

82Po03

(I°B,°B) ~°sPb('°B,gB),E=3Z-38 MeV; m e a s u r e d <7(g(*°B)),

82Ve 11 (l°B,l°B)

13C(Z°B,J°B),E=18 .... MeV; m e a s u r e d Z4Mg(t°B,i°B),E=87.5 MeV; m e a s u r e d a(O).

82Ma20 82Fu09

ZSMg(t°B,t°B),E=87.5 MeV; m e a s u r e d ~(0). 6°Ni(1°B,I°B),E=87.5 MeV; m e a s u r e d a(O).

82Fu09 82Fu09

(loB,loB,) Z4M~(1°B,*°B'),E=87.5 MeV; m e a s u r e d o-(e). S°Ni(i°B,l°B'),E=87.5 MeV; m e a s u r e d a(e).

z°epb(*°B,*°B'),E=32-38

82Fu09 82Fu09

(I°B,*'B) ZQsPb(*°B,IIB),E=32-38 MeV; measured

<7(E(*°B)),

82Veil O°B,X)

t3C(I°B,X),E=I4-48 MeV; m e a s u r e d <7(fragment O,E)

82Ma20

128

MeY; measured

(7(E(I°B)),

82Yell

REACTION

INDEX

(lIB,4n) tagLa(lXB,4n),E=54 MeV; m e a s u r e d

ET,IT,reeoil.

82Ro05

('lB,na) teC(i~B,na),E=32 MeV; measured E3,,17,DSA,recoil.

82Ko24

(IIB,6Li) a~Mg(ttB,SLi),E=79.6 Me'V; m e a s u r e d

tr(0) vs

82Fu09 (llB,TLi)

e~Mg(ttB,'rLi),E=79,6 MeV; m e a s u r e d

a(O) vs

82Fu09 (IIB,7Be)

e~Mg(~B,TBe),E=79.6 MeV; m e a s u r e d

or(0) v s

82Fu09 (llB,SLi)

e~Mg(ilB,eLi),E=79.6 MeV; m e a s u r e d

a(0) v s

82Fu09

(IlB,SBe) eeMg(ttB,SBe),E=79.6 MeV; m e a s u r e d

o'(0) v s

82Fu09

(llB,l°Be) e~Mg(tlB,t°Be),E=79.6 MeV; m e a s u r e d

a(0) v s

82Fu09

(11B,'oB) ZSMg(t~B,~°B),E=79.6 MeV; m e a s u r e d

a(0) v s

82Fu09

(lIB,i'B) taC(llB,ttB),E=~5,40,50 MeV; m e a s u r e d e4Mg(HB,nB),E=79.5 MeV; m e a s u r e d a(O). eSMg(nB,nB),E=79.5 MeV; m e a s u r e d tr(O). ZSMg(IiB,IIB),E=79.5 MeV; m e a s u r e d ~(0). 26Mg(nB,nB),E=79.6 MeV; m e a s u r e d 0"({9) v s

82Ma20

27Al(nB,nB),E=79.5 MeV; m e a s u r e d or(0). ~gCo(ttB,I1B),E=79.5 MeV; m e a s u r e d or(e). °°Ni(I{B,nB),E=79.5 MeV; m e a s u r e d ~(0). ~STAu(nB,nB),E~79.5 MeV; m e a s u r e d tx(0).

82Fu09 82Fu09 82Fu09 82Fu09

82Fu09 82Fu09 B2Fu09 83Fu09

("S,'IB') e4Mg('IB,1*B'),E=79.5 MeV; m e a s u r e d

a(0).

8ZFu09

ZeMg(nB,nB'),E=79.5 MeV; m e a s u r e d

(lXB,laC) ZSMg(nB,I~C),E=79.6 MeV;

measured

o'(O) vs

8~Fu09

("B,~2B) aSMg(nB,12B),E=79.6 MeV;

measured

0.(0) v s

82Fu09

("B,'2C) Z°Mg(nB,laC),E=79.6 /~[eV; m e a s u r e d

o'(0) vs

82Fu09

(l~B,13C) ZSMg(~lB,~aC),E=79.6 MeV; m e a s u r e d

o'(0) v s

82Fu09

129

~(0).

82Fu09

REACTION

INDEX

(nB,xn) taaNd(llB,xn),E=50-68 MeV; m e a s u r e d

E~,IT,

8~Be46

IS°Nd(11B,xn),E=50-68 MeV; m e a s u r e d E~/,17,

82Be46

("B,X) ~ZC(nB,X),E=I4-54 MeV; m e a s u r e d a ( f r a g m e n t

0,E)

8~MaSO

(~2c,?) ~He(I~C,7),E(em)=l.44-3.38 MeV; m e a s u r e d G(E,E(3,))

82K e 10

SSNi(leC,'y),E=30-42 MeV; m e a s u r e d

E(X-ray),

82Se05

(*aC,p) ~Be(lZC,p),E(cm)=6-15 MeV; m e a s u r e d G(O,E). tZC(leC,p),E(cm)=2.8-6.3 MeV; m e a s u r e d G(0,E).

81Hul2 81Be60

ISeW(~SC,p),E=77-167

MeV; measured

a(E),a(fission)

82Ra06

(12C,2n)

8SZn(IZC,2n),E=39 SSZn(~SC,gn),E=36

MeV; measured MeV; measured

E)',Iv,~'(0),recoil, ET,lT,DSA,77-eoin.

~Zc(~SC,np),E=16,19,24 MeV; m e a s u r e d relative lSO(~ZC,np),E=32.1 MeV; m e a s u r e d r e l a t i v e tgF(tZC,np),E=20.1 MeV; m e a s u r e d r e l a t i v e

82PiOl 8~An06

J°spd(I~C,Sn),E=58 MeV; m e a s u r e d

77-eoin,T(O),

82ChO1

81Xe01 81Xe01 81Xe01

Z4Mg(lZC,npv),E=32-35 MeV; m e a s u r e d G(E%0), 2aSi(leC,np),E=16.5,19.5 MeV; m e a s u r e d r e l a t i v e 2SSi(laC,np),E=24 MeV; m e a s u r e d r e l a t i v e

82Va02 81XeO1 81XeO1

(12C,d) 9Be(tZC,d),E(cm)=6-15 MeV; m e a s u r e d (r(0,E). ~zC(tzC,d),E=16,19,24 MeV; m e a s u r e d r e l a t i v e

81Hul~ 81Xe01

2eSi(tzC,d),E=16.5,19.5 MeV; m e a s u r e d r e l a t i v e ~ezW(lzC,d),E=77-167 MeV; measured a(E),a(fission)

81XeOl 82Ra06

(12e,sp) 5SNi(~ZC,Sp),E=40

MeV; m e a s u r e d ET,IT,73'(O,H).

82Ba42 (12C,3n)

l°aRh(lzC,3n),E=50 MeV; m e a s u r e d IT(0,t,H). ttocd(l~C,3n),E=52-75 MeV; m e a s u r e d a(E,E~,0), llzCd(laC,3n),E=52-75 MeV; m e a s u r e d ~r(E,ET,O),

82Ma29 82Ba31 82Ba31

144Sm(IaC,3n),E=53-65 MeV; m e a s u r e d E~',IT(E),IT(t) la~Sm(laC,3n),E ~ 76 MeV; m e a s u r e d ET,IT,T(O),

8~Ca09 82Fo06

(IZC,2np)

4aTi(leC,Enp),E=39

MeV; measured

7-spectra,recoil.

aSKeD7

7aGe(12C,Snp),E=33-48 MeV; m e a s u r e d E(7),I(E(7)),

82Pa20

(IZc,t) gBe(12C,t),E(cm)=6-15 MeV; m e a s u r e d

~(@,E).

81Hul2

*SaW(12C,t),E=77-167

MeV; measured

a(E),q(fission)

82Ra06

(lZC,4n) 76Ge(~aC,4n),E=48-60 MeV; m e a s u r e d ET,lT,TT--eoin,

82D e 05

197Au(12C,4n),E=77 MeV; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) , 7 ( t )

8aSj01

('ec,~) aBe(JSC,a),E(em)=6-15 MeV; m e a s u r e d q(O,E). IeC(12C,a),E(em)=2.8-6.3 MeV; m e a s u r e d ~(O,E). I~C(12C,a),E=30 MeV; m e a s u r e d G(E(a),O(al)), laC(lZC,a),E(em)=22--28 MeV; m e a s u r e d a(O,E). taC(~ZC,a),E=33-44 MeV; m e a s u r e d g(0) vs E. laC(laC,a),E=29.5-30.5 MeV; m e a s u r e d cr(O),a(E).

81Hul2 81Be60 81G a 35 81Ho30 82Fo03 82Ka17

12C(laC,ot),g=32.fi,33.5 MeV; m e a s u r e d G(ET,0), e4Mg(lZC,a),E=fil.8-26 MeV; m e a s u r e d a(O=5°,E). e4Mg(12C,a),E(cm)=ll.9-16.1 MeV; m e a s u r e d a(E). e4Mg(~eC,a),E=a4-36 MeV; m e a s u r e d a(Ea),a(O) ve E. lsaW(tZC,~),E=77-167 MeV; m e a s u r e d cr(E),~(fission)

130

82Sp02 8lAb07 81Ca16 82DalO 82Ra06

REACTION

INDEX

(IZC,5n) ~a°Ce(lZC,5n),E=96 MeV; m e a s u r e d ET,l-~,77-coin,

82Br13

('2C,n~) 4°Ca(~ZC,n~x),E=38 MeV; m e a s u r e d

~rT-coin,-),7(t).

82Ha36

4eTi(l~C,na),E=39 MeV; m e a s u r e d 7 - s p e c t r a , r e c o i l .

82Ke07

(laC,6n) ~4aSm(laC,6n),E=120 MeV; m e a s u r e d E7,I7,77-,

82Mo19

(laC,2na) ~SGe(~ZC,2na),E=42-52 MeV; m e a s u r e d ET,17,recoil.

82Br05

('2C,°Be) OBe(tZC,SBe),E(cm)=:6-15 MeV; m e a s u r e d (~(O,E). ~C(I2C,aBe),E=68-80 MeV; m e a s u r e d ac~-eoin.

81Hu12 81A126

'2C(iac,SBe),E(cm)=22-28 MeV; measured ~(O,E).

81Ho30

(12C,"C) ~eC(~eC,HC),E=49 .... MeV; m e a s u r e d

a(O).

U°spb('~C,3a),E=187 MeV; m e a s u r e d a ( E a ) , a a - c o i n ,

79Ch42

82Sh01

('2C,12C) 4He(12C,ISC),E=5.6-:L3.7 MeV; m e a s u r e d cr(E,O). SBe(leC,leC),E(cm)=6-15 MeV; m e a s u r e d a(O,E). nB(leC,lzC),E(cm)=L4.6 MeV; m e a s u r e d a(O). C(~UC,13C),E-0.3-0.4 MeV; m e a s u r e d o p t i c a l CP, tZC(12C,IzC),E=49 .... MeV; m e a s u r e d or(O). IeC(~2C?zC),E=I20-290 MeV; m e a s u r e d (r(O) vs ~eC(leC,leC),E=l.O16 GeV; m e a s u r e d a(O). leC(lzC,lee),E(cm)=25.2 MeV; m e a s u r e d (leC)(lSc)-,

82K e l O 81Hu12 81Hu13 82Lu02 79Cb42

'2C(IeC,JzC),E=240,300 MeV; m e a s u r e d cr(O),•(total) ~4Mg(x2c,IZC),E=20-60 MeV; m e a s u r e d eY(elastic), eSMg(IZC}eC),E=20-56 MeV; m e a s u r e d a ( e l a s t i c ) , °3Cu(12C,lzC),E=45 MeV; m e a s u r e d a(E(12C)), e4Zn(t2C,12C),E=45,54,6(} MeV; m e a s u r e d a(E(leC)), SSSr(lZC,laC),E=80 MeV; m e a s u r e d a(O),o(E(*2C)), a°spb(leC,laC),E=sub-Coulomb; m e a s u r e d cr(Ol)/a(Oz)

81Co22 82Bu17

82Vo04 82Da09 82Da09 82Vo03 82Be15 821n01 82Ly02

82Me05

(i2C,lzC,) ~Zc(lZc,*ZC'),E=49 .... MeV; m e a s u r e d a(O). l~C(zeC,lzC'),E(cm)=15-35 MeV; m e a s u r e d cr(O=90°,E) leC(12C,12C'),E(cm)=15-35 MeV; m e a s u r e d a ( t o t a l ) , leC(leC,l~C'),E(cm)=25.2 MeV; m e a s u r e d (IZC)(*zC)-

79Ch42 81Tr09 81Tr09 82Me05

63Cu(ZZc,leC'),E=45 MeV; m e a s u r e d a(E(leC)), eeSr(leC,leC'),E=80 MeV; m e a s u r e d a(O),a(E(*2C)), 2°apb(luC,12C'),E=132 .... MeV; m e a s u r e d ~(0).

('2C)3C) SSSr(~2C,~3C),E=80 MeV; m e a s u r e d q(O),a(E(12C)),

821noi

12C(IzC}3N),E=49 .... MeV; m e a s u r e d

79Ch42

a(O).

('2C)~N) nB('2c,lsN),E(cm)=9.8-17.2 MeV; m e a s u r e d a(E).

8LFr26

(12c,1S0) i1B(lzC,ieO),E(em)=9.8 17.2 MeV; m e a s u r e d or(E).

81Fr26

131

82Vo03 821n01 82Sh21

REACTION

INDEX

(~c,~sF) nB(ieC,~eF),E(cm)=9.8-17.~ MeV; m e a s u r e d a(E).

81Fr26

(~ec,e~Ne) UB(leC,a~Ne),E(cm)=9.8-17.2 MeV; m e a s u r e d a(E).

81Fr26

('eC,xn) i~°Pd(~aC,xn),E n o t nlsn(~aC,xn),E=ll8 nSSn(~aC,xn),E=ll8 neSn(*aC,xn),E=ll8 laSSn(laC,xn),E=ll8 *aaSn(laC,xn),E=ll8

given; m e a s u r e d n e u t r o n MeV; m e a s u r e d 7 7 - c o i n . MeV; m e a s u r e d 7 7 - c o i n . MeV; m e a s u r e d 7 7 - c o i n MeV; m e a s u r e d 7 T - c o i n . MeV; m e a s u r e d 7 7 - c o i n .

82Ja01 83Li05 82Li05 82Li05 82Li05 82Li05

lZ4Sn(leC,xn),E n o t gi ve n; m e a s u r e d n e u t r o n lS°Te(laC,xn),E not g i v e n ; m e a s u r e d n e u t r o n 14SNd(12C,xn),E=80-110 MeV; m e a s u r e d ES',IT(0),a tSONd(12C,xn),E=80-110 MeV; m e a s u r e d ET,IT(0),a 144Sm(12C,xn),E n o t g i v e n ; m e a s u r e d %/e,ET,17, 14~Sm(L2C,xn),E n o t g i v e n ; m e a s u r e d TI/2,ET,I 7,

82Ja01 82Ja01 82Lu03 82Lu03 82To14 82To14

(JeC,xn~) n4Sn(*aC,(xxn),E=ll8 MeV; m e a s u r e d 7 7 - c o i n . nSSn(*eC,cxxn),E=ll8 MeV; m e a s u r e d 7 7 - c o i n . nSSn(lZC,(xxn),E=ll8 MeV; m e a s u r e d 7 7 - c o i n .

82Li05 82Li05 82Li05

12°Sn(laC,c(xn),E=l18 MeV; m e a s u r e d 7 T - c o i n . lZesn(laC,(~xn),E=ll8 MeV; m e a s u r e d 7 7 - c o i n . iS°Nd(12C,xna),E=80-110 MeV; m e a s u r e d (x f o r x = 4 - 6 .

82Li05 82Li05 82Lu03

('aC,xnyp) Fe(lZC,xnyp),E=48 MeV; m e a s u r e d ET,17,7(t), S~Co(i2C,xnyp),E=48 MeV; m e a s u r e d ET,lT,7(t), ~°Ni(~aC,xnyp),E=48 MeV; m e a s u r e d ET,IT,7(t), SSCu(i~C,xnyp),E=48 MeV; m e a s u r e d ET,17,7(t), S~Cu(*eC,xnyp),E=48 MeV; m e a s u r e d ET,17,7(t), S~Y(~eC,xnyp),E=48 MeV; m e a s u r e d ET,17,7(t),

82An09 82An09 82A n09 82An09 82An09 82An09

9°Zr(laC,xnyp),E=48 ~lZr(laC,xnyp),E=48 SeZr(lZC,xnyp),E=48 93Nb(lZC,xnyp),E=48 95Mo(12C,xnyp),E=48

MeY; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

ET,17,T(t), ET,lT,7(t), ET,I%7(t), ET,17,7(t), ET,lT,7(t),

82An09 82An09 83An09 82An09 82An09

('aC,F) Ni(1aC,F),E=30-84 M e V / n u c l e o n ; m e a s u r e d a(0,,Oa) ~8~W(*eC,F),E=77-167 MeV; m e a s u r e d a ( E ) , a ( f i s s i o n ) Au(*eC,F),E=30-84 M e V / n u c l e o n ; m e a s u r e d a(0,,0a) ~Au(~ZC,F),E=72.5 MeV; m e a s u r e d f r a g m e n t *~TAu(*eC,F),E=72.5 MeV; m e a s u r e d

Pb(IZC,F),E=72.5 MeV; m e a s u r e d a°SBi(12C,P),E=72.5 MeV; m e a s u r e d U(IzC,F),E=30-84 M e V / n u c l e o n ; m e a s u r e d a(01,0~) e~SU(IZC,F),E=81 MeV; m e a s u r e d ~ ( f r a g m e n t O).

82Ga15 82Ra06 82Ga15 79Su15 80Yu01

80YuOI 80Yu01

82Ga15 82Bu06

('2C,X) teC(~eC,X),E=4.2-7 MeV; m e a s u r e d a ( f u s i o n ) vs E. 13C(*~C,X),E=3.1-6.7 MeV; m e a s u r e d a ( f u s i o n ) vs E. a°Ne(leC,X),E(em)=ll-33 MeV; m e a s u r e d E7,I7. 2~Mg(*ZC,X),E=20-63 MeV; m e a s u r e d a ( f u s i o n ) vs E. a4Mg(*eC,X),E=20-60 MeV; m e a s u r e d a ( e l a s t i c ) , a~Mg(~ee,x),R(cm)=16.4-29.8 MeV; m e a s u r e d e~Mg(*ZC,X),E=20-56 MeV; m e a s u r e d a ( e l a s t i c ) , aSSi(IeC,X),E(cm)=18.4-35 MeV; m e a s u r e d E7,17, 4°Ti(*~C,X),E=21-57 MeV; m e a s u r e d p r o d u c t i o n a(E) S*V(*ZC,X),E n o t g i v e n ; m e a s u r e d r e s i d u a l s Cu(*ec,x),E=86 M e V / n u c l e o n ; m e a s u r e d c u m u l a t i v e , Ag(*eC,X),E=84 M e V / n u c l e o n ; m e a s u r e d Ag(~eC,X),E=86 M e V / n u c l e o n ; m e a s u r e d p r o d u c t UaSn(*aC,X),E=84 M e V / n u c l e o n ; m e a s u r e d USSn(*eC,X),E=84 M e V / n u c l e o n ; m e a s u r e d l~48n(~C,X),E=84 M e V / n u c l e o n ; m e a s u r e d

82D a 16 82D a 16 82De10 82D a 09 82D a 09 82G a 09 82Da09 82Le04 81Ca17 8~Pa19 82Lu04 81Bl15 82Lu05

Dy(*ZC,X),E=l GeV; m e a s u r e d p r o d u c t i o n (;(E) f o r Ho(lZC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r Er(LaC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r Tm(IeC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r 189Tm(12C,X),E=l GeV; m e a s u r e d a ( f r a g m e n t O), Yb(*2C,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r 17eyb(1aC,X),E=l GeV; m e a s u r e d a ( f r a g m e n t 0), Ta(12C,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r IetTa(IaC,X),E=I GeV; m e a s u r e d o r ( f r a g m e n t 0), *BaW(IZC,X),E=I GeV; m e a s u r e d a ( f r a g m e n t e),r~ecoi] IeOw(12C,X),E=l GeV; m e a s u r e d ( ; ( f r a g m e n t e),recoil Pt(IaC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r Au(*eC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r Pb(IaC,X),E=I GeV; m e a s u r e d p r o d u c t i o n a(E) f o r U(12C,X),E=936 MeV; m e a s u r e d a b s o l u t e , c o m p a r a t i v e

81BI15 81BI15 81BI15

(12C,pX) S°Ni(iZC,pX),E=90 .... MeV; m e a s u r e d a(Op),a(Od),

82Au04

(12C,dX) SONi(*eC,dX),E=90 .... MeV; m e a s u r e d a(Op),a(Od),

82Au04

132

82Du15 82Du15 82Du15 83Du15 82Du02 82Du15 8RDu02 82Du15 82Du02 82Du02 82Du02 82Du15

82Du15 8~Du15 81Bj04

REACTION

INDEX

(laC,tX) 6°Ni(lZc,tX),E=90 .... MeV; m e a s u r e d

a(Op),a(0d),

82Au04

(tZC,3HeX) 9ONi(IZC,3HeX),E=90 .... MeV; m e a s u r e d

a(Op),a(Od),

82Au04

(lZC,aX) cr(Op),a(Od),

6°Ni('ZC,aX),E=90 .... MeV; m e a s u r e d

82Au04 (t3C,3n)

l l ° P d ( 1 3 C , 3 n ) , E = 4 0 .... MeV; m e a s u r e d 77-coin,7(0), tOSAg(13C,3n),E=52 MeV; m e a s u r e d IT(0,t).

83Ch01 82Da17

u ° C d ( 1 3 C , 3 n ) , E = 5 2 MeV; m e a s u r e d

77-coin,7(0),

82Ch01

G(E(JzC)),

82Vo03

~r(E(laC)),

82Vo03

(*3< 0 6Li(lSC,t),E=54.2

NeV; m e a s u r e d

cr(Et),(r(0).

82Ab02

(13c,~) -~ZC(13C,aT),E=19.7 MeV; m e a s u r e d

aT-coin,DSA.

81An21

(13C,lzC) 4eTi(IaC,IaC),E=25-60

MeV; m e a s u r e d

(r(E).

81Ri13

(13C,13C) C(13C,13C),E=0.3-0.4

MeV; m e a s u r e d

optical

CP,

82Lu02

63Cu(IaC,t3C),E=45 MeV; m e a s u r e d

('3C,'3C,) 4eTi(13c,lSc'),E=25-60

MeV; m e a s u r e d

o'(E).

eacu(Iac,IaC'),E=45MeV; m e a s u r e d

8lRil3

('3c,x) 13C(13C,X),E(em)=4-15.8 MeV; m e a s u r e d a(E,ET). ~eTi(laC,X),E=36,46,56 MeV; m e a s u r e d or(E) f o r 47Ti(13C,X),E=36,46,56 MeV; m e a s u r e d a(E) f o r 48Ti(13C,X),E=46 MeV; m e a s u r e d (particle)7-coin.

83Ch05

48Ti(IaC,X),E=36,46,56 MeV; measured (r(E) for

82Do03 82Do03 81Du21

4STi(13C,X),E=36,46,56 MeV; m e a s u r e d 5 ° T i ( l a c , x ) , E = 3 6 , 4 6 , 5 6 MeV; m e a s u r e d

or(E) f o r a(E) for

82Do03 82Do03 82Do03

o'(O),cr(E(160)).

82Ma30

cr(0),a(E(lSO)).

82Ma30 8~Ma30

(14C,12Be) t~C(14C,laBe),E=50-63

MeV; m e a s u r e d

a(0)

v s E,

82Be42

(~4C,'4C) 92Mo(14C,~4C),E=71 MeV; m e a s u r e d

(r(O),a(E(160)).

8EMa30

I°°Mo(14C,t4C),E=71 MeV; m e a s u r e d

('4c,14c,) t 4 C ( l a C , I 4 C ' ) , E ( e m ) = 1 2 . 5 - 3 2 . 5 MeV; m e a s u r e d o'(E), 1 4 C ( 1 4 C , t 4 C ' ) , E ( c m ) = l S - 3 5 MeV; m e a s u r e d cr(0=90°,E)

9ZMo(14C,14C'),E=71 MeV; m e a s u r e d 10°Mo(14C,14C'),E=71 MeV; m e a s u r e d

81Be64

81Tr09

(r(O),o'(E(laO)).

(14C,'60) 79Zn(14C,160),E=72 MeV; m e a s u r e d SZMo(14c,tSO),E=71 MeV; m e a s u r e d 94Mo(14c,l°O),E=71 MeV; m e a s u r e d

if(O). a(O),a(E('60)). o'(O),a(E(tSO)).

9eMo(14C,'eO),E=7l MeV; m e a s u r e d o'(O),o-(E(~sO)). 9eMo(14C,leO),E=71 MeV; m e a s u r e d o'(O),(r(E(IsO)). t°°Mo(14C,lS0),E=71 MeV; m e a s u r e d ~(0),c¢(E(160)).

82Be27 82Ma30

82Ma30

133

82Ma30 82Ma30 82Ma30

REACTION

INDEX

(t4C,xn) t4C(14C,xn),E(em)=13.5-32,5 MeV; m e a s u r e d a(E),

81Be64 (t4C,xna)

P~C(t4C,xna),E(em)=12.5-32.5 MeV; m e a s u r e d o'(E),

81Be64 (14N,'y)

~H(I'JN,3"),E=3.86 MeV; m e a s u r e d a b s o l u t e

82Be2g

4He(J4N,T),E=5.62 MeV; m e a s u r e d

absolute

82Be29

(i4N,p) t4N(taN,p),E=18-5~ MeV; m e a s u r e d r e s i d u a l s

82De39

SSNb(14N,p),E=95 MeV; m e a s u r e d a(E,O),spin

82Su07

(14N,np) t4N(t4N,np),E=18-52 MeV; m e a s u r e d r e s i d u a l s

82De39 (~'N,2p)

14N(t4N,2p),E=18-53 MeV; m e a s u r e d r e s i d u a l s

82De39 (14N,n2p)

t4N(t4N,n~p),E=lS-52 MeV; m e a s u r e d r e s i d u a l s 55Mn(t4N,n2p),E=47 MeV; m e a s u r e d E3",I3",recoil.

82De39 82C102

SSNi(14N,nap3"),E=47.6

MeV; m e a s u r e d E3",I3",recoil

781v03

(t4N,4n) ~'~SNd(14N,4n),E=72 MeV; m e a s u r e d 3"3"-coin.

82Lo05 (14N,(x)

1°B(14N,a),E(em)=8-17.5 MeV; m e a s u r e d a(O,E).

81Ho30

t4N(taN,a),E=lll MeV; m e a s u r e d a(O,E).

82Ta07

(14N,5n) 15gTb(t'tN,5n),E=95 JaSTb(J4N,Sn),E=95

MeV; m e a s u r e d 3'"/-energy MeV; m e a s u r e d 3"7(t),'r(O).

81De36 81Jall

tatTa(t4N,5n),E=lO0 MeV; m e a s u r e d E3",I3",3"3"-coin,

82GulO

(14N,not) t4N(P~N,na),E=I8-52 MeV; m e a s u r e d r e s i d u a l s

83De39 (14N,pot)

t4N(taN,pa),E=18-53 MeV; m e a s u r e d r e s i d u a l s

82De39 (t4N,6n)

l~gTb(14N,6n),E=95

MeV; m e a s u r e d "/3,-energy

81De36

tSSTb(laN,6n),E=95

(14N,npo~) 14N(t4N,npa),E=18 52 MeV; m e a s u r e d r e s i d u a l s

82De39 (14N,2p~)

14N(14N,Rpa),E=18-52

MeV; m e a s u r e d r e s i d u a l s

82De39

134

MeV; m e a s u r e d

3"3"(t),3'(9).

81Jall

REACTION

INDEX

(14N,2a) laN(t4N,2a),E=18-52 MeV; m e a s u r e d r e s i d u a l s aTAI(i4N,Ea),E=ll5 MeV; m e a s u r e d q(EpEs,0,,0a).

82De39 82Ko17

93Nb(t4N,2a),E=l15 MeV; m e a s u r e d

~(EI,Es,OI,es).

82Ko17

(14N,SBe) l°S(14N,eBe),E(cm):=8-17.5 MeV; m e a s u r e d a(O,E).

81Ho30 (14N,p2ot)

14N(14N,p2a),E=18--52 MeV; m e a s u r e d

residuals

82De39 (14N,3a)

14N(14N,3(x),E=18-52

MeV; m e a s u r e d

residuals

82De39

(14N,'2C) *CB('4N,laC),E(cm)::6-10 MeV; m e a s u r e d a(O,E).

81Ho30

(14N,14N) IaC(t4N,14N),E(cm):=16.9

MeV; m e a s u r e d a(O).

81Hu13

2°spb(14N,14N),E=sub-Coulomb; m e a s u r e d cr(01)/~(O~)

82Ly02

(14N,xnp) 154Sm(14N,xnp),E=167 MeV; m e a s u r e d

81YalO (14N,xnd)

*54Sm(14N,xnd),E=167 MeV; m e a s u r e d

81YalO (14N,xnt)

*54Sm(14N,xnt),E=167 MeV; m e a s u r e d

81YalO (14N,X)

L°B(14N,X),E=86-180 MeV; m e a s u r e d a ( f r a g m e n t O,E) 13C(14N,X),E=86 .... MeV; m e a s u r e d o r ( f r a g m e n t O,E) Z~AI(t4N,X),E=62 MeV; m e a s u r e d cr(O,fragment E) for Ag(I*N,X),E=O.125-4 M e V / n u c l e o n ; m e a s u r e d L - s h e l l

820r02 82Di13 81Ta22 81Ba56

ISSTb(14N,X),E=I40 MeV; m e a s u r e d 7 7 - c o i n , Ta(i4N,X),E=O.125-4 M e V / n u c l e o n ; m e a s u r e d L - s h e l l Au(*4N,X),E=O.125-4 M e V / n u c l e o n ; m e a s u r e d L - s h e l l

82Wi02 8 1 Ba5 6 8 1 Ba5 6

('4N,aX) SaNb(14N,aX),E=208 MeV; m e a s u r e d o r ( f r a g m e n t O,Oa)

82Fu04 (15N,4n)

146Nd(tSN,4n),E=74.

MeV; m e a s u r e d

Iv(O),vT coin.

82Ha27

(IaN,15N) c(~SN,15N),E=0.3-0.4 MeV; m e a s u r e d o p t i c a l CP,

82Lu02

Z°sPb(15N,tSN),E=sub-Coulomb; m e a s u r e d

~(0,)/~(02)

82Ly02

(*~N,X) 181

Ta(

15

N,X),E=86,95,103 MeV; m e a s u r e d

83Ka08

23aTh(15N,X),E=86,95,103

('6o,7) *H(160,7),E=14.4 MeV; m e a s u r e d

(r.

82Be29

135

MeV; m e a s u r e d

82Ka08

REACTION

INDEX

(~SO,p) 3He(l°O,p),E=19.4 MeV; m e a s u r e d D S A , p ~ - c o i n . SHe(~SO,p),E=15,18,21 MeV; m e a s u r e d DSA. Al(~SO,p),E=100 M e V / n u c l e o n ; m e a s u r e d a(e,Ep), eTAl(lSO,p),E=140 .... MeV; m e a s u r e d a(0p,Ep), ~TAl(~SO,p),E=310 MeV; m e a s u r e d a ( e p , E p ) , Ni(~SO,p),E=tO0 M e V / n u c l e o n ; m e a s u r e d a(0,Ep),

82Ba40 82Mo09 82Au07 82Aw01 82Ly01 82Au07

9ezr(160,p),E=215,310 MeV; m e a s u r e d cr(Ùp,Ep), Sn(lSO,p),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep), Au(180,p),E=100 M e V / n u c l e o n ; m e a s u r e d ¢r(0,Ep), lSTAu(160,p),E=140 .... MeV; m e a s u r e d a(Op,Ep), lS~Au(160,p),E=310 MeV; m e a s u r e d cr(0p,Ep),

8~Aw01 8~Au07 8~Au07 82Aw01 82Ly01

(leO,rip) l~C(~SO,np),E=ll.l .... MeV; m e a s u r e d r e l a t i v e lSc(lSO,np),E=13.8,18.2 MeV; m e a s u r e d r e l a t i v e

81Xe01 81Xe01

5SNi(tSO,np),E=40-55 MeV; m e a s u r e d ET,IT,Iv(t), SSNi(tSO,np),E=50 MeV; m e a s u r e d DSA,recoil,ET.

8~Ga06 8~Ga22

('60,d) lSC(l~O,d),E=ll.1 .... MeV; m e a s u r e d r e l a t i v e 13C(lSO,d),E=13.8,18.2 MeV; m e a s u r e d r e l a t i v e Al(lSO,d),E=100 M e V / n u e l e o n ; m e a s u r e d a(e,Ep), 2~Al(160,d),E=140 .... MeY; m e a s u r e d a ( 0 p , E p ) , Ni(lsO,d),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep),

81Xe01 81Xe01 82Au07 82Aw01 82Au07

SOZr(lSo,d),E=215,310 MeV; m e a s u r e d cr(Op,Ep), Sn(lSO,d),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep), Au(lSO,d),E=100 M e V / n u c l e o n ; m e a s u r e d cr(e,Ep), tS7Au(lSO,d),E=140 .... MeV; m e a s u r e d a(Op,Ep),

8~Aw01 82Au07 8~Au07 8~Aw01

(~6o,2p) $TAl(l°O,2p),E=310 MeV; m e a s u r e d cr(0p,Ep), SSFe(~SO,~p),E=46 MeV; m e a s u r e d ET,Iv,recoil.

82Ly0t 82C102

ISTAu(IS0,2p),E=310

MeV; m e a s u r e d

a(Op,Ep),

8~LyOl

(160,3n) ~2~Sn(lSO,3n),E=6~ MeV; m e a s u r e d

ET,IT,7(t),recoil

82Ze01

(~6o,t) Al(160,t),E=100 M e V / n u c l e o n ; m e a s u r e d ~(O,Ep), ~ A I ( ~ O , t ) , E = 1 4 0 .... MeV; m e a s u r e d ~(Op,Ep), Ni(lSO,t),E=100 M e V / n u c l e o n ; m e a s u r e d a(O,Ep), 9°Zr(~So,t),E=215,310 MeV; m e a s u r e d a(0p,Ep),

82Au07 82Aw01 82Au07 82Aw01

Sn(160,t),E=100 MeV/nueleon; m e a s u r e d cr(0,Ep), Au(160,t),E=I00 MeV/nueleon; m e a s u r e d cr(0,Ep), ISTAu(180,t),E=140 .... MeV; m e a s u r e d a(0p,Ep),

8~Au07 82Au07 82Aw01

(160,pd) aVAl(IS0,pd),E=310

MeV; m e a s u r e d

a(0p,Ep),

82LyO1

197Au(lSO,pd),E=310 MeV; m e a s u r e d

cr(0p,Ep),

82Ly01

(160,SHe) H(IaO,sHe),E=75 .... C(160,SHe),E=75 .... N(~SO,SHe),E=75 .... O(tSO,SHe),E=75 .... Al(l~o,SHe),E=100

MeV/nucleon; MeV/nucleon; MeV/nucleon; MeV/nucleon; MeV/nucleon;

m e a s u r e d a(E~,O), m e a s u r e d a(Ecx,O), m e a s u r e d a(Ea,0), ~ m e a s u r e d a(Ec%Ù), m e a s u r e d a(0,Ep),

82B~01 82B~01 82Bj01

Ni(ISO,SHe),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep), Br(lSo,SHe),E=75 .... M e V / n u e l e o n ; m e a s u r e d a(Ecx,0) Ag(lSO,SHe),E=75 .... M e V / n u c l e o n ; m e a s u r e d a(Ec~,O) Sn(lSO,3He),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep), Au(160,SHe),E=I00 M e V / n u c l e o n ; m e a s u r e d a(0,Ep),

8eBj01 82Au07

8~Au07

8eBj01 8~Bj01 82Au07 8~Au07

(160,4n)

~eZSn(ISO,4n),E=75,80 MeV; m e a s u r e d 17(E),7(t), 135Ba(le0,4n),E=77-84 MeV; m e a s u r e d 7T-coin,17(O), i~°Gd(IS0,4n),E=80,90 MeV; m e a s u r e d E7,I7. 16~Er(i~0,4n),E=80-105 MeV; m e a s u r e d a(E,0),

82Ze04 82Ba46 82Pe10 82Dr03

lSeEr(lSO,4n),E=80-105 MeV; m e a s u r e d cr(E,O), 168Er(leo,4n),E=80-105 MeV; m e a s u r e d a(E,0), 17°Er(leO,4n),E=81 MeV; m e a s u r e d ET,IV,77(t),7(O), 19Spt(leO,4n),E ,~ 90 MeV; m e a s u r e d V T - , n T - c o i n ,

82Dr03 82Dr03 82Fa01 82Po03

(160,~) H(I~0,c0,E=75 .... M e V / n u c l e o n ; m e a s u r e d cr(Ea,O), SLi(leO,a),E=24 MeV; m e a s u r e d ET,Iv,aT-coin,cc),(O ). i°B(tSO,a),E=42.4-60.1 MeV; m e a s u r e d a(E). C(160,a),E=75 .... M e V / n u c l e o n ; m e a s u r e d a(Ea,0), t2C(laO,a),E=28.5-100 MeV; m e a s u r e d a(0). taC(lS0,a),E=48.8 .... MeV; m e a s u r e d a(O),a(Ea). l~C(~eO,a),E=94-150 MeV; m e a s u r e d cr(Ea) v s E. tec(lSO,a),E=145 MeV; m e a s u r e d a(0,Ea). ~SC(lsO,a),E=29.5--52.6 MeV; m e a s u r e d a(E). 13C(lsO,a),E=145 MeV; m e a s u r e d a(O,Ea).

82Bj01 180(l°O,a),E ~ 2 0 - 4 5 MeV; m e a s u r e d a(O,E). 82Fr15 180(160,a),E=145 MeV; m e a s u r e d cr(0,Ea). 82Pa02 eONe(JSO,a),E=145 MeV; m e a s u r e d a(O,Ea). 82Bj01 Al(laO,a),E=100 M e V / n u c l e o n ; m e a s u r e d a(8,Ep), 81Sz06 e~Al(lso, a),E=140 .... MeV; m e a s u r e d a(Op,Ep), 81Sz07 Ni(laO,a),E=100 M e V / n u c l e o n ; m e a s u r e d a(0,Ep), 82Stll Br(lSO,a),E=75 .... M e V / n u c l e o n ; m e a s u r e d a(Ea,0), 82Ta02 9OZr(160,a),E=215,310 MeV; m e a s u r e d o'(Sp,Ep), 82Pa02 Ag(160,a),E=75 .... M e V / n u c l e o n ; m e a s u r e d a(Ea,O), 82Ta02 Sn(lSO,a),E=100 M e V / n u c l e o n ; m e a s u r e d o'(e,Ep), continued

136

81Po16 82Ta0Z 82Ta02 82Au07 82Aw01 82Au07 82Bj01 82Aw01 82Bj01 82Au07

REACTION

(~o,a) N(laO,a),E=75 .... MeV/nucleon; m e a s u r e d ~(Ba,O), ~N(~aO,a),E=145 MeV; m e a s u r e d a(O,Ea). O(laO,a),E=75 .... lvleV/nucleon; m e a s u r e d a(Ea,O), ~sO(*aO,a),E(cm)=15.5-17 MeV; m e a s u r e d ¢(0) vs E.

INDEX

continued

8aBjO1 83Ta02 8aBj01 81Ga33

~S'*Sn(~O,a),E=90 .... MeV; m e a s u r e d a(Oa),cr(Ea,Oa) Au(/~O,a),E=100 M e V / n u c l e o n ; m e a s u r e d a(O,Ep), i97Au(XSO,a),E=140 .... MeV; m e a s u r e d (~(Op,Ep),

82Tr02 82Au07 82AwOl

(160,5n) tS°Gd(*so,5n),E=80,90 MeV; m e a s u r e d ET,I 7. ~7°Er(~0,Sn),E=96 MeV; m e a s u r e d ET,17,77(t),7(O),

8~PelO 8~Fa01

lS*Ta(lS0,5n),E=100 MeV; m e a s u r e d IT(~,t).

82Da17

(160,6n) le°Gd(~eO,6n),E=llD-134 MeV; m e a s u r e d

E7,17.

8~Pel0 (160,7n)

~e°Gd(*SO,Tn),E=l:[0-134 MeV; m e a s u r e d E7,17.

8~PelO (160,8n)

~a°Gd(iaO,8n),E=120 .... MeV; m e a s u r e d

By,IT.

8~PelO

(160,l°S) ~°B(~aO,~°B),E=42.4-60.1 MeV; m e a s u r e d a(E).

82Pa02

(160,lZC) lZC(~aO,~eC),E(cm)=12.a-13.5 MeV; m e a s u r e d a(O) vs eONe(taOJZC),E(crr0=22.8-38.6 MeV; m e a s u r e d a(E), ZaMg(l~O,tzC),E(cm) ~ 3 2 - 3 6 MeV; m e a s u r e d a(0=5 s)

81Ta24 82Se13 8aFu06

6°Ni(lSO,lzC),E=60 MeV; m e a s u r e d a(E(IaC)),q(0). SSRu(160,tZC),E=70 MeV; m e a s u r e d ~(E(IzC)),

8 2 Be1 5 82Th61

(180,~3C)

laC(~aO,~sC),E=29.5-5~.6 MeV; m e a s u r e d

o~(E).

aORu(ISO,13C),E=70 MeV; measured ~r(E(lzC)),

8~Pa02

8~Th01

(160,14C) 9SRu('80,'4C),E=7,3 MeV; m e a s u r e d q(E(~zC)),

82ThOl

I°4Pd(IsO,14C),E=70

MeV; m e a s u r e d

c;(E(IsC)),

8~ThOl

(160,15N) aSCa(*SO,*SN),E=158.2 MeV; m e a s u r e d a(0),

82HulO

(160,150) *r°Er(~SO,lsO),E=120

MeV; m e a s u r e d

ISOT-eoin ,

82Kr03

(160,160) ~°B(*S0,1SO),E=42.4-60.1 MeV; m e a s u r e d a(E). X2C(l~0,*~O),E=45.5-49 MeV; m e a s u r e d a(0),cr(E). laC(lsO,~SO),E=~9.5-52.6 MeV; m e a s u r e d a(E). iaC(t~O,lSO),E(cm)=10-60 MeV; m e a s u r e d q(0), ~SO(*sO,lsO),E(cm)=15.5-17 MeV; m e a s u r e d a(0) vs E ~°Ca(~So,*~O),E=60 MeV; m e a s u r e d a(0),a(E(~so)).

82Pa02 82Wi 04 82Pa02 82H e 07 81G a 33 82Re03

4ZCa(ISO,tsO),E=60 MeV; m e a s u r e d ~(0),cr(E(lS0)). 44Ca(ISO,leO),E=60 MeV; m e a s u r e d a(O),cr(E(180)). 48Ca(180,180),E=158.2 MeV; m e a s u r e d a(0), 48Ca(ISo,lSO),E=56 MeV; m e a s u r e d a(0),a(E(*80)). 6°Ni(lao,lSO),E=45,54,60 MeV; m e a s u r e d o(E(12C)), Z°aPb(tsO,leO),E=50 MeV; m e a s u r e d a(01)/q(Oz) vs E

8~Re03 8~Re03 8~HulO 8 ~Re0 3 8~Bel5 8RLy08

(160,160') ~SO(tsO)sO'),E(em)=33.1 MeV; m e a s u r e d a(O,E(~SO)) *~O(*~O,lsO'),E(cm)=25-35 MeV; m e a s u r e d a(O=90s,E) ~O(tSO,*sO'),E(cm)=24-41 MeV; m e a s u r e d 7 7 - c o i n . ~°Ca(~O,~O'),E=60 MeV; m e a s u r e d cr(O),o'(E(~sO)).

4ZCa(JSo,lSO'),E=60 MeV; m e a s u r e d a(O),a(E(~So)). ~4Ca(l~O,~eO'),E=60 MeV; m e a s u r e d a(0),a(E(~S0)). aSCa(iSO,~eO'),E=158.2 MeV; m e a s u r e d o'(0), ~eCa(~aO,~O'),E=56 MeV; m e a s u r e d c~(0),a(E(l~O)).

81Ba55 81Tr09 82We07 82Re03

137

8ERe03 83Re93 83HulO 8~Re03

REACTION INDEX

(~OOl~O) 4eCa(160,170),E=158.a MeV; m e a s u r e d

a(e),

82HulO

(l°O,a°Ne) 2 ° N e ( Z ° O , 2 ° N e ) , E ( c m ) = 2 2 . 8 - 3 8 , 6 MeV; m e a s u r e d

a(E).

82Sc13

(Z°O,xn) u°Pd(l°O,xn),E(cm)=55-70 MeV; m e a s u r e d 1 4 4 S m ( 1 6 0 , x n ) , E ( c m ) = 5 5 - 7 0 MeV; m e a s u r e d

neutron neutron

82JaO1 82JaO1

lS4Sm(leO,xn),E(cm)=55-70

MeV; m e a s u r e d

neutron

82Ja01

(160,F) 2aeU(l°O,F),E=140,315 MeV; m e a s u r e d

82ViOl

('°o,x) 12C(leO,X),E=IO0-315 MeV; m e a s u r e d a(O) f o r X=B,C, 1 2 C ( l e O , X ) , E ( c m ) = 1 2 - 2 0 MeV; m e a s u r e d 1 4 C ( 1 6 0 , X ) , E ( c m ) = l O - 6 0 MeV; m e a s u r e d a(O), l°O(l°O,X),E=102 MeV; m e a s u r e d 2 ° N e ( 1 8 0 , X ) , E ( c m ) = 1 5 - 2 9 MeV; m e a s u r e d production 2~AI(ieO,X),E=IO0-315 MeV; m e a s u r e d a(O) f o r X=B,C 27Al(160,X),E=lO0 MeV; m e a s u r e d a(fragment 8) v s

81Mel5 82Fr04 82He07 82Pe08 83XaOl 81Me15 82Yo01

(SCa(leO,X),E=158.2 MeV; m e a s u r e d a(O),a(E(leO')), 48Ti(ISO,X),E=IO0 MeV; m e a s u r e d 6 ° N i ( l ° O , X ) , E = l O 0 - 3 1 5 MeV; m e a s u r e d o'(8) f o r X=B,C a a C u ( 1 6 0 , X ) , E = 4 0 - 8 5 MeV; m e a s u r e d E7,I7. e ° s P b ( l e O , X ) , E = l O 0 - 3 1 5 MeV; m e a s u r e d a ( 8 ) f o r X=B, 23aTh(tSO,X),E=97 .... MeV; m e a s u r e d aiSCm(160,X),E=98 MeV; m e a s u r e d production a for

82HulO 81TrlO 81Mel5 82Ba33 81Me15 82Ka08 82LEO1

(160,nX) 4eca(leO,nX),E=142 MeV; measured nX-,pX-,aX-coin.

82Ya03 (lSO,pX)

4eCa(180,pX),E=142 MeV; m e a s u r e d

nX-,pX-,aX-coin.

82Wa03

(lsO,~X) 48Ca(160,aX),E=142 MeV; m e a s u r e d

nX-,pX-,aX-coin.

82Wa03

(t~o,~) leC(iTO,a),E=30-57

MeV; m e a s u r e d

or(E).

82Pa02

13C(170,~),E=30-57 MeV; m e a s u r e d

a(E).

8aPa02

(170,5n) tgept(l~O,5n),E ~ 96 MeV; m e a s u r e d

~T-,n'y-coin,

82Po03

(170,1aC) lZC(ivO,iaC),E=30-57 MeV; m e a s u r e d

a(E).

82Pa02

(l~O,13C) IaC(170,13C),E=30-57 MeV; m e a s u r e d

a(E).

82Pa02

(i~O,'°O) 2°sPb(lVo,lSO),E=66-88

MeV; m e a s u r e d

a(E(°O)),

82Kul4

(t70,'70) t2C(170,ZTO),E=30-57 MeV; m e a s u r e d a(E). 12C(170,170),E=54-140 MeV; m e a s u r e d o'(8),

82Pa02 82He07

13C(110,170),E=30-57 MeV; m e a s u r e d

138

~(E).

82Pa02

REACTION INDEX

(170,170') Z°spb(l:'O,tTO'),E=66-88 MeV; m e a s u r e d

a(E(170)),

82Ku14 (170,180)

Z°spb(170,180),E=66-88 MeV; m e a s u r e d

~(E(160)),

82Ku14 (170,xn)

15eSm(iTO,xn),E=80-84 MeV; m e a s u r e d

77-coin,7(0),

B2Ro08

IS4Sm(IVO,xn),E=80-84

MeV; measured

77-eoin,7(O),

82Ro08

('~O,X) ~°B(*~0,X),E=54 .... MeV; m e a s u r e d

a(fragment

O,E)

82Ch07

ISc(1~O,X),E=54-140 MeV; m e a s u r e d a(0),

82He07

(~8o,7) tH(Iso,7),E=2,7,20.88 MeV; m e a s u r e d a b s o l u t e

82Be29

12C(180,7),E=5O-8J MeV; measured

production

or(E)

8IBa66

(tSO,p) tH(tSO,p),E=47 MeV; m e a s u r e d D S A , ( p a r t i c l e ) T - c o i n .

82Ba06

(180,2np) zgSi(180,2np),E=30-99 MeV; m e a s u r e d i s o m e r

82Gr20

(180,a) 4He(180,c~),E=34

MeV; m e a s u r e d

DSA,(particle)7-coin

82Ba06

lZc(lSo,a),E=50-81 MeV; m e a s u r e d

(tSO,Sn) lZC(tsO,5n),E=50-81

MeV; m e a s u r e d E7,I3'.

82Ba49

(180,5np) lac(lSO,5np),E=50-81 MeV; m e a s u r e d

E7,17.

82Ba49

(180,Sn2p) lZC(tsO,5nEp),E=50-81 MeV; m e a s u r e d

E7,I7.

82Ba49

(180,2a) ~Zc(tSo,2a),E=50-81

MeV; measured

E7,17.

82Ba49 (180,naa)

tac(tSO,nSc~),E=50-81 MeV; m e a s u r e d

E7,I7.

82Ba49

C8o73c) lZc(Jao,tSC),E=50-81 MeV; m e a s u r e d

E7,I7.

82Ba49

(IB0,14C) IZC(180,~aC),E=50-81

MeV; m e a s u r e d

E7,17-

82Ba49

139

E7,17.

8 2 Ba4 9

REACTION

INDEX

(1BO,15N) iaC(leO,iSN),E=50-81 MeV; m e a s u r e d

ET,I 7.

82Ba49

(180,'60) 12C(*80,1SO),E=50-81 MeV; m e a s u r e d

E7,I7.

82Ba49

('e0,17C) 4eCa(lSO,tvC),E=ll2 MeV; m e a s u r e d

a(E(ieC)),

82FilO

('eO,l~O) 12C(leO,170),E=50-SJ MeV; m e a s u r e d

E7,17.

82Ba49

4°Ca(*e0,1~O),E=62.14 MeV; m e a s u r e d

a(O),a(E(lvO))

82Re14

('80,18C) CSCa('eO?aC),E=ll2 MeV; m e a s u r e d

a(E(1sC)),

82Fi10

4eCa(leO,leC),E=100 MeV; m e a s u r e d

a(E(18C)),Q.

82Na04

(180,180) laC(laO)80),E=32-140

MeV; m e a s u r e d

or(0),

40Ca(leO,teO),E=62.14 MeV; m e a s u r e d

82He07

o'(0),cr(E(l~O))

82Re14

(180,1809 lac(tSo, ieO'),E=50-81 MeV; m e a s u r e d

ET,] 7.

82Ba49

4°Ca(teO,IsO'),E=62.14MeV; measured G(O),

82Re14

(lSo,isN)

tSo('80,tSN),E=lO0 MeV; measured

a(E(19N)),

82Na08

('eO,'~F) 4°Ca(t80,tSF),E=62.14

MeV; m e a s u r e d

a(0),cr(E(tTO))

82Re14

(180,2'0) taO(isO,2tO),E=92 MeV; m e a s u r e d

82Na08

o'(E(tgN)),

(18O,xn) t2C(leO,xn),E=50-81 MeV; measured production cr(E) tS~Sm(tSO,xn),E=80-84 MeV; measured 77-coin,7(0),

81Ba66 82Ro08

154Sm(ISO,xn),E=80-84MeV; measured 77-coin,7(8), JSSEr(JSO,xnT),E=81 MeV; measured ET,IT,(T(ET,0),

82Ro08 82Li04

(*SO,X) t2c(lSO,X),E=50-S1 MeV; m e a s u r e d IaC(tSO,X),E=50-81 MeV; m e a s u r e d

production E7,I7.

G(E)

81Ba66 82Ba49

1aC(tSO,X),E=32-140 MeV; m e a s u r e d G(0), 24SCm(iSO,X),E=97 MeV; m e a s u r e d p r o d u c t i o n

G for

82He07 82Le01

(19F,p) *TSLu(lgF,p),E=135,184

MeV; m e a s u r e d

cr(E),

82Ra06

(19F,d) t75Lu(~SF,d),E=135,184

MeV; m e a s u r e d

or(E),

82Ra06

(IgF,anp) aSCu(iOF,2np),E=46-62

MeV; m e a s u r e d

E(3,),I(E(7)),

82Pa20

SSCu(tgF,2np),E=50,55,58

140

MeV; m e a s u r e d

ET,recoil

82Pa06

REACTION

INDEX

(*aF,t) 17SLu(*°F,t),E=135,184 MeV; m e a s u r e d a(E),

82Ra06 (19F,n2p)

63Cu(19F,nSp),E=46-62 MeV; m e a s u r e d

E(T),I(E(7)),

82Pa20

(19F,a) IH(iaF,aT),E=6.42,16.44 MeV; m e a s u r e d a b s o l u t e ~S4Sn(ISF,a),E=104 MeV; m e a s u r e d a(Oa),o'(Ec(,Oa),

82Be29 82Tr02

17~Lu(10F,a),E=135,184

MeV; m e a s u r e d ~;(E),

8 2 Ra0 6

(19F,Sn) tTSHf(10F,5n),E=85-120 MeV; m e a s u r e d a(E7),7(0),

81Kr20 (19F,2na)

83Cu(laF,2n~),E=58 MeV; m e a s u r e d

recoil.

82Ke01 ('SF,xnyp)

S~Al(*aF,xnyp),E=47-108 MeV; m e a s u r e d

ET,77-coin,

81HeS0

(19F,F) I~SLu(lSF,F),E=135,184 MeV; m e a s u r e d a(E), leITa(IaF,F),E=80-125 MeV; m e a s u r e d

82Ra06 82Hi09

ISlTa(19F,F),E=80-126 MeV; m e a s u r e d

~(fission),

82Le05

IalTa(IOF,X),E=80-125 MeV; m e a s u r e d IaITa(IaF,X),E=80-126 MeV; m e a s u r e d a ( f i s s i o n ) ,

82Hi09 82Le05

(19F,X) ZTAl(IaF,X),E=34-75 MeV; m e a s u r e d or(fusion,E). aaSi(10F,X),E=34-75 MeV; m e a s u r e d a ( f u s i o n , E ) . SOsi(10F,X),E=34-75 MeV; m e a s u r e d a ( f u s i o n , E ) .

81Ch32 81Ch32 81C h32

(Ne,Tr-) F(Ne,rr-),E=183 M e V / n u e l e o n ; m e a s u r e d pion Na(Ne,~T-),E=I83 M e V / n u c l e o n ; m e a s u r e d p i o n

82Na10 82Na10

Pb(Ne,~v-),E=183 M e V / n u e l e o n ; m e a s u r e d

pi on

82NalO

(2°Ne,Tr-) C(2°Ne,~r-),E=280-480 M e V / n u c l e o n ; m e a s u r e d F(ZONejr-))E=280-480 M e V / n u e l e e n ; m e a s u r e d Na(2°Ne,zr-),E=280-480 M e V / n u c l e o n ; m e a s u r e d

82Su01 82S u01 82S u01

Cu(2°Ne,~-),E=280-480 M e V / n u c l e o n ; m e a s u r e d U(S°Ne,Tr-),E=280-480 M e V / n u c l e o n ; m e a s u r e d

82SuOl 82Su01

(Z°Ne,vr+) C(Z°Ne,zr+),E=280-480 M e V / n u e l e o n ; m e a s u r e d F(Z°Ne,Tr+),E=280-4BO M e V / n u e l e o n ; m e a s u r e d Na(S°Ne,~r+),E=280-480 M e V / n u c l e o n ; m e a s u r e d

82S u01 82SuO1 82SuOl

Cu(aONejr+),E=280-480 M e V / n u c l e o n ; m e a s u r e d U(a°Ne,vr+),E=280-480 M e V / n u e l e o n ; m e a s u r e d

(2°Ne,p)

17"~yb(Z°Ne,p),E=125,25;~ MeV; m e a s u r e d c~(E),

82Ra06 (2°Ne,d)

174

Yb(

20

Ne,d),E=125,252 MeV; m e a s u r e d

o'(E),

82Ra06 (Z°Ne,t)

174Yb(20Ne,t),E=125,252 MeV; m e a s u r e d o'(E),

82Ra06

141

82Su01 82Su01

REACTION

INDEX

(2°Ne,a) 124Sn(2°Ne,a),E=l12,156 MeV; m e a s u r e d

a(ecx),

82Tr02

a74Yb(2°Ne,a),E=125,252 MeV; m e a s u r e d

~(E),

82Ra06

vs

828a21

(2°Ne,Sn) 14SNd(2°Ne,5n),E=136 MeV; m e a s u r e d

a

vs

82Sa21

(a°Ne,6n) 82Ja08

140Nd(2°Ne,6n),E=136,149 MeV; m e a s u r e d

14eNd(2°Ne,6n),E=136 MeV; m e a s u r e d

a

(Z°Ne,7n) 146Nd(2°Ne,7n),E=136 MeV; m e a s u r e d

a

vs

82Sa21

(Z°Ne,a'SN) 197Au(2°Ne,aLSN),E=290 MeV; m e a s u r e d

a(lSN) - ,

82Ho10

(Z°Ne,al60) 197Au(egNe,c~160),E=290 MeV; m e a s u r e d

a(15N) - ,

82Ho10

(Z°Ne,Z°Ne) SaNi(~°Ne,e°Ne),E=392

MeV; m e a s u r e d

a(E(2°Ne)).

82Vo04 (ZONe,ZONe')

SSNi(2°Ne,2°Ne'),E=392 MeV; m e a s u r e d

a(E(2°Ne)).

82Vo04

(Z°Ne,F) 174Yb(e°Ne,F),E=125,252 MeV; m e a s u r e d a(E), l~TAu(2°Ne,F),E=172 MeV; m e a s u r e d fission lgTAu(2°Ne,F),E=252 MeV; m e a s u r e d

82Ra06 82Du09 82Mo06

197Au(2°Ne,F),E=252 MeV; m e a s u r e d fission 238u(2ONe,F),E=252 MeV; m e a s u r e d 23eU(2°Ne,F),E=252 MeV; m e a s u r e d fission

82Mo21 82Mo06 8~Mo21

(Z°Ne,pF) 197Au(2°Ne,pF),E=265 MeV; m e a s u r e d

fission

82Ri06

(Z°Ne,dF) 197Au(2°Ne,dF),E=265 MeV; m e a s u r e d

fission

82Ri06

(a°Ne,tF) l g T A u ( 2 ° N e , t F ) , E = 2 6 5 MeV; m e a s u r e d

fission

82Ri06

(Z°Ne,~F) 197Au(2°Ne,aF),E=265 MeV; m e a s u r e d

fission

82Ri06

(a°Ne,X) L2C(2°Ne,X),E=291 MeV; m e a s u r e d o" ( f r a g m e n t e) vs 27Al(2°Ne,X),E=291 MeV; m e a s u r e d a (fragment 0) vs 4OCa(2°Ne,X),E=291 MeV; m e a s u r e d a (fragment 0) v s Cu(2ONe,X).E=IT0,252 MeV; m e a s u r e d Ag(2ONe,X).E=0.125-4 M e V / n u c l e o n ; m e a s u r e d L-shell

82Mo15 82Mo15 82Mo15 82Ma01 81Ba56

Ta(2°Ne,X),E=0.125-4 MeV/nucleon; measured L-shell Au(a°Ne,X),E=0.125-4 MeV/nucleon; measured L-shell 197Au(2°Ne,X),E=lT0,252 MeV; m e a s u r e d a*SCm(a°Ne,X),E=II5 MeV; m e a s u r e d production a for

142

81Ba56 81Ba56 82Ma01 82Le01

REACTION

INDEX

(a°Ne,pX) lSTAu(2eNe,pX),E=100,156 M e V / n u c l e o n ; m e a s u r e d

82We I

1

(2°Ne,dX) 197Au(a°Ne,dX),E=100,156 M e V / n u e l e o n ; m e a s u r e d

82Well (e°Ne,tX)

lgTAu(2°Ne,tX),E=100,156 MeV/nueleon; m e a s u r e d

82Well (2°Ne,o~X)

197Au(2°Ne,c~X),E=100,156

MeV/nucleon; measured

82We 1 1 (~2Ne,xn)

~47Sm(Z2Ne,xn),E=l10,136 MeV; m e a s u r e d

81Br30

ET,IT.

(SaNe,F)

W(22Ne,F),E=I74 MeV; m e a s u r e d

a(fragment

0).

82Bu06

(22Ne,X) e4SCm(UaNe,X),E=ll6 MeV; m e a s u r e d

production

cr for

82LeOl

(a4Mg,n)

3He(24Mg,n),E=50 MeV; m e a s u r e d

3,T-coin,DSA.

82AI 15

(24Mg,5n) teOTm(e4Mg,5n),E=liS-135 MeV; m e a s u r e d

a(E3'),T(0),

81Kr20 (24Mg,Z4Mg)

12C(S4Mg,24Mg),E(cm)=24-43 MeV; m e a s u r e d

a(0=lS0 o)

82Me06 (a4Mg,a4Mg')

12C(24Mg,24Mg'),E(elxl)=24-43 MeV; m e a s u r e d

82Me06 (24Mg,xn)

141Pr(24Mg,xn),E=llO-130 MeV; m e a s u r e d

production

82Sc15

142Nd(24Mg,xn),E=l10-130 MeV; m e a s u r e d p r o d u c t i o n

82Se15

(24Mg,xnyp) SSNi(24Mg,xnyp),E=iL00 MeV; m e a s u r e d

ET,IT,Tnn-,

82Li08 (24Mg,X)

~aC(24Mg,X),E(em)=16.4-29.8 MeV; m e a s u r e d 24Mg(24Mg,X),E(cm)=21-41.6 MeV; m e a s u r e d a ( f u s i o n )

82Ga09 82Ga09

aSMg(24Mg,X),E(em)=20.3-32.9 MeV; m e a s u r e d ~°Si(~4Mg,X),E(em)=24.2-38.1 MeV; m e a s u r e d

(e°Mg,4n) lSSTm(aSMg,4n),E=120 MeV; m e a s u r e d

a(ET).T(0),

81Kr20

143

82Ga09 82Ga09

REACTION

INDEX

(ZSMg,2°Mg') ~°spb(2SMg,26Mg'),E=80-120

MeV; m e a s u r e d Coulomb

82Sp05 (27A1,5n)

ISeEr(27A1,5n),E=130-160 MeV; m e a s u r e d G(E-/),T(O),

81.Kr20 (2aSi,n) 82A122

aHe(2aSi,n),E=60 MeV; m e a s u r e d DSA.

(2aSi,4n) 14aSm(ZaSi,4n),E=145 MeV; m e a s u r e d 7~-coin,7(0).

82Du13

lS°Sm(2aSi,4n),E=138 MeV; m e a s u r e d -/7-coin,7(O).

82Du13

(2aSi,a) t2C(zaSi,a),E=84-92 MeV; m e a s u r e d a(Ea,E). leC(2aSi,a),E=75-102 MeV; m e a s u r e d q(Ea),G(0=0 °)

81Pa27 82Pa17

13C(zsSi,~),E=75-102 MeV; m e a s u r e d a(Ecx),cr(O=O°)

82Pa17

(2aSi,5n) 124Sn(ZSsi,5n),E=128-140 MeV; m e a s u r e d 7T-coin,

82Ba46 (2asi,2a)

laC(2aSi,2a),E=68-80

MeV; measured

as-coin.

81A126 (ZaSi,12C)

leC(2aSi,12C),E=99-133

MeV; m e a s u r e d a(E(lzC)),

82Sh16 (28Si,'aN)

12C(2aSi,i4N),E=99-133 MeV; measured

q(E(12C)),

82sh16 (2aSi,160)

tZC(2aSi?SO),E=99-133

MeV; measured

a(E(12C)),

82Sh16 (2asi,2asi)

tZc(2Ssi,2Ssi),E=55-99 MeV; m e a s u r e d a(0=1800,E). tac(2eSi,zaSi),E=55-99 MeV; m e a s u r e d G(0=180°,E).

82Ch02 82Ch02

SaNi(2SSi,2Ssi),E= 140 MeV; m e a s u r e d G(0).

82Bo25

(2asi,2aSi') 6aNi(2aSi,2Ssi'),E = 140 MeV; m e a s u r e d G(0).

82Bo25 (2aSi,xn)

12OSn(2aSi,xn),E=108-144 MeV; m e a s u r e d l~/(O,H,t)

82Ha22

124Sn(2SSi,xn),E=108-144 MeV; m e a s u r e d I-y(8,H,t)

82Ha22

(2aSi,xnyp) a4Fe(2SSi,xnypT),E=80-99 MeV; measured SSFe(2aSi,xnyp~/),E=80-99 MeV; measured

E'/,I~/, E~,I~/,

82Th03 82Th03

SaNi(zaSi,xnyp),E not given; m e a s u r e d E~/,I%~nn -,

82Li08

(2asi,x) 12C(aSSi,X),E(cm)=15.1-24.6 MeV; m e a s u r e d 2aSi(22Si,X),E(cm)=27.9-41.4 MeV; m e a s u r e d

82Ga09 82Ga09

SSSi(2aSi,X),E(cm)~27.4-42.1 MeV; measured 3aSi(zSsi,X),E(cm)=27.3-42.8 MeV; m e a s u r e d

144

82Ga09 82Ga09

REACTION

INDEX

(agSi,xnyp) SSNi(aSSi,xnyp),E not

given;

measured

ET,lT,Tnn-,

82Li08

(30Si,F) l ? ° E r ( a ° S i , F ) , E = 1 2 5 - - 1 7 0 MeV; m e a s u r e d

82Hi09

17°Er(aOsi,F),E=125-168 MeV; m e a s u r e d

(;(fission),

82LEO5

a(fission),

82Le05

(3°si,x) l~°Er(SOsi,X),E:125-170

MeV; m e a s u r e d

82Hi09

1 7 ° E r ( a ° S i , X ) , E = 1 2 5 - 1 6 8 MeV; m e a s u r e d

(32S,Sn) 15STb(3aS,5n),E=16C,-165 MeV; m e a s u r e d

a(ET),7(0),

81KrS0

(32S,32S) 12C(asS,suS),E=55-99 MeV; m e a s u r e d 12C(ssS,seS),E=65-99 MeV; m e a s u r e d

a(0=180°,E). a(e).

82Ch02 82Ch02

*aC(szS,ssS),E=55-99

MeV; m e a s u r e d

cr(0=i80°,E).

82Ch02

(32S,32S,) n o p d ( 3 2 S , s a S ' ) , E = 9 0 - 1 2 0 MeV; m e a s u r e d 7(0,H,T), 1 5 ° S m ( a e s , a e s ' ) , E = 9 0 - 1 2 0 MeV; m e a s u r e d 7(0,H,T), laSOs(aSS?sS'),E ~ 80 MeV; m e a s u r e d 7(0,H) i n 188Os(32S,ssS'),E = 80 MeV; m e a s u r e d 7(O,H) i n

82Dall 82Dall 82Le02 82Le02

*94pt(32S,asS'),E ~ 80 MeV; m e a s u r e d 7(@,H) i n *S°pt(SeS,seS'),E ~ 80 MeV; m e a s u r e d 7(0,H) i n 2 ° 8 p b ( S a S ? s S ' ) , E = 1 2 2 - 1 6 0 MeV; m e a s u r e d Coulomb

8ZLe02 82LeO2 82VeO9

(3eS,xn) l e S S n ( S Z S , x n ) , E = t 6 0 MeV; m e a s u r e d *U4Sn(SSS,xn),E=150 MeV; m e a s u r e d

77(0) ratio, ET,IT,linear

1aOTe(32S,xn),E=150 MeV; measured E T , I T , l i n e a r 1 4 4 S m ( S S S , x n ) , E = 1 3 9 . 5 - 2 0 1 MeV; m e a s u r e d Ea,Ia.

82Se07 82Tr01

82Tr01 82En03

(3ZS,xnypza) 144sm(aSS,xnypza),E=139.5-201

MeV; m e a s u r e d

Ea,lcx.

82En03

(32S,F) 7SGe(SZS,F),E=158,... MeV; m e a s u r e d

absolute

81Gu16

(32s,x) 180(aaS,X),E=225 MeV; m e a s u r e d ZTAl(aSS,X),E=135,190 MeV; m e a s u r e d

82Pe08 82Pe08

STAI(aSS,X),E=152.6,175 MeV; m e a s u r e d or(0), 7SGe(SSS,X),E=158 .... MeV; m e a s u r e d absolute

82ROI0 81Gu16

(34S,4n) I~4Sn(S4S,4n),E=145-165

MeV; m e a s u r e d

77-coin,7(0)

82PalO (34S,X)

45Sc(S4S,X),E=85-130 MeV; m e a s u r e d

ET,I 7.

82Ba33

(35C1,4n) 155

Gd(

35

CI,4n),E=I55-170

MeV; m e a s u r e d

a(ET),7(O),

81Kr20 (asCl,F)

SSNi(sSCI,F),E=155-300 MeV; m e a s u r e d SSNi(sSCI,F),E=200,215 MeV; m e a s u r e d U S S n ( a S C l , F ) , E = 1 5 5 - 3 0 0 MeV; m e a s u r e d llSSn(SSCl,F),E=200,215 MeV; m e a s u r e d

82Si01 82Si05 82Si01 82Si05

14*Pr(SSCI,F),E=155-300 MeV; m e a s u r e d 14*pr(SSCI,F),E=200,215 MeV; m e a s u r e d 1 9 7 A u ( s S C l , F ) , E = 2 0 4 - 3 1 7 MeV; m e a s u r e d

145

fission

82Si01 82Si05 82Be34

REACTION

INDEX

(35cl,x) eSNi(SSCl,X),E=155-300 MeV; measured ~Ni(~SCI,X),E=200,215 MeV; measured HSSn(~SCI,X),E=I55-300 MeV; measured ItSSn(~CI,X),E=200,215 MeV; measured

82Si01 82Si05 82Si01 82Si05

141pr(SSCl,X),E=155-300 MeV; measured 141Pr(3~CI,X),E=200,215 MeV; measured IStTa(SSCI,X),E=205 MeV; measured a(fragment e,E) tgVAu(SScI,X),E=204-317 MeV; measured fission

82Si01 82Si05 82Ka08 82Be34

t 4 g S m ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative 1 5 0 S m ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative 1 5 S S m ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, t S 4 S m ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, I S 1 E u ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative l S S E u ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative

82Ri01 82Ri01 82Ri01 82Ri01 82Ri01 82Ri01

tS4Gd(Ar,X),E=275

82Ri01

(Ar,X) 1SSLa(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, t4OCe(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, t4~Ce(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, t 4 t p r ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, t 4 ~ N d ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative X~SNd(Ar,X),E=~75,245 MeV; m e a s u r e d cumulative I ~ 4 N d ( A r , X ) , E = 2 7 5 , ~ 4 5 MeV; m e a s u r e d cumulative t 4 S N d ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative 14SNd(Ar,X),E=~75,245 MeV; m e a s u r e d cumulative t~SNd(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, t S ° N d ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, ~Sm(Ar,X),E=275,245 MeV; m e a s u r e d cumulative ~Sm(Ar,X),E=275,245 MeV; m e a s u r e d cumulative I4SSm(Ar,X),E=275,245 MeV; m e a s u r e d c u m u l a t i v e

82Ri01 82Ri01 82Ri01 82Ri01 82Ri01 82RiOt 82RiOt 82Ri01 82Ri01 82RiOt 82Ri01 82Ri01 82Ri01 82Ri01

MeV; measured

cumulative

yields,

t S S G d ( A r , X ) , E = 2 7 5 , 2 4 5 MeV; m e a s u r e d cumulative t S e G d ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, lS~Gd(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, tSSGd(Ar,X),E=275 MeV; m e a s u r e d cumulative yields, I S ° G d ( A r , X ) , E = 2 7 5 MeV; m e a s u r e d cumulative yields, ~SSTb(Ar,X),E=275 MeV; m e a s u r e d cumulative yields,

82Ri01 82Ri01 82Ri01 82Ri01 82Ri01 82Ri01

(39K,xnyp) 4°Ca(SSK,xnyp),E not

given;

measured

E~,l~',Tnn-,

82Li08

(4OAr,vr-) C(4°Ar,Tr-),E=l.05 G e V / n u c l e o n ; measured a(E,0). C(4°Ar,Tr-),E=535 M e V / n u c l e o n ; m e a s u r e d a(Evr,Ovr). Cl(40Ar,Tr-),E=0.36-1.8 GeV/nucleon; measured pion Cl(40Ar,~r-),E=535 M e V / n u c l e o n ; m e a s u r e d a(E~r,01r). K(4OAr,~r-),E=0.36-1.8 G e V / n u c l e o n ; measured pion

K(4°Ar,~r-),E=535 MeV/nucleon; measured a(Evr,0zr). Ca(4OAr,lr-),E=l.05 GeV/nucleon; measured a(E,0). l(4°Ar,~r-),E=977,772 MeV/nucleon; measured pion Ba(4OAr,zr-),E=977,772 M e V / n u c l e o n ; m e a s u r e d pion U(4°Ar,Tr-),E=l.05 G e V / n u c l e o n ; measured a(E,0).

82Fr05 82Su01 82St13 82SuOl 82St13

82Su01 82Fr05 82Stt3 82St13 82Fr05

(4°Ar,Tr+) C(4°Ar,vr+),E=l.05 G e V / n u c l e o n ; C(4°Ar,~r+),E=535 M e V / n u c l e o n ; Cl(4°Ar,vr+),E=535 M e V / n u c l e o n ;

measured measured measured

a(E,O). a(ETr,0~r). a(E~r,O~r).

K(~°Ar,~r+),E=535 M e V / n u c l e o n ; m e a s u r e d cr(E~r,07r). Ca(4°Ar,w+),E=l.05 GeV/nucleon; measured a(E,0). U(4°Ar,vr+),E=l.O5 G e V / n u c l e o n ; measured a(E,0).

82Fr05 82Su01 82Su01

82Su01 82Fr05 82Fr05

(4°Ar,p) A g ( 4 O A r , p ) , E = 3 0 0 MeV; m e a s u r e d

cr(O,Ep),a(O,Ed),

81At20

a(E),

82Ra06

MeV; m e a s u r e d

a(E),

82Ra06

1 5 4 S m ( 4 O A r , t ) , E = I 9 6 - 3 4 0 MeV; m e a s u r e d

a(E),

82Ra06

1 5 4 S m ( 4 ° A r , p ) , E = 1 9 6 - 3 4 0 MeV; m e a s u r e d

(4°Ar,d) A g ( 4 ° A r , d ) , E = 3 0 0 MeV; m e a s u r e d

a(O,Ep),cr(O,Ed),

81Ar20

lS4Sm(4°Ar,d),E=196-340

(4°Ar,t) A g ( 4 ° A r , t ) , E = 3 0 0 MeV; m e a s u r e d

a(0,Ep),a(0,Ed),

81Ar20

(4°Ar,a) A g ( 4 ° A r , a ) , E = 3 0 0 MeV; m e a s u r e d a(0,Ep),a(0,Ed), 1 5 4 S m ( 4 ° A r , a ) , E = 1 9 6 - 3 4 0 MeV; m e a s u r e d a(E),

81Ar20 82Ra06

1 9 V A u ( 4 ° A r , a ) , E = 2 9 0 MeV; m e a s u r e d

81Vo10

a~(0),

(4OAr,4OAr') t o s p d ( 4 ° A r , 4 ° A r % E = l S 0 , 1 2 9 . 1 MeV; m e a s u r e d 11gpd(4OAr,4OAr'),E=120,129.1 MeV; m e a s u r e d

E'~,I'y, E-/,I~,

82Le07 82Le07

t S a G d ( 4 ° A r , 4 ° A r ' ) , E = 1 4 7 . 2 MeV; m e a s u r e d

Coulomb

82Jo04

(4°Ar,xn) 12C(4°Ar,xn),E(cm)=90-120 t60(4OAr,xn),E(cm)=90-120

MeV; m e a s u r e d MeV; m e a s u r e d

neutron neutron

8EJa01 t°4Pd(4°Ar,xn),E(cm)=90-120 82Ja01 ltopd(4°Ar,xn),E(em)=90-120 continued

146

MeV; m e a s u r e d MeV; m e a s u r e d

neutron neutron

82JaO1 82JaO1

REACTION

(4°Ar,xn) 5eNi(t°Ar,xn),E(cra)=90-120 6°Ni(t°Ar,xn),E(cm)=90-120 SSNi(t°Ar,xn),E(cm)=90-120 S~Ni(~°Ar,xn),E(cm)=9O-120

MeV; MeV; MeV; MeV;

measured measured measured measured

neutron neutron neutron neutron

INDEX

continued

82JaOl 82JaOl 82JaOl 82JaOl

i l a S n ( * ° A r , x n ) , E ( c m ) = 9 0 - 1 2 O MeV; m e a s u r e d

neutron

124Sn(4°Ar,xn),E(em)=90-120

measured

neutron

82JaOl 82Ja01

measured

neutron

82JaOi

MeV;

13°Te(4OAr,xn),E(cm)=90-120 MeV

(4°Ar,F) 1 5 4 S m ( 4 ° A r , F ) , E = 1 9 6 - 3 4 0 MeV; m e a s u r e d

82RaO6

a(E),

tSTAu(4OAr,F),E=343 MeV; m e a s u r e d

82Du10

(4°Ar,pF) 12SSn(4°Ar,pF),E=333 MeV; m e a s u r e d ( f r a g m e n t ) p - , 154Sm(4°Ar,pF),E=:333 MeV; m e a s u r e d ( f r a g m e n t ) p - ,

82Ri02 82Ri02

tSTAu(4°Ar,pF),E=333 MeV; m e a s u r e d

(fragment)p-,

82Ri02

(fragment)p-,

82Ri02

(fragment)p-,

82Ri02

107Au(4°Ar,aF),E=333 MeV; m e a s u r e d ( f r a g m e n t ) p - , 238U(4°Ar,aF),E=340 MeV; m e a s u r e d ~(~a,Ea),

82Ri02 82Ki06

(4°Ar,dF) 116Sn(4°Ar,dF),E=333 MeV; m e a s u r e d ( f r a g m e n t ) p - , J54Sm(4OAr,dF),E=:333 MeV; m e a s u r e d ( f r a g m e n t ) p - ,

82Ri02 82Ri02

tS~Au(4°Ar,dF),E=333 MeV; m e a s u r e d

(4°Ar,tF) n 6 S n ( 4 ° A r , t F ) , E = 3 3 3 MeV; m e a s u r e d ( f r a g m e n t ) p - , 154Sm(4°Ar,tF),E=333 MeV; m e a s u r e d ( f r a g m e n t ) p - ,

82Ri02

L97Au(4°Ar,tF),E=333 MeV; m e a s u r e d

82Ri02

(4°Ar,aF) t l S S n ( 4 ° A r , a F ) , E = 3 3 3 MeV; m e a s u r e d ( f r a g m e n t ) p - , 154Sm(4°Ar,aF),E=333 MeV; m e a s u r e d ( f r a g m e n t ) p - ,

82Ri02 82Ri02

(4°Ar,X) SBe(4°Ar,X),E=ll.4. GeV; m e a s u r e d a ( f r a g m e n t ) vs 48Ti(4°Ar,X),E=330 MeV; m e a s u r e d a ( f u s i o n ) vs O. Ag(4°Ar,X),E=300 MeV; m e a s u r e d a(e,Ep),a(O,Ed),

82Mu08 82BalO 81Ar2O

lg~Au(4°Ar,X),E=343 MeV; m e a s u r e d 2°SBi(4°Ar,X),E=255 MeV; m e a s u r e d c r ( f r a g m e n t e) vs

82Du10 82Lel~

(4°Ca,n2p) 5SNi(4°Ca,n2p),E=:35 MeV; m e a s u r e d

ET,IT,73'-coin,

82No06 (4°Ca,4°Ca')

4°Ca(4°Ca,4°Ca'),E=ld0 MeV; m e a s u r e d

a(O),

82B104

(4°Ca,xnyp) 4 ° C a ( 4 O C a , x n y p ) , E = l l 7 MeV; m e a s u r e d ET,IT,"ynn-, 5SNi(4°Ca,xnyp),E=4 M e V / n u c l e o n ; m e a s u r e d E7,]7,

82Li08 82Ku15

6 a N i ( t ° C a , x n y p ) , E = 4 M e V / n u c l e o n ; m e a s u r e d E7,I7, 83Cu(4OCa,xnyp),E=4 M e V / n u c l e o n ; m e a s u r e d E7,I7,

82Ku15 82Ku15

(4°Ca,X) 4°Ca(4OCa,X),E(cm) ~ 6 0 - 8 0 MeV; m e a s u r e d 4°Ca(4°Ca,X),E=112.5-165 MeV; m e a s u r e d a ( f u s i o n , E )

81To18 82To03

4SCa(4°Ca,X),E=330 MeV; m e a s u r e d

a(fusion)

vs e.

83Ba10

(Cr,X) 14aNd(Cr,X),E=332 t43Nd(Cr,X),E=332 144Nd(Cr,X),E=332 14SNd(Cr,X),E=332 146Nd(Cr,X),E=332 1448m(Cr,X),E=333

MeV; MeV; MeV; MeV; MeV; MeV;

measured measured measured measured measured measured

cumulative cumulative cumulative cumulative cumulative cumulative

yields, yields, yields, yields, yields, yields,

82RIO1 82Ri01 82Ri01 82Hi01 82RIO1 82Ri01

147Sm(Cr,X),E=332 14SSm(Cr,X),E=332 t4SSm(Cr,X),E=332 15°Sm(Cr,X),E=332 lSSSm(Cr,X),E=332

147

MeV; MeV; MeV; MeV; MeV;

measured measured measured measured measured

cumulative cumulative cumulative cumulative cumulative

yields, yields, yields, yields, yields,

82RIO1 82Ri01 82Ri01 82RiOl 82Ri01

REACTION

INDEX

(Fe,X) 14ZNd(Fe,X),E=356 I~4Nd(Fe,X),E=356 14eNd(Fe,X),E=356 ~eNd(Fe,X),E=356 l~eSm(Fe,X),E=356

MeV; measured MeV; m e a s u r e d MeV; measured MeV; m e a s u r e d MeV; m e a s u r e d

cumulative cumulative cumulative cumulative cumulative

yields, yields, yields, yields, yields,

8~RiOl 82RIO1 82RiOl 8~RiO1 82RIO1

l~SSm(Fe,X),E=356 l~OSm(Fe,X),E=356 la~Sm(Fe,X),E=356 I~Sm(Fe,X),E=356

MeV; MeV; MeV; MeV;

measured cumulative measured cumulative measured cumulative measured cumulative

yields, yields, yields, yields,

82RiOl 82RiOl 82RiOl 82RiOl

(5~Fe,X) l~°Sn(~eFe,X),E=330-456 MeV; m e a s u r e d ZZ~Sn(5eFe,X),E=330-456 MeV; m e a s u r e d

82B 119 82B119

~e~Ho(~Fe,X),E=462 MeV; m e a s u r e d

82Ho01

(5eNi,xnyp) ~eMo(aeNi,xnyp),E=249 .... MeV; m e a s u r e d c u m u l a t i v e OeRu(~SNi,xnyp),E=261-30~ MeV; m e a s u r e d c u m u l a t i v e 9~Ru(aaNi,xnyp),E=97.4,98.1 MeV; m e a s u r e d

82Ho04 82Ho04 82Ho04

~°°Ru(SSNi,xnyp),E=97.4,98.1 MeV; m e a s u r e d 192pd(58Ni,xnyp),E=240-302 MeV; m e a s u r e d

82Ho04 82Ho04

(5SNi,xnypza) ~°Zr(59Ni,xnypza),E=233,250 MeV; m e a s u r e d ET,IT, mZr(saNi,xnypza),E=233,250 MeV; m e a s u r e d E%I-/, 63Nb(~eNi,xnypza),E=233-250 MeV; m e a s u r e d a(E'y),

82Gu07 82Gu07 82No07

°2Mo(~eNi,xnypza),E=233-250 MeV; m e a s u r e d a(E~,), ~4Mo(SSNi,xnypza),E=233-250 MeV; m e a s u r e d a(E~/),

82No07 82No07

(58Ni,X) S2Ni(~SNi,X),E=215-275 e4Ni(SaNi,X),E=I71-215 74Ge(~SNi,X),E=171-215 9eZr(SSNi,X),E=225-285 9~Zr(SSNi,X),E=225-285

MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d a(E'y),')'T-, MeV; m e a s u r e d a(E~/),'/'/-,

82Si04 B2Be06 82Be06 8~He08 8~He08

SSNb(SeNi,X),E=225-285 MeV; m e a s u r e d 9~Mo(SSNi,X),E=225-285 MeV; m e a s u r e d 94Mo(SeNi,X),E=225-285 MeV; m e a s u r e d 9~Mo(SeNi,X),E=2R5-285 MeV; m e a s u r e d I~4Sn(SSNi,X),E=249 MeV; m e a s u r e d

cr(E~,),~,'y-, cr(E-y),~,-y-, a(E'y),-yT-, a(E'y),~/-,

82He08 83He08 83He08 82He08 82Ch08

92Mo(S2NI,X),E=225-285 MeV; m e a s u r e d a(E~'),~'5'-, a4Mo(e2Ni,X),E=225-285 MeV; m e a s u r e d a(E'y),')'V-, 9~Mo(S2Ni,X),E=225-285 MeV; m e a s u r e d q(E~),'y~,-,

82He08 82He08 82He08

(°°Ni,xnypza) ~aMo(e°Ni,xnypza),E=240-E59 MeV; m e a s u r e d a(E'/),

83No07

(62Ni,X) g2Zr(e~Ni,X),E=225-285 MeV; m e a s u r e d a(E~'),'y-y-, 94Zr(SeNi,X),E=225-285 MeV; m e a s u r e d a(E~'),VT-, g3Nb(e2Ni,X),E=225-285 MeV; m e a s u r e d a(ET),77-,

82He08 82He08 8;~He08

(Cu,X) Z4°Ce(Cu,X),E=401 *42Ce(Cu,X),E=401 142Nd(Cu,X),E=401 Z44Nd(Cu,X),E=401 14SNd(Cu,X),E=401 14SNd(Cu,X),E=401 144Sm(Cu,X),E=401 ~4SSm(Cu,X),E=401 149Sm(Cu,X),E=401

MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d MeV; m e a s u r e d

cumulative cumulative cumulative cumulative cumulative cumulative cumulative cumulative cumulative

yields, yields, yields, yields, yields, yields, yields, yields, yields,

15°Sm(Cu,X),E=40t MeV; m e a s u r e d c u m u l a t i v e y i e l d s , IS2Sm(Cu,X),E=40I MeV; measured c u m u l a t i v e yields, I~iEu(Cu,X),E=401 MeV; m e a s u r e d c u m u l a t i v e y i e l d s , 153Eu(Cu,X),E=401 MeV; m e a s u r e d c u m u l a t i v e y i e l d s , 154Gd(Cu,X),E=401 MeV; m e a s u r e d c u m u l a t i v e y i e l d s , 15eGd(Cu,X),E=401 MeV; m e a s u r e d c u m u l a t i v e y i e l d s , 15SGd(Cu,X),E=401 MeV; m e a s u r e d c u m u l a t i v e y i e l d s , Au(Cu,X),E=400 MeV; m e a s u r e d ~ , - m u l t i p l i c i t i e s .

82ttiO1 82RIO1 82RIO1 82RiOl 82RiOl 82Ri01 82RiOl 82RiOl 82RiOl

82RiOl 82RiOl 82RIO1 82RIO1 821~i01 82Ri01 82RIO1 82Be43

(SaCu,SaCu') 15~sm(aScu,SSCu'),E=154,230 MeV; m e a s u r e d (SSCu)')'154Sm(S3Cu,SaCu'),E=154,230 MeV; m e a s u r e d (63Cu)TGd(SaCu,SaCu'),E=I54,230 MeV; m e a s u r e d (SSCu)~'-, l~eGd(eSCu,eSCu'),E=154,230 MeV; m e a s u r e d (SSCu)~,-

82An I O 82An10 82AnlO 82AnlO

Dy(SSCu,eSCu'),E=154,230 MeV; m e a s u r e d (S3Cu)~'-, ISSTm(SSCu,OSCu'),E=I54,230 MeV; m e a s u r e d (eSCu)'yIr'4Yb(SSCu,e3Cu'),E=t54,230 MeV; measured (SSCu)~-

82AnlO 82An10 82AnlO

(64Ni,X) 64

Ni( 6 4 Ni,X),E=I71-215 MeV; m e a s u r e d

82Be06

74Ge(e4Ni,X),E=171-215 MeV; m e a s u r e d

148

82Be06

REACTION

INDEX

(79B r ~ 9B r' ) ~SSSm(7~Br,TaBr'),F,=200,240 MeV; m e a s u r e d (°3Cu)T~54Sm(7~Br,7aBr'),F,=200,240 MeV; m e a s u r e d (aaCu)TOd(7~Br,TaBr'),E=200,240 MeV; m e a s u r e d (S3Cu)7-, ~SGd(TaBr,TaBr'),E=200,240 MeV; m e a s u r e d (6~Cu)7-

82An10 82An10 82An10 82An10

Dy(7~Br,~gBr'),E=200,240 MeV; m e a s u r e d (6SCu)7-, lSSTm(TSBr,79Br'),E=200,240 MeV; m e a s u r e d (S3Cu)7174Yb(~OBr,7~Br'),E=200,240 MeV; m e a s u r e d (S3Cu)7-

82An10 82An10 82An10

(SlBr,StBr') ~SaSm(S~Br,S~Br'),E=200,240 MeV; m e a s u r e d (63Cu)7~S4Sm(a~Br?*Br'),E=200,240 MeV; m e a s u r e d (S3Cu)TGd(SlBr,8~Br'),E=2{10,240 MeV; m e a s u r e d (S3Cu)7-, 15~Gd(S*Br?iBr'),E=200,240 MeV; m e a s u r e d (~3Cu)7-

82An10 82An10 82An10 82An10

Dy(SlBr,alBr'),E=200,240 MeV; m e a s u r e d (SSCu)7-, l°STm(SlBr,SlBr'),E=200,240 MeV; m e a s u r e d (S3Cu)71~4yb(SIBr,8*Br'),E=200,240MeV; measured (SaCu)7-

82An10 82Ant0 82An10

(8ZK r,S ZK r' ) aTAl(SZKr,SSKr'),E=ll5,118 S4Zn(SaKr,S~Kr'),E==ll5,118 SSZn(eSKr,SaKr'),E=ll5,118 ~°Ge(SZKr,SSKr'),E=l15,118

MeV; MeV; MeV; MeV;

measured measured measured measured

Coulomb Coulomb Coulomb Coulomb

82Ke01 82Ke01 82Ke01 82Ke01

72Ge(SaKr,SaKr'),E=l15,118 ~4Ge(SSKr,SSKr'),E=l15,118 7SGe(SSKr,S~Kr'),E=l15,118

MeV; m e a s u r e d C o u l o m b MeV; m e a s u r e d C o u l o m b MeV; m e a s u r e d C o u l o m b

82KeOl 82KeOl

~SGe(S4Kr,84Kr'),E=l15,118 MeV; m e a s u r e d C o u l o m b ~4Ge(B4Kr,S4Kr'),E=II5,118MeV; measured Coulomb 76Ge(84Kr?4Kr'),E=II5,118MeV; measured Coulomb

82Ke01 82Ke01 82Ke01

82Ke01

(S4Kr,S4Kr') ~AI(O*Kr,S*Kr'),E-:II5,118 S4Zn(S4Kr,S4Kr'),E=l15,118 SSZn(e*Kr,S4Kr'),E==l15,118 7~Ge(84Kr,S4Kr'),E=l15,118

MeV; MeV; MeV; MeV;

measured measured measured measured

Coulomb Coulomb Coulomb Coulomb

82Ke01 82KeOl 82Ke01 82Ke01

(84Kr,F)

~°Zr(84Kr,F),E=12.,l M e V / n u c l e o n ; m e a s u r e d

fragment

82Ha14

16eEr(e4Kr,F),E=lS.4MeV/nucleon; measured

82Ha14

(86Kr,S6Kr)

SSSr(S~Kr,S~Kr),E=380,400 MeV; m e a s u r e d 9aZr(SSKr,SSKr),E=380,400 MeV; m e a s u r e d

~(0), ~r(0),

82Si10 82Si10

DSMo(S~Kr,SSKr),E=380,400

MeV; m e a s u r e d ¢7(0),

82Si10

(86Kr,SSKr') tVSHf(aSKr,aSKr'),E=384-594 MeV; m e a s u r e d

E7,17,

82Ha25

lS°Hf(SSKr,86Kr'),E=384-594 MeV; m e a s u r e d

E7,17,

82Ha25

(aSKr,xn) SSNi(8~Kr,xn),E n o t g i v e n ; m e a s u r e d SaNi(SaKr,xn),E n o t g i v e n ; m e a s u r e d

neutron neutron

82Ja01 82Ja01

64Ni(86Kr,xn),E not g i v e n ; m e a s u r e d

neutron

82JaOl

(86Kr,X) 8aSr(SSKr,X),E=38{3,400 MeV; m e a s u r e d 9°Zr(eSKr,X),E=38E,400 MeV; m e a s u r e d

a(O),

82Si10 82Si10

¢;(0),

92Mo(SSKr,X),E=380,400

MeV; m e a s u r e d (;(0),

82Si10

aSSU(~SMo,X),E=I4.8MeV/nueleon; measured

82Pe09

(92Mo,X) 9SMo(OaMo,X),B=148

MeV/nucleon; measured

82Pe09

(98Mo,X) gSMo(OSMo,X),E=148

MeV/nucleon; measured

IS4Sm(OeMo,X),E=12MeV/nucleon; m e a s u r e d

82Pe09

82Pe09

(1271,1271,) S3STh(lSTI 127I') E= [.I M e V / n u e l e o n ; m e a s u r e d

E7,

82Ha03

S3Su(ZaTI,lS~I'),E=4.1 M e V / n u e l e o n ; m e a s u r e d

149

ET,I 7

83Ha03

REACTION

INDEX

('SOXe,xn) ~eSi(iaSXe,xn),E=720

MeV; measured

82Hu03

DSA,ET,I 7.

(I~SXe,F) l~ZSn(l~Xe,F),E=12.5 MeV/nueleon; m e a s u r e d

82G103

ISSSn(12gXe,F),E=12.5 MeV/nueleon; m e a s u r e d

82Ha14

(136Xe,136Xe,) ~TSHf(t3SXe,136Xe'),E=384-594 MeV; m e a s u r e d EV,IT, 178Hf(13SXe?3SXe'),E=628 .... MeV; m e a s u r e d ET,IT,

82Ha25 82Ha25

lSOHf(13OXe,~SSXe'),E=384-594 MeV; m e a s u r e d E'y,I~,

82Ha25

(13°Xe,xn) ZSsi(13SXe,xn),E=740

MeV; measured

82Hu03

DSA,ET,IT.

('38Xe,X) 181Ta(ISSXe,X),E=l150 MeV; measured

E-/,IT,

82Dr04 (142Nd,142Nd')

232Th(142Nd,142Nd'),E=5.1 MeV/nucleon;

measured

ET

82Ha03

23SU(142Nd,I~2Nd'),E=5.1 MeV/nucleon; measured ET,

82Ha03

(144Sm,X) 144Sm(144Sm,X),E=1000

MeV; m e a s u r e d

81Wu03 (154Sm,X)

IS~Sm(LS4Sm,X),E=970

MeV; m e a s u r e d

81Wu03 ('SSHo,X)

16SHo(IOSHo,X),E=l.4 GeV; m e a s u r e d T - m u l t i p l i c i t y ,

82Me02 ('65Ho,aX)

ISITa(ISSHo,aX),E=I354 MeV; m e a s u r e d

82So06 (208pb,2°8pb')

i°4Ru(2°6Pb,2°spb'),E=4.6 MeV/nucleon; m e a s u r e d 232Th(S°spb,2°sPb'T),E=5.3 MeV/nucleon; m e a s u r e d

82St09 820w01

234U(2°ePb,Z°sPb'T),E=5.3 23Su(2°sPb,2°ePb'~,),E=5.3

MeV/nucleon; m e a s u r e d MeV/nucleon; m e a s u r e d

820w01 820w01

(2°sPb,X) Z6Mg(2°spb,X),E=5.2-8 Z~Al(S°sPb,X),E=5.2-8 4SCa(a°ePb,X),E=5.2-8 S°Ti(2°sPb,X),E=5.2-8

MeV/nucleon; MeV/nucleon; MeV/nucleon; MeV/nucleon;

measured measured measured measured

82Bo29 B2Bo29 82Bo29 82Bo29

52Cr(S°spb,X),E=5.2-8 MeV/nucleon; m e a s u r e d 58Fe(2°sPb,X),E=5.2-8 MeV/nucleon; m e a s u r e d S4Ni(~Oepb,X),E=5.2-8 MeV/nucleon; m e a s u r e d 23Su(S°spb,X),E=8 MeV/nueleon; m e a s u r e d Ea,la,SF

82Bo29 82Bo29 82Bo29 81Lu06

(e3eTh,e3ZTh') 2ospb(~32Th,a32Th'),E=5.6

MeV/nucleon; m e a s u r e d ET

82si03 (U,F)

Au(U,F),E=10 MeV/nueleon; m e a s u r e d Pb(U,F),E=IO MeV/nueleon; m e a s u r e d

82De25 82De25

U(U,F),E=10 MeV/nucleon; m e a s u r e d

150

82De35

REACTION

INDEX

(a38U,X) e4eCm(238U,X),E=7.4 MeV/nucleon; measured

82Sc05

151

REFERENCES

78An28

78An29

78Av08

78Ba81 78Bo41

78De42

78Ef02 78Go21 78Gu27

781v03 78Ka40 78Pr10 78Ri07 78Vi04

78Za12 79Ce04 79Ch40

79Ch41 79Ch42

79Ne09 79Re09 79Sh25

79Su14

79Su15

79Wa24

79Zy04

A.E.Antropov, V.P.Gusev, P.P.Zarubin, P.D.Ioannu - Probl.Yad.Fiz.Kosm.Luchei 8, 25 ( 1 9 7 8 ) A Study of Excitation Functions of Chromium a n d I r o n I s o t o p e s (I) A.E.Antropov, V.P.Gusev, P.P.Zarubin, P.D.Ioannu, B.N.Orlov Probl.Yad.Fiz.Kosm.Luchei 8, 31 (1978) Proton Scattering b y 5iV (II) V.D.Avchukhov, M.R.Akhmed, M.A.A1-Amili, S.AI-Nadzhar, K.A.Baskova, A.B.Vovk, L.I.Govor, A.M.Demidov, M.M.Komkov, N.Rammo - Probl.Yad.Fiz.Kosm.Luchei 8, 18 (1978) De-Excitation of the nSIn Levels in (n,n'7) Reaction M.I.Babenkov, B.V.Bobykin, V.S.Zhdanov, V.K.Petukhov - Probl.Yad.Fiz.Kosm.Luehei 8, 36 ( 1 9 7 8 ) The K-LX, K-MX and K-NX Auger Transitions i n 13*Xe S.P.Borovlev, G.V.Danilyan, V.V.Novitskij, V.S.Pavlov - Probl.Yad.Fiz.Kosm.Luchei 8, 93 (1978) Circular Polarization of 7 R a y s i n t h e *35Ba(n,T0) a n d laVBa(n,T0) R e a c t i o n s o n P o l a r i z e d T h e r m a l Neutrons A.M.Demidov, L.I.Govor, M.R.Akhmed, Ya.S.AI-Shiraida, S.A1-Nadzhar, M.A.AI-Amili Probl.Yad.Fiz.Kosm.Luchei 8, 113 ( 1 9 7 8 ) A Study of 7 Transitions i n 152,1~4Sm w i t h F a s t P i l e N e u t r o n s V.P.Efrosinin, Yu.G.Kudenko, R.M.Musaelyan, V.I.Popov - Probl.Yad.Fiz.Kosm.Luchei 8, 121 (1978) Excitation of the Collective States of Germanium in Inelastic Scattering of Low-Energy Neutrons V.G.Gonchar, V.V.Tokarevskij - Probl.Yad.Fiz.Kosm.Luchei 8, 15 (1978) Search for Possible Spin-Orbital Effects in Elastic Scattering o f 27.2 MeV A l p h a P a r t i c l e s b y Sip G . M . G u r e v i c h , L . E . L a z a r e v a , V.M.Mazu, G . V . S o l o d u k h o v , V.A.Tyutin - Probl.Yad.Fiz.Kosm.Luehei 8, 106 (1978) Total Photoabsorption Cross-Section o f 76Se a n d e a s e i n t h e G i a n t D i p o l e R e s o n a n c e R e g i o n M.A.Ivanov, I.Kh.Lemberg, A.S.Mishin - Probl.Yad.Fiz.Kosm.Luchei 8, 54 (1978) Lifetimes o f t h e 69As E x c i t e d S t a t e s F e d i n H e a v y - I o n Reactions M.Kase, J . K i k u c h i , T.Doke - Nucl.Instrum.Methods 154, 335 ( 1 9 7 8 ) Half-Life o f 2aSU S p o n t a n e o u s Fission and Its Fragment Kinetic Energies G.A.Prokopets, B.Kholmkvist, A.V.Murzin - Probl.Yad.Fiz.Kosm.Luchei 8, 76 (1978) T h e 19F(n,XT) R e a c t i o n s i n t h e 1 6 - 2 2 MeV R a n g e o f N e u t r o n Energy D.M.de C . R i z z o - A n n . A c a d . B r a s i l . C i e n c . 50, 303 (1978) Fissao Espontanea d o 2aSU e M e d i d a d a s u a C o n s t a n t e de Desintegracao L.I.Vinogradov, O.V.Chubinskij, Yu.F.Andronov, F.M.Ehl-Ashri, L.V.Gustova, Yu.V.Kangropol Probl.Yad.Fiz.Kosm.Luchei 8, 96 ( 1 9 7 8 ) Spin-Flip in Inelastic Scattering o f 6 MeV P r o t o n s b y 24Mg a n d 2SSi P.P.Zarubin, R.Mikhu - Probl.Yad.Fiz.Kosm.Luchei 8, 51 (1978) Conversion Electrons from the l°spd(p,nT)l°SAg Reaction A.Cesana, G.Sandrelli, V.Sangiust, M.Terrani - Energ.Nucl.(Milan) 26, 526 ( 1 9 7 9 ) Gamma-Ray S p e c t r a o f 233U,2a~Np,238,a39,24°,a41pu,a41Am S a m p l e s Chang Huan-Qiao, Liu Zu-Hua - Chin.J.Nucl.Phys. i, 9 (1979) T h e M e a s u r e m e n t of t h e A v e r a g e N u m b e r of P r o m p t N e u t r o n s a n d t h e D i s t r i b u t i o n of P r o m p t N e u t r o n Numbers f o r 252Cf S p o n t a n e o u s Fission Chang Huan-Qiao, Xu J i n - C h e n g , Wen Tong-Qing - Chin.J.Nucl.Phys. I, 21 ( 1 9 7 9 ) Determination of the Half-Lives of a Disintegration and Spontaneous F i s s i o n o f 242Cm C h u Y u n g - T a i , F a n G u o - Y i n g , Wu Z h o n g - L i , F e n g E n - P u , L i a n g G u o - Z h a o , Li F a - W e i , J i a o D u n - L o n g , Li X i a n - H u i , G u o Y i n g - X i a n g , X i a G u o - Z h o n g , S u Y i n g - Q u a n , X i a o Q i n - P i a n - C h i n . J . N u c l . P h y s . i, 31 (1979) The Research of Scattering and Transfer R e a c t i o n o f 12C w i t h 12C W.Neumann, L.Cleemann, J.Eberth, N.Wiehl, V.Zobel - Nucl.lnstrum.Methods 164, 539 ( 1 9 7 9 ) Details of Conversion Electron Spectroscopy with Mini-Orange Spectrometers R . C . R e e d y , G . F . H e r z o g , E . K . J e s s b e r g e r - E a r t h P l a n e t . S c i . L e t t . 4 4 , 341 (1979) T h e R e a c t i o n M g ( n , a ) N e a t 14.1 a n d 14.7 MeV: C r o s s s e c t i o n s a n d i m p l i c a t i o n s for meteorites Shi Zong-Ren, Shi Xia-Min, Zeng Xian-Tang, Lu Z h i - R o n g , Xing Jin-Qiang, Shen Rong-Lin, Ding Da-Zhao - Chin.J.Nucl.Phys. I, 4 5 ( 1 9 7 9 ) Gamma-Ray Production Cross Sections from Interactions o f 14.9 MeV N e u t r o n s w i t h C,F,AI,Si,Fe a n d Cu S u n H a n - C h e n g , Yao J i n - Z h a n g , S u n T s u - X u n , Wen K e - L i n g , Lu H u i - J u n , Dai N e n g - X i o x g , J i n R o n g - H u a , Yah Chen - Chin.J.Nucl.Phys. i, 1 ( 1 9 7 9 ) d + eLi a n d a + eLi Q u a s i - F r e e P r o c e s s e s a t Low E n e r g i e s Sun Xiang-Fu, Pan Zong-You, Yuan Shuang-Gui, Xu Guo-Jun - Chin.J.Nucl.Phys. I, 93 ( 1 9 7 9 ) Determination of t h e L i f e t i m e of E x c i t e d C o m p o u n d N u c l e i f r o m 12C + 19TAB R e a c t i o n b y B l o c k i n g effect W a n g X i n - L i n , W a n g S h u - M a o , Mao Z h e n - L i n , W a n g F a n g - L i n , C e ng P i n - L i u - C h i n . J . N u c l . P h y s . I, 63 (1979) Deuteron-lnduced R e a c t i o n s o n 12C a t B o m b a r d i n g E n e r g y o f 9 MeV J . L . Z y s k i n d , J . M . D a v i d s o n , M . T . E s a t , M . H . S h a p i r o , R . H . S p e a r - N u e l . P h y s . A331, 180 ( 1 9 7 9 ) Competition Cusps in (a,7) Reactions

152

REFERENCES

80Ad08

M.Adilbish,

M.I.Fominykh,

V.A.Khalbin,

O.Knotek,

N.G.Zaitseva

-

Radiochem.Radioanal.Lett.

45,

227 (1980)

80Ar23 80Ba64

80Ch38

Cumulative C r o s s - S e c t i o n s 2°°T1,2°lTI,2°2T1 P r o d u c t i o n i n 660 MeV P r o t o n - I n d u c e d S p a l l a t i o n o f L ead and Bismuth C.Ardisson, M.Valladon, J.Vernois, G.Ardisson - Radiochem.Radioanal.Lett. 45, 41 (198 0 ) Mesure des Rayonnements 7 Associes a la Desintegration p a r C a p t u r e d e 234Np Bai X i x i a n g , Wen Shenlin, S u n D a z e , Li A n l i , C h e n G u a n r e n , Huang Tangzi, Sun Fengxian Chin.J.Nucl.Phys. 2, 327 (19 80) The Angular Distribution for Elastic Scattering o f 14.7 MeV N e u t r o n s by Deuterons and the Neutron Spectra from the Break-Up of Deuterons ( : h e n S h i p i n g , L i u F e n g y i n g , Z h o u Li ng, Y a n g C h u n x i a n g , Li G u a n g s h e n g , Weng P e i k u n , Z h a n g Y o u f a n g Chin.J.Nucl.Phys. 2, 382 ( 1 9 8 0 ) 7,-Ray Spectrum f r o m 147Nd D e c a y A.S.Deinenko, I.I.Zalyubovsky, I.Ya.Malakhov, V.D.Sarana, V.E.Storizhko, N.A.Shlyakhov Izv.Akad.Nauk SSSR, S e r . F i z . 4 4 , 2 6 5 2 (1980); B u l l . A c a d . S c i . U S S R , P h y s . S e r . 4 4 , No.12, 163 ( 1 9 8 0 ) Features o f t h e R e a c t i o n 9 B e ( d ( p o l ) , p ) l ° B e a t Low P o l a r i z e d - D e u t e r o n Energies F a n P e i g u o , Lu H a n l i n , Li J i z h o u , H u a n g J i a n z h o u - Chin.J.Nucl.Phys. 2, 337 (1980) The Broad Structure in the Excitation Curve of 115In(n,n')llSmIn Reaction V.A.Goldshtein, R.I.Dzhibuti, R.Ya.Kezerashvili, E.L.Kuplennikov Izv.Akad.Nauk SSSR, S e r . F i z . 4 4 , 2 6 5 5 (1980); B u l l . A c a d . S c i . U S S R , P h y s . S e r . 4 4 , No.12, 166 (1980) Quasi-elastic Scattering of Electrons b y 4He N u c l e u s w i t h R e c o r d i n g o f e p C o i n c i d e n c e s R.Hanninen, J.Raisanen, A.Anttila - Radiochem.Radioanal.Lett. 4 4 , 201 (1980) F,l e m e n t a l A n a l y s i s o f Li a n d B w i t h P r o t o n I n d u c e d 7-Ray Reactions Huang Jianzhou, Lu H a n l i n , Li J i z h o u , F a n P e i g u o - C h i n . J . N u c l . P h y s . 2, 213 (1980) F,x c i t a t i o n Curve Measurement f o r t h e R e a c t i o n 89Y (n,2n)S S Y l,.Jarczyk, B.Kamys, K.Seliger, Z.Wrobel, J.Lang, R.Muller, C.M.Schweizer-Teodorescu Acta P h y s . P o l . B l l , 641 (1980) Investigation of Nucleon-Unbound S t a t e s i n 29Si a n d 2Sp b y t h e R e a c t i o n 2 S S i ( d , p n ) G.D.Jones, L.P.Ekstrom, F.Kearns, T.P.Morrison, P.J.Twin, R.Wadsworth, N.J.Ward, B.Collinge, C.L.Wilkinson - Nucl.lnstrum.Methods 178, 581 (1980) An On-Line Computer Controlled Time Digitizer for Half-Life Measurements Liu Zuhua, Zhang Huanqiao - Chin.J.Nucl.Phys. 2, 53 (1980) T h e D i s t r i b u t i o n of P r o m p t N e u t r o n N u m b e r s f o r Long R a n g e s - P a r t i c l e - A c c o m p a n i e d F i s s i o n o f 252Cf Li Q i n g l i , L u F u b a o , Hart S h u k u i , G u o Q i n g j i a n g , Li Z h i c h a n g , Chert Ruixie, Dang Zhijia, Jiang Chenglie - Chin.J.Nucl.Phys. 2, 316 ( 1 9 8 0 ) Intermediate R e s o n a n c e s i n t h e R e g i o n of D e u t e r o n E n e r g y f r o m 1.0 t o 2.5 MeV i n t h e 28Si(d,p)~9Si Reaction L u H a n l i n , Li J i z h o u , F a n P e i g u o , H u a n g J i a n z h o u - Chin.J.Nucl.Phys. 2, 286 (1980) Measurement of Cross Section for the Reaction 55Mn(n,2n)54Mn Ma H o n g c h a n g , Li J i z h o u , H u a n g J i a n z h o u , F a n P e i g u o , Lu H a n l i n - C h i n . J . N u c l . P h y s . 2, 4 7 (1980) Measurement of Cross Section for the Reaction 45Sc(n,2n)44mSe and Isomeric Cross Section Ratio -

80De45

80Fa20 80Go21

80Ha55 80Hul5 8OJal8

80Joll

80Li20 80Li21

80Lu09 80Ma47

o'(m)/o'(g) 80Ma48 800m01 80Ru03

80Sh28

80Yal0

80Yall

80Ya12

Ma W e i y i , W a n g Dao, Y a n C h e n , S u n H a n c h e n g - Chin.J.Nucl.Phys. 2, 239 (1980) ~Li(d,n) Neutron Spectra and the 7Li(d,2a)n Reaction Induced b y 13.2 MeV D e u t e r o n s T . O m o r i , M.Yagi, H . Y a m a z a k i , T . S h i o k a w a - Radiochem.Radioanal.Lett. 4 4 , 307 ( 1 9 8 0 ) Excitation Functions for 3He-Induced Reactions on Silver W.D.Ruhter, D.C.Camp - Nucl.Instrum.Methods 173, 4 8 9 (1980) Directional-Correlation R e s u l t s f o r 134Ba a n d n ° C d u s i n g a M e g a c h a n n e l G a m m a - G a m m a Coincidence System A.K.Sharma, Ravinder Kaur, H.R.Verma, K.K.Suri, P.N.Trehan - Proc.Indian N a t l . S c i . A c a d . 4 6 A , 181 (1980) D e c a y o f 56Co t o L e v e l s i n 56Fe Yang Chunxiang, Li G u a n g s h e n g , Weng Peikun, Cheng Shiping, Liou Fengyeng, Zhou Ling, Zhang Youfang - Chin.J.Nucl.Phys. 2, 41 (1980) T h e D e c a y o f 99Mo Y a n C h e n , S u n H a n c h e n g , Na X i a n g y i n , Ma W e i y i , C u i Y u n f e n g , H u X u a n w e n - C h i n . J . N u c l . P h y s . 2, 137 (1980) The Neutron Spectra of 7Li(d,n) Reaction Induced b y 4 0 0 ~ 1200 k e V D e u t e r o n s Yang Jinqing, Ni X i n b a i , C h a n g Y i n g q i , J i a n g D a z h e n , C h e n g X i a o w u - C h i n . J . N u c l . P h y s . 2, 155

(1980) 80Ye02 80Yu01

(,~,p) R e a c t i o n s I n d u c e d b y 31.2 MeV c~ P a r t i c l e s Ye B i n q i , Wen K e l i n g , Z h a n g P e i h u a , Y u a n R o n g f a n g , H u a n B i n g y i n - C h i n . J . N u c l . P h y s . 2, 147 (1980) Interaction o f 9.05 MeV D e u t e r o n s o n 7Li N u c l e u s Yu Jusheng, W a n g S u f a n g , T i a n Y u h o n g , H o u M i n g d o n g , Mi a o D e g u i , Z e n g W e n b i n g , Li G u a n g w e i Chin.J.Nucl.Phys. 2, 19 ( 1 9 8 0 ) Study of the Fission of the Excited Nuclei near Radium

153

REFERENCES

80Zh04

80Zh05 80Zu02 81Ab06

8lAb07

81Ac02

8lAg08

81Ah05 81A123

81A126 81A127

81A128

81An20

81An21 81An23

81An24 81An25

8lAp01

81Ar2O

81Ar23

81Ar24

81AuO9

Zhang Huanqiao, Xu Jincheng, Liu Zuhua, Wen T o n g q i n g , Ding Shengyao, Chen Zhicai C h i n . J . N u c l . P h y s . 2, 29 (1980) T h e D e p e n d e n c e o f A v e r a g e N u m b e r s o f P r o m p t F i s s i o n N e u t r o n of 239pu o n I n c i d e n t F a s t N e u t r o n Energies Z h a n g P e i h u a , S u n Z u h s u n , Wen Keling, Wang F a n g l i n , Wang S h u m a o - C h i n . J . N u c l . P h y s . 2, 219 (1980) Quasi-free S c a t t e r i n g i n 6,~Li(cx,2a)2,aH R e a c t i o n s a t Low E n e r g y E.Zupranska, K.Rusek, J.Turkiewicz, P.Zupranski - A c t s P h y s . P o l . Bll, 853 (1980) Excitation Functions f o r ( n , a ) R e a c t i o n s i n t h e N e u t r o n E n e r g y R a n g e f r o m 13 to 18 MeV B.M.Abramov, l.A.Dukhovskoy, V.V.Kishkurno, A.P.Krutenkova, V.V.Kulikov, M.A.Matsyuk, I . A . R a d k e v i c h , E . N . T u r d a k i n a , E . A . A y r a p e t o v , L . S . B a g d a s a r y a n - N u c l . P h y s . A372, 301 (1981) E n e r g y D e p e n d e n c e o f B a c k w a r d 7r-d E l a s t i c S c a t t e r i n g i n t h e 1 - 2 GeY R e g i o n M.A.Abou-Leila, l.Brancus, A.Buta, C.Grama, S.U.El-Kameesy, I.Lazar, I.Mihai, M.Petrascu, M . P e t r o v i c i , V . S i m i o n - F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 1 , 39 (1981) R e s o n a n t B e h a v i o u r o f 24Mg(lZC,(~)32S R e a c t i o n i n t h e E n e r g y R a n g e 2 1 . 8 - 2 6 . 0 MeV K.Ackermann, K.Bangert, U.E.P.Berg, G.Junghans, R.K.M.Schneider, R.Stock, K.Wienhard N u c l . P h y s . A372, 1 (1981) Ground State Dipole Transitions i n 5eNi S.K.Aggarwal, A.V.Jadhav, S.A.Chitambar, K.Raghuraman, S.N.Acharya, A.R.Parab, C.K.Sivaramakrishnan, H.C.Jain - Radiochem.Radioanal.Lett. 46, 69 (1981) H a l f - L i f e of 2aepu S . A . A h m a d , A . V e n u g o p a l a n , G . D . S a k s e n a - I n d i a n J . P u r e A p p l . P h y s . 19, 1183 (1981) Isotope Shifts in Lines of the First Spectrum of Dysprosium in the 4125-4685 A° Region G.D.Alkhazov, E.E.Berlovich, K.A.Mezilev, Yu.N.Novikov, V.N.Panteleev, A.G.Polyakov, V.P.Afanasev, N.Ganbaatar, K.Ya.Gromov, V.G.Kalinnikov, Ya.Kormitski, A.Lyatushinski, A.Potempa, F.Tarkani, Yu.V.Yushkevich - I z v . A k a d . N a u k SSSR, S e r . F i z . 45, 1827 (1981) New N u c l i d e s 145Tb a n d 14SDy N . A l a m a n o s , C.Le M e t a y e r , C.Levi, W.Mittig, L . P a p i n e a u - F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 1 , 43 (1981) (12C + 2asi) R e a c t i o n s L e a d i n g to 3aS F i n a l S t a t e s N.Alamanos, J.Arvieux, B.Berthier, B.Bonin, G.Bruge, J.L.Escudie, H.Faraggi, L.Farvacque, D.Legrand, J.C.Lugol, W.Mittig, L.Papineau, M.Buenerd, M.LeVine, D.K.Scott, A.I.Yavin F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 1 , 83 (1981) E l a s t i c a n d I n e l a s t i c S c a t t e r i n g ( G i a n t R e s o n a n c e s ) o f 120 M e V / A A l p h a P a r t i c l e s V.P.Alfimenkov, S . B . B o r z a k o v , Vo V a n T k h u a n , Yu.D.Mareev, L.B.Pikelner, D.Rubin, A.S.Khrykin, E . I . S h a r a p o v - P i s m a Z h . E k s p . T e o r . F i z . 34, 308 (1981); J E T P L e t t . ( U S S R ) 34, 295 (1981) Experimental Study of P-Par ity Nonconservation i n t h e N e u t r o n R e s o n a n c e o f llTSn L.E.Antonuk, D.Bovet, E.Bovet, J.-P.Egger, F.Goetz, P.Gretillat, C.Lunke, E.Schwarz, C.Perrin, J.-P.Perroud, G . S . B l a n p i e d , B . M . P r e e d o m - H e l v . P h y s . A c t a 54, 327 (1981) D i f f u s i o n Q u a s i L i b r e de P i o n s G.Andritsopoulos, W . N . C a t f o r d , E . F . G a r m a n , D . M . P r i n g l e , L . K . F i f i e l d - N u c l . P h y s . A372, 281 (1981) S t a t e s i n 21Ne v i a t h e lZC(laC,aT)21Ne R e a c t i o n M . R . A n d e r s o n , S . R . K e n n e t t , M . E . S e v i o r , D . G . S a r g o o d - A u s t . J . P h y s . 34, 105 (1981) 4~Sc(p,p')45Sc * a n d t h e A t t a i n m e n t of a T h e r m a l Distribution of States in an Astrophysical Environment B . A n t o l k o v i c , G.Paic, R . J . P e t e r s o n - F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 2 , 31 (1981) Fragmentation o f t h e 7Li + 3He S y s t e m a t E(aHe) = 42.9 MeV V.A.Anufriev, S.I.Babich, N.G.Kocherygin, V.M.Lebedev, S.N.Nikolsky, V.N.Nefedov, V.M.Nikolaev, V . A . P o r u c h i k o v , A . A . E l e s i n - A t . E n e r g . 51, 330 (1981); S o v . A t . E n e r g y 51, 736 (1981) Measurement of the Total N e utron Cross S e c tions a nd Re s ona nc e P a ra m e te rs o f 243Cm i n t h e O.4-66-eV Energy Region E.Aprile, C.Eisenegger, R.Hausammann, E.Heer, R.Hess, C.Lechanoine-Leluc, W.R.Leo, S . M a n g o , S . M o r e n z o n i , Y.Onel, D . R a p i n - H e l v . P h y s . A c t a 54, 311 (1981) A Direct Experimental Reconstruction of t h e p p Elastic S c a t t e r i n g A . G . A r t u k h , G . F . G r i d n e v , M . G r u s z e c k i , W.Karcz, A . N . M e z e n t s e v , V . L . M i h k e e v , L . P o m o r s k i , A . P o p e s c u , D . G . P o p e s c u , V . V . V o l k o v - Z . P h y s . A303, 41 (1981) Multi-Nucleon Transfer Reactions and the Formation of Light C h a r g e d P a r t i c l e s in t h e System A g ( n a t ) + 4 ° A r (285 MeV) Yu.M.Arkatov, P.I.Vatset, V.I.Voloschyk, V.N.Gurev, V.A.Zolenko, i.M.Prokhorets - U k r . F i z . Z h . 26, 1774 (1981) Quadrupole Resonance 7-Absorption in t h e R e a c t i o n 4He(7,n)3He Z.Arvay, T.Fenyes, J.Gulyas, T.Kibedi, E.Koltay, A.Krasznahorkay, S.Laszlo, B.D.Kern, V.Paar, S . B r a n t , Z . H l o u s e k - F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 2 , 38 (1981) T h e S t r u c t u r e of *°°Tc a n d 96Nb f r o m l°SMo(p,nT)i°°Tc a n d aSZr(p,nT)gBNb R e a c t i o n s a n d t h e P a r a b o l i c Rule V.Augustynyak, L.Glovatska, Zh.Dalmas, L.Zemlo, Ya.Turkevich, M . Y a s k u l a , Le V a n K k h o i I z v . A k a d . N a u k SSSR, S e r . F i z . 45, 2172 (1981) S t u d y of E n e r g y a n d A n g u l a r D i s t r i b u t i o n of a - P a r t i c l e s i n t h e R e a c t i o n 143Nd(n,a)14°Ce I n d u c e d b y Fast Neutrons

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81AulO 81Av04

8lAy05

81Ba54

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81Be53 81Be54

81Be55

81Be56

81Be57 81Be60 81Be62

81Be64

81Bi16

81Bi17 81Bj04

81BI15 81Bo37

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L e t t . 47, 1823 (1981) Test of Data-to-Data R e l a t i o n s f o r t h e R e a c t i o n s 9 ° , 9 a Z r ( p ( p o l ) , p ' ) a t 800 MeV J.Barrette, E.Deuring, Z.Fraenkel, H.Lehr, I.Tserruya, S . W a l d - P h y s . R e v . C24, 2731 (1981) S e a r c h f o r a L o w - 1 W i n d o w L e a d i n g t o Deep I n e l a s t i c S c a t t e r i n g o f 160 + 160 a t E ( c . m . ) = 32.1 MeV C,Bauer, H.Richter, P.Gippner, R.Mann, W.Rudolph, B.Eckhardt, K . O . G r o e n e v e l d - Z . P h y s . A 3 0 3 , 13 (1981) L-Shell Vacancy Production in Ag,Ta,and Au for Incident I o n s Z l < 10 i n t h e E n e r g y R a n g e o f 0.125-4 MeV/amu H.W.Baer, J.A.Bistirlich, K.M.Crowe, W.Dahme, C.Joseph, J.P.Perroud, M.Lebrun, C.J.Martoff, U.Straumann, P.Truol - Helv.Phys.Acta 54, 314 (1981) T = 2 States in the A = 14-System: Radiative P i o n C a p t u r e i n 14C P . H . B a r k e r , T.B.Ko, M . J . S c a n d l e - N u c l . P h y s . 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C24, 2401 (1981) Ghost Anomaly in abe Studied w i t h 9 B e ( p , d ) a t E ( p ) = 14.3 a n d 26.2 MeV C.E.Bemis,Jr., F.K.McGowan, J.L.C.Ford,Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Phys.Rev. C24, 2 7 2 3 (1981) Coulomb Excitation of Rotational States and Ground-State Quadrupole Moment for 243Am G.Bellia, L.Calabretta, A . D e l Z o p p o , E . M i g n e e o , G . R u s s o , R . C . B a r n a , D.De P a s q u a l e Phys.Rev. C24, 2 7 6 2 (1981) Shelf Effect in the Subthreshold Photofission o f 2a2Th C.L.Bennett, A.L.Hallin, R.A.Naumann, P.T.Springer, M.S.Witherell, R.E.Chrien, P.A.Baisden, D . H . S i s s o n - P h y s . L e t t . 107B, 19 (1981) The X-ray Spectrum f o l l o w i n g 163Ho M E l e c t r o n C a p t u r e F.Becvar, J.Honzatko, M.Kralik, Nguyen Dang Nhuan, S.A.Telezhnikov - Y a d . F i z . 34, 1158 (1981) Investigation o f t h e R e a c t i o n 154Gd(n,~/)155Gd a t I s o l a t e d R e s o n a n c e s H.W.Becker, K.U.Kettner, C.Rolfs, H.P.Trautvetter - Z . P h y s . 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81Br28

81Br29

81Br3O 81Bu22 81Bu23 81Bu24

81Bu25

81Bu26

81Bu27 81Ca16 81Ca17

81Ce06 81Ch32 81Ch34 81Ch35 81Ch36 81Ch37

81Ch38

81Ch39

V.A.Bondarenko, E.P.Grigorev, P.T.Prokofev - Izv.Akad.Nauk SSSR, S e r . F i z . 45, 2141 (1981) -/-Radiation from the Reaction (n,n'7) on Even-Even Er I s o t o p e s N.S.Borisov, V.G.Vovchenko, V.A.Efimovyh, A.A.Zhdanov, M.Yu.Kazarinov, Yu.M.Kazarinov, Yu.F.Kiselev, A.I.Kovalev, M.Yu.Liburg, B.S.Neganov, V.V.Polyakov, V.E.Popov, A.N.Prokofiev, V.Yu.Trautman, Yu.A.Usov, A.V.Shvedchikov - Z h . E k s p . T e o r . F i z . 81, 1583 (1981) Investigation of Energy Dependence of Spin-Spin Correlation in the Diproton Resonance Range M.Bogdanovic, R.Brissot, G.Barreau, K.Schreckenbach, S.Kerr, I.A.Kondurov, Yu.E.Loginov, V.V.Martynov, P.A.Sushkov - Fizika(Zagreb) 13, S u p p l . 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81Erl2

81EyO2 81FaO8

81Fi06 81Fi07 81F106

81Fo13

81Fr24 81Fr26 81Fu12

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81Ko43

81Kr20

Half-Life a n d M a g n e t i c M o m e n t o f a 7 / 2 + L e v e l i n t2aTe V.A.Ionescu, &Kern, C.Nordmann, S.Olbrich, W.Reichart - Nucl.lnstrum.Methods 190, 19 (1981) Improved Analysis of T-Ray Angular Distributions in (Particle,xn) Experiments B.S.Ishkhanov, Yu.A.Novikov, E.S.Omarov, I.M.Piskarev Yad.Flz. 33, 570 (1981); Sov.J.Nucl.Phys. 33, 296 (1981) Partial Cross Sections for Various Channels of the 52Cr(')',X~/')Reaction H.A.tsmail, H.Hanafi, M.Morsy, A.Nada, H.Abu-Leila - Acta Phys.Acad.Sci.Hung. 50, 391 (1981) The Radioactive D e c a y o f lS2Eu H.A.Ismail, A.E1-Naem, S.A.Et-Malalk, H.Abou Leila, N.Wali-E1-Din - Rev.Roum.Phys. 26, 461 (1981) The Ground S t a t e B a n d s i n 152Sm a n d 16°Dy T.Iwashita - J.Phys.Soc.Jpn. 50, 3191 (1981) Gamma-Gamma Directional Correlation i n t h e D e c a y o f 168Tm R.V.F.Janssens, M.J.A.de Voigt, H.Sakai, H.J.M.Aarts, C.J.van der Poel, H.F.R.Arciszewski, D.E.C.Scherpenzeel, J.Vervier - P h y s . L e t t . 106B, 4 7 5 (1981) Backbending i n t67Hf a n d 16SHf a n d t h e B a n d - C r o s s i n g Picture B.Jeckelmann, J.Kern, U.Kiebele, J.-A.Pinston, R.Weber, B.Aas, W.Beer, I.Beltrami, K.Bos, G.deChambrier, P.F.A.Goudsmit, Th.V.Ledebur, H.J.Leisi, W.Ruckstuhl, G.Strassner, A.Vacchi Helv.Phys.Acta 54-, 321 (1981) Spektroskopische Quadrupolmomente y o n 2SMg u n d 27A1 a u s M u o n i s c h e n X-Ray Ubergangen D.T.Jost, H.R.Von Gunten - J.Inorg.Nucl.Chem. 43, 2 6 2 9 (1981) Independent Y i e l d s o f 92mNb i n t h e T h e r m a l Neutron-lnduced F i s s i o n of 233U,235U a n d 239pu R.Julin, J.Kantele, M.Luontama, A . P a s s o j a - Z . P h y s . A 303, 147 (1981) D e c a y o f 0+2 S t a t e s i n 8e,~2,94Zr a n d E0 S y s t e m a t i c s o f Zr I s o t o p e s J.Kallne, J.Davis, R.C.Minehart, R.R.Whitney, R.L.Boudrie, J.B.McClelland, A.W.Stetz &Phys.(London) G7, L287 (1981) T h e (Tr+,p) R e a c t i o n s a n d N u c l e a r p p a n d p n C o r r e l a t i o n s J . K a l l n e , R . R . W h i t n e y - P h y s . L e t t . 107B, 23 (1981) Manifestations of Pion-Nucleon Scattering in Nuclear Pion Absorption V . I . K a s i l o v , N . I . L a p i n - Y a d . F i z . 34, 865 (1981) Anisotropy in Angular Distributions of Fission Fragments o f 2aSU N u c l e i I n d u c e d by Photons Emitted by High-Energy Electrons Interacting with a Monocrystal o f Si D.K.Kaipov, Yu.G.Kosyak, Yu.A.Lysikov - Izv.Akad.Nauk SSSR, S e r . F i z . 45, 1889 (1981) Lifetimes a n d S p i n s o f E x c i t e d S t a t e s o f S5Mn A.F.Khodyachikh, P.l.Vatset, V.N.Gurev, I.V.Dogyust, V.V.Kirichenko - Y a d . F i z . 34, 1 4 2 5 (1981); Sov.J.Nucl.Phys. 34, 789 (1981) Momentum Distribution of Quasideuterons in the p-Shell of the Carbon Nucleus l.A.Kondurov, E.M.Korotkikh, Y u , V . P e t r o v , G . I . S h u l j a k - P h y s . L e t t . l(]6B, 383 (1981) Acceleration of Thermal Neutrons b y I s o m e r i c N u c l e i (18°mHf) M . K o z l o w s k i , H . H . M u e l l e r , R . W a g n e r - P h y s . L e t t . 107B, 27 (1981) Analyzing Power for the (p(pol),ax) Reaction in the Continuum a t Ep = 72 MeV H.-G.Korber, R.Beckmann, D . F r o h l i n g , U . H o l m - N u c l . P h y s . A 372, 109 (1981) Analyzing P o w e r o f t h e 3 H e ( p o l ) ( 3 H e , p ) 5 L i ( 3 / 2 - ) R e a c t i o n a t 14 MeV I.A.Korzh, V.P.Lunev, V.A.Mishchenko, E.N.Mozhzhukhin, M.V.Pasechnik, N.M.Pravdivyi - At.Energ. 50, 398 (1981); S o v . A t . E n e r g y 50, 359 (1981) Angular Distributions of Neutrons with 5-7-MeV Energy Elastically and Inelastically Scattered by Nickel Isotopes E.A.Kolomensky, V.M.Lobashev, A.N.Pirozhkov, L.M.Smotritsky, N.A.Titov, V.A.Vesna - Phys.Lett. 107B, 272 (1981) Gbservation of Parity Violating Effects in the Polarized Thermal Neutron Total and Radiative Capture C r o s s S e c t i o n s o f ~ T S n a n d ~agLa E.G.Kopanets, A.S.Kachan, L.P.Korda - Izv.Akad.Nauk SSSR, S e r . F i z . 45, 2157 (1981) Study of the T-Radiation Angular Distribution f o l l o w i n g t h e 25Mg(p,T)26A1 R e a c t i o n K.Kobayashi, Y.Fujita, N.Yamamuro - J.Nuel.Sci.Technol.(Tokyo) 18~ 823 (1981) N[easurement of Neutron Capture Cross Section of Thorium-232 from 1 keV to 408 keV S.Kossionides, K.-H.Moebius, R.Boettger, P.Egelhof, Z.Moroz, E.Steffens, G.Tungate, W.Dreves, I.Koenig, D.Fick - Fizika(Zagreb) 13, S u p p l . N o . 1 , 9 (1981) Deformation Dependence of the Cross Section of 7Li(pol) Induced Reactions K.Kobayashi, S.Yamamoto, I.Kimura - Ann.Rep.Res.Reactor I n s t . , K y o t o U n i v . 14, 1 (1981) The U-235 Fission Spectrum A v e r a g e d C r o s s S e c t i o n f o r t h e 199Hg(n,n')~9~mHg R e a c t i o n P r o c e s s e d with Covariances between the Data Uncertainties A.J.Kreiner, C.Baktash, G.Garcia Bermudez, M.A.J.Mariscotti - Phys.Rev.Lett. 47, 1709 (1981) Evidence for Predicted Level Crossings in fr(h9/2) x u(i13/2) Bands in very Neutron-Deficient, D o u b l y O d d T1 I s o t o p e s

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81Ma37 81Ma38 81Ma39 81Ms41 81Mc14 81Me15 81Mi16 81Mi17

81Mo25 8 1Mu18 81Na14 81No12 810h08 810h09 810xOl 81Pa22

81Pa25

81Pa26 81Pa27

W.M.Lattimer, K.S.Krane, N.J.Stone, G.Eska - J.Phys.(London) G7, 1713 (1981) Nuclear Orientation o f 191Pt i n Fe J.Lange, K.R.Baker, J.H.Hamilton, A.V.Ramayya, L.Varnell, J.J.Pinajian, V.Maruhn-Rezwani Z . P h y s . A 3 0 3 , 321 (1981) Directional Correlations i n t h e D e c a y o f 1 2 0 0 y 166Ho Y.Le B o r n e c , L . B i m b o t , N.Koori, F.Reide, A.Willis, N.Willis, C.Wilkin Fhys.Rev.Lett. 47, 1870 (1981) Coherent Pion Production near Threshold w i t h a 3He P r o j e c t i l e V.I.Levin, A.B.Malinin, I.N.Tronova - Radiochem.Radioanal.Lett. 49, 111 (1981) Production of Radionuclides by Photonuclear Reactions. I. 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K.Paulsen, D.Rehder - Z.Naturforsch. 37a , 139 (1981) Nuclear Quadrupole Perturbations i n 5IV NMR S p e c t r a o f O x o v a n a d i u m ( + V ) Complexes T.Q.Phan, G.Piller, A.Ruetschi, L.A.Schaller, L.Schellenberg, H.Schneuwly Helv.Phys.Acta 54, 6 4 8 (1981) Magnetische Momente aus Kernubergangen in Muonisehem ~°gBi D.Pocanic, K.Van Bibber, W.A.Seale, J.Dunham, J.L.Thornton, S.S.Hanna Fizika(Zagreb) 13, S u p p l . N o . l , 35 (1981) Intermediate Structure i n t h e 160 + l e o S y s t e m O b s e r v e d v i a t h e a E x i t C h a n n e l A.Rahbar, B.Aas, E.Bleszynski, M.Bleszynski, M.Haji-Saeid, G.J.tgo, F.Irom, G.Pauletta, A.T.M.Wang, J.B.McClelland, J.F.Amann, T.A.Carey, W.D.Cornelius, M.Barlett, G.W.Hoffmann, C . G l a s h a u s s e r , S . N a n d a , M . M . G a z z a l y - P h y s . R e v . L e t t . 47, 1811 (1981) First Measurement of the Spin Rotation Parameter Q f o r p - 4°Ca E l a s t i c S c a t t e r i n g a t 500 MeV J.Ramm-Arnet, V.Meyer - Helv.Phys.Acta 54, 326 (1981) Elastische Streuung yon Protonen a n e4Zn P.Riehs, R.Prasad, G.Eder, H.Jasicek, H.H.Muller, W.Reiehart, S.Steiner - Helv.Phys.Acta 54, 317

(1981) 81Ri13

81Ro12

8IRo13

81Ro15

81Rull 81Ru12

81Ru13

81Sa34 81Sa35 81Sa39

81Sa42 81Sc21 81Se15 81Se16 8iSh22 81Sh23 81Sh26 81Si15 81Si16 81Si17

Measurement and Analysis of Prompt Fission Neutrons o f ZSZCf(sf) D.Rizzo, E.Bozek, B . D e l a u n a y , J.Delaunay, A.D'Onofrio, H.Dumont, M.G.Saint Laurent, F.Terrasi Fizika(Zagreb) 13, S u p p l . N o . 1 , 53 (1981) Excitation Functions of the Neutron Transfer a n d I n e l a s t i c S c a t t e r i n g f o r 13C o n 4STi ( 2 5 - 6 0 MeV lab) R.G.H.Robertson, P.Dyer, R.A.Warner, R.C.Melin, T.J.Bowles, A.B.McDonald, G.C.Ball, W.G.Davies, E.D.Earle - Phys.Rev.Lett. 47, 1867 (1981) Observation of t h e C a p t u r e R e a c t i o n 2H(a,v)SLi a n d Its Role i n P r o d u c t i o n o f SLi i n t h e Big B a n g R . R o y , F . S e i l e r , H . E . C o n z e t t , F . N . R a d - P h y s . R e v . C24, 2421 (1981) Cross Section and Vector Analyzing P o w e r iT,1 o f t h e P r o c e s s e s 3 H e ( d ( p o l ) , d ) 3 H e , 3 H e ( d ( p o l ) , p ) 4 H e between 15 a n d 4 9 MeV L.Ph.Roesch, N.Schlumpf, D.Taqqu, V.L.Telegdi, P.Truttmann, A.Zehnder Phys.Lett. 107B, 31 (1981) Measurement of t h e C a p t u r e R a t e s t o t h e E x c i t e d S t a t e s i n 12C(;l-,v)laB* a n d a N o v e l T e c h n i q u e to Deduce the Alignment o f 12B*(1-) H.D.Ruter, E.W.Duczynski, W.Haaks, E.Gerdau - Hyperfine Interactions 11, 37 (1981) T h e 183Re G r o u n d State Dipole Moment and Nuclear Spin-Lattice Relaxation o f Re i n Fe W.Ruekstuhl, B.Aas, W . B e e r , I . B e l t r a m i , K.Bos, P . F . A . G o u d s m i t , H.J.Leisi, G.Strassner, A.Vacchi, R.Weber, J.M.v.d.Velden - Helv.Phys.Acta 54, 6 4 4 (1981) Die H y p e r f e i n a u f s p a l t u n g des ls-Zustandes i n ~ - 7Li a l s T e s t d e r W e c h s e l w i r k u n g Z w i s c h e n M y o n e n und Nukleonen W.Ruckstuhl, B.Aas, I.Beltrami, K.Bongardt, P.F.A.Goudsmit, H.J.Leisi, G.Strassner, A.Vacchi, F.W.N.De B o e r , U . K i e b e l e , R . W e b e r - H e l v . P h y s . A c t a 54, 6 4 4 (1981) Bestimmung des Ladungsradius v o n 12C a u s e i n e r M e s s u n g d e s M y o n i s c h e n ( 2 p - l s ) - R o n t g e n u b e r g a n g s H . S a u v a g e o n - P h y s . R e v . C24, 2667 (1981) Production of 3SAr a n d 39At i n t h e I n t e r a c t i o n o f G ol d a r i d T h o r i u m w i t h 1,2.5,and 24 GeV P r o t o n s H.Sakai, N.Matsuoka, K.Hatanaka, K.Okada, H.Shimizu - P h y s . R e v . C24, 2 7 6 6 (1981) Observation of the Vector and Tensor Analyzing P o w e r s of t h e C o n t i n u u m Spectra Sa J u n , T a n g H o n g q i n g , Z h a n g Y i n g , L i a n g D o n g q i , S h e n W e i q i , W a n g X i a o z h o n g , D o n g M i n l i , Ye Chunying, Gu Y i f a n - C h i n . J . N u c l . P h y s . 3, 302 (1981) Measurement of Scattering C r o s s S e c t i o n s o f 11.6 MeV N e u t r o n s from Carbon J.Sato, T.Hirose - Radiochem.Radioanal.Lett. 46, 145 (1981) Half-Life o f 13SLa W.-D.Schmidt-Ott, R . K a n t u s , E . R u n t e , U . J . S c h r e w e , R . M i c h a e l s e n - P h y s . R e v . C24, 2 6 9 5 (1981) A t o m i c M a s s e s o f 14aDy a n d 14aTb ( T l / a = 2.2 r a i n ) W.Semmler, P.Raghavan, M . S e n b a , R . S . R a g h a v a n - Z . P h y s . B45, 29 (1981) Temperature Dependence of the Quadrupole Interaction o f 69Ge(T1) a n d 113Sn(Sn) K . S e i d e l , A . M e i s t e r , D . P a b s t , L . B . P i k e l n e r , W . P i l z - Y a d . F i z . 34, 1173 (1981) Resonance Interaction of Neutrons with a Molecular Gas and with Crystals S.Shirato - Nucl.lnstrum.Methods 190, 29 (1981) 0 ° Cross Section for the t2C(d,n9)taN Reaction Produced by Means of Beam Stopping D . L . S h p a k , G . G . K o r o l e v - Y a d . F i z . 33, 860 (1981); S o v . J . N u c l . P h y s . 33, 4 4 9 (1981) Angular Anisotropy of Fragments in the Near-Threshold F i s s i o n o f 236U a n d 23SU b y N e u t r o n s F.Shahin - Indian J - P h y s . 55A , 4 3 4 (1981) Methods of Extracting the Coherence Energy from Fluctuating Excitation Function A.Simonits, L . M o e n s , F.De C o r t e , A.De W i s p e l a e r e , J . H o s t e - J . R a d i o a n a l . C h e m . 67, 61 (1981) Absolute Intensity o f t h e 140.5 k e V G a m m a - R a y o f 9SMo H . R . S i d d i q u e , S . J . H a l l - I n d i a n J . P h y s . 55A, 365 (1981) Differential Cross Sections of Neutron Scattering from 2Ssi a n d 32S S.P.Simakov, G°N.Lovchikova, O.A.Salnikov, A.M.Trufanov, G.V.Kotelnikova, N.N.Shchadin A t . E n e r g . 51, 2 4 4 (1981); S o y . A t . E n e r g y 51, 655 (1981) CJ:oss S e c t i o n s o f F a s t - N e u t r o n Elastic and Inelastic Scattering on Indium Isotopes

I61

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81sjo3

81Sk04 81SI03

81Sr02 81S125

81St28 81St29 81Sul0

81Su12

81Sz06

81Sz07

81Ta22 81Ta23

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81Ta26 81Ta27 81Te02

81To15

81To18

81Tr08

81Tr09

81TrlO

81Un02

J . J . S i m p s o n - P h y s . R e v . D23, 649 (1981) Measurement of the fl-Energy S pe c trum o f 3H t o D e t e r m i n e t h e A n t i n e u t r i n o Mass T.P.Sjoreen, P.H.Pile, R.D.Bent, M.C.Green, J.J.Kehayias, R.E.Pollock, F.Soga, M.C.Tsangarides, J . G . W i l l s - P h y s . R e v . C24, 2569 (1981) Positive Pion Production b y 149 - 166 MeV P r o t o n s o n 160 a n d 28Si E . A . S k a k u n , V.G.Baty, Y u . N . R a k i v n e n k o - I z v . A k a d . N a u k SSSR, S e r . F i z . 45, 2170 (1981) T h e 89Y(p,n)SOm,aZr i n t h e P r o t o n E n e r g y R a n g e o f 5 - 9 MeV R.J.Slobodrian, C . R i o u x , R.Roy, H . E . C o n z e t t , P . v o n R o s s e n , F . H i n t e r b e r g e r - Phys.Rev.Lett. 47, 1803 (1981) Evidence of Time-Symmetry Violation in the Interaction of N u c l e a r P a r t i c l e s C . V . S r i n i v a s a Rao, N . L a k s h m a n a Das, B . V . T h i r u m a l a Rao, J . R a m a Rao - P h y s . S c r . 24, 935 (1981) Activation Cross-Sections f o r 14.2 MeV N e u t r o n s o n M o l y b d e n u m H.Steuer, W.Eyrich, A.Hofmann, H.Ortner, U.Scheib, R.Stamminger, D.Steuer, H.Rebel P h y s . R e v . L e t t . 47, 1702 (1981) Neutron Decay of the Giant Qua drupole R e s o n a n c e R e g i o n i n 2°sPb M . P . S t o j a n o v i c , J . S i m i c , S . K o i c k i - F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 2 , 43 (1981) Investigation o f i77LLI 150.392 k e V I s o m e r i c S t a t e F e e d i n g G . M . S t u k o v - A t . E n e r g . 51, 61 (1981); S o y . A t . E n e r g y 51, 483 (1981) Determination of Some Neutron Activation Parameters o f 115In Su Zongdi, Ma Z h o n g y u , Z h o u C h u n m e i , Ding X u n l i a n g , Lu Z h o n g d a o , Ding D a z h a o - C h i n . J . N u c l . P h y s . 3, 97 (1981) The Measurements,Evaluations and t h e T h e o r e t i c a l A n a l y s e s of t h e Cross Sections f o r the N e u t r o n Radiative Capture Reactions P.A.Sushkov, I.A.Kondurov, M.Bogdanovie, T.Mitsunari, T.D.Mac M a h o n , H . A . B a a d e r , D . B r e i t i n g , R.Koch, H.Seyfarth, O.W.B.Schult, H.Borner, R.Brissot, G.Barreau, H.Faust, K.Schreekenbaeh F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 2 , 39 (1981) The Level Scheme of n°Ag f rom the (n,7) Re a c tion A.Szanto de T o l e d o , T . M . C o r m i e r , M.Herman, B.Lin, P.M.Stwertka, M.M.Coimbra, N.C.Filho P h y s . R e v . L e t t . 47, 1881 (1981) Limiting Angular Momenta for Light Heavy-lon F us ion at High E ne rgy A.Szanto de T o l e d o , M . M . C o i m b r a , N . C . F i l h o , T . M . C o r m i e r , P.M.Stwertka - Fizika(Zagreb) 13, S u p p l . N o . l , 29 (1981) An Interpretation of Gross S truc ture s i n t h e E n e r g y S p e c t r a o f t h e lUC(160,a)24Mg R e a c t i o n s S . L . T a b o r , L . C . D e n n i s , K . A b d o - P h y s . R e v . C24, 2552 (1981) A b s o r p t i v e B r e a k u p o f 14N P r o j e c t i l e s T.Tanabe, M.Yasue, K.Sato, K.Ogino, Y.Kadota, Y.Taniguchi, K.Obori, K.Makino, M.Tochi P h y s . R e v . C24, 2556 (1981) (6Li,d) R e a c t i o n o n 160 a n d 28Si a t 75 MeV P . T a r a s , G.C.Ball, W.G.Davies, H . R . A n d r e w s , B.Haas - P h y s . L e t t . 107B, 35 (1981) Evidence for Alpha-Cluster Structure a t 12.9 MeV CM i n t h e 12C + 160 S y s t e m M.Tanaka, K.Iwamoto, T.Yamagata, S.Kishimoto, B.Saeki, K.Yuasa, T . F u k u d a , K.Okada, I.Miura, M . I n o u e , H.Ogata - N u c l . P h y s . A372, 173 (1981) T h e 12C(3He,a)llC R e a c t i o n a t 1 0 0 - 1 4 0 MeV Tao Z h e n l a n , Z h u F u y i n g , Qiu H u i y u a n , W a n g G o n g q i n g - C h i n . J . N u c l . P h y s . 3, 242 (1981) T h e E x c i t a t i o n F u n c t i o n s f o r t h e R e a c t i o n lsz-lsSW(d,2n)lSz-186Re a n d ls6W(d,p)laTW R.B.Taylor, P.Teansomprasong, I.B.Whittingham - A u s t . J . P h y s . 34, 125 (1981) E l a s t i c S c a t t e r i n g o f 152Eu 7 R a y s b y T u n g s t e n G.M.Ter-Akopian, A.G.Popeko, E.A.Soko], L.P.Chelnokov, V.I.Smirnov, V.A.Gorshkov Nucl.Instrum.Methods 190, 119 (1981) A Neutron Multiplicity Detector for Rare Spontaneous Fission Events W . T o r n o w , E.Woye, G.Mack, R . L . W a l t e r , C.E.Floyd, P . P . G u s s , R . C . B y r d - N u c l . I n s t r u m . M e t h o d s 190, 523 (1981) Small-Angle Neutron Polarization f o r t h e Z H ( d ( p o l ) , n ( p o l ) ) 3 H e R e a c t i o n n e a r E(d) = 8 MeV E.Tomasi, D.Ardouin, J.Barreto, V.Bernard, H . D o u b r e , C.Ngo, C . M a z u r , E . P i a s e c k i , M.Ribrag F i z i k a ( Z a g r e b ) 13, S u p p l . N o . 1 , 6 (1981) F u s i o n E x c i t a t i o n F u n c t i o n o f t h e 46Ca + 4°Ca S y s t e m n e a r T h r e s h o l d P.Trocellier, Ch.Engelmann - J . R a d i o a n a l . C h e m . 67, 135 (1981) Fonctions D'Excitation des Reactions N u c i e a r i e s : 23Na(p,p'7)23Na,23Na(p,(xT)26Ne et 23Na(P,~6)eONe e n t r e 500 et 1700 k e V W.Trombik, W.Trautmann, W.Dunnweber, K.A.Eberhard, W.Hering, D.Konnerth, R.Singh F i z i k a ( Z a g r e b ) 13, S u p p i . N o . 1 , 25 (1981) T h e Role of t h e I n e l a s t i c C h a n n e l s f o r t h e O c c u r r e n c e of I n t e r m e d i a t e R e s o n a n c e s i n *ZC + 12C a n d 14C + 14C W . T r a u t m a n n , W . D u n n w e b e r , W.Hering, C . L a u t e r b a e h , H.Puchta, R.Ritzka, W . T r o m b i k 13, S u p p l . N o . 1 , 80 (1981) Constrained P h a s e S p a c e A p p r o a c h to t h e 160 + 48Ti R e a c t i o n I . J . U n u s , P . A . I n d i r a , P . V e n u g o p a l a Rao - J . P h y s . ( L o n d o n ) G7, 1683 (1981) Internal Ionisation Probability i n t h e Beta D e c a y of 151Sm

-

Fizika(Zagreb)

REFERENCES

81Va24

81Va26

81Va27

81Va28

81Va29

P..Van C a m p , R . V a n d e V y v e r , E . K e r k h o v e , D . R y c k b o s c h , H . F e r d i n a n d e , P.Van 0tten, P.Berkvens P h y s . R e v . C24, 2 4 9 9 (1981) Experimental Determination of the Proton Escape Width in the Giant Dipole Resonance of 89y V.M.Vakhtel, T s . V y l o v , N.A.Golovkov, B.S.Dzhelepov, A . K a r a k h o d z h a e v , V . V . K u z n e t s o v , M.Ya.Kuznetsova, M.Milanov, Yu.V,Norseev, T.l.Popova, V . P . P r i k h o d t s e v a , V . G . C h u m i n , Yu.V.Yushkevich - Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1841 (1981) "y-Spectra and I n t e r n a l Conversion Electrons of Z°eAt. Transition Multipolarities in 2°SPo V.M.Vakhtel, N.A.Golokov, R.B.Ivanov, M.A.Mikhailova, A.F.Novogorodov, Yu.V.Norseev, V.G.Chumin, Yu.V.Yushkevieh - Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1861 (1981) (x-Spectra of 21°,a°s,a°e,2°4At and 212Fr S.K.Vasilev, B.S.Dzhelepov, R.B.Ivanov, M.A.Mikhailova, A.V.Mozzhykhin, B.I.Shestakov Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1895 (1981) "y-Radiation Accompanying aZTAc a-Decay V.M.Vakhte], N.A.Golovkov, R.B.Ivanov, M.A.Mikhailova, V.G.Chumin - Izv.Akad.Nauk SSSR, Ser.Fiz.

45, 1966 (1981) 81Vel6 81Vel7 81Vo09 81Vo10 81Vo12

8 1Wa3 1 81We15 81Wel7 81Wil5

81~u03

81Xe01

81YalO

81Ye02 81Y008 81YuOl 8IYu02

81YuO3 81Zd01 81Zh04

81Zh05 81ZhO6

{x-Decay Schemes for zlo ~0s,20e,204At and ai2Fr II.C.Verma, J.Chappert, G.N.Rao - Hyperfine Interactions Ii, 45 (1981) Quadrupo]e I n t e r a c t i o n at 57Fe in Zirconium Metal B.Vekic, L.Horvath, V.Horvat, M.Vlatkovic - Radiochem.Radioanal.Lett. 47, 35 (1981) Production of 1-123 by A l p h a - B o m b a r d m e n t of Natural A n t i m o n y Von G.Otto, E.Zschau, A.AI-Khafaji - Ann.Phys.(Leipzig) 38 298 (1981) Lebensdauermessungen an Resonanzzustanden im aeSi-Compoundkern m i t t e l s S c h a t t e n - E f f e k t V.V.Volkov - Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1810 (1981) Formation of Light Charged Particles in Heavy Ion Reactions A.S.Voronin, S.M.Solovyev, I.S.Koretskaya, V.L.Kuznetsov, V.G.Nedorezov, N.V.Nikitina, V.l.Noga, S.A.Pashchuk, Yu.N.Ranyuk - Yad.Fiz. 34, 1439 (1981) Fission of Nuclei aSaTh,asaU,asSu,2aSU,aaSU,237Np and 239pu Induced by Electrons with Energies f r o m 1OO up to 275 MeV C.Wagemans, E.Allaert, G.Barreau, A.Emsallem, P.D'Hondt - Nucl.lnstrum.Methods 190, 167 (1981) Determination of Atomic Masses via (n(th),p) and (n(th),a) Reactions R.Wenz, A.Timmermann, E . M a t t h i a s - Z . P h y s . A 303, 87 (1981) Subshell Effect in Mean Square Charge Radii of Stable Even Cadmium Isotopes &Weber - Helv.Phys.Acta 54, 5 4 7 (1981) The (n,d) Differential E l a s t i c C r o s s S e c t i o n a t 2 MeV K . W i s s h a k , F . K a p p e l e r - N u c l . S c i . E n g . 77, 58 (1981) Determination of the Capture W i d t h o f t h e 27.7 k e V s - W a v e N e u t r o n Resonance in Iron-56 E.C.Wu, K . D . H i l d e n b r a n d , H.Freiesleben, A.Gobbi, A.Olmi, H.Sann, U.Lynen - Phys.Rev.Lett. 47, 1874 (1981) I n f l u e n c e of S h e l l S t r u c t u r e o n N e u t r o n a n d P r o t o n E x c h a n g e i n t h e R e a c t i o n s of 144Sm o n 1 4 4 8 m a n d 154Sm on 154Sm A.C.Xenoulis, A.E.Aravantinos, C.J.Lister, J.W.Olness, R.L.Kozub - Phys.Lett. I06B, 461 (1981) Systematics of the Competition between pn and d Emission in Heavy-Ion Induced Nuclear Reactions H.Yamada, C.F.Maguire, J.H.Hamilton, A.V,Ramayya, D.C.Henslcy, M.L.Halbert, R.L.Robinson, F.E.Bertrand, R . W o o d w a r d - P h y s . R e v . C34, 3 5 6 5 (1981) Localized 1 Window from Partial Fusion Reactions Accompanied by Proton,Deuteron,and Triton Emission Ye Z h o n g y u a n , Li J i n g w e n , Z h o u S h u h u a , Hao X i u h o n g - C h i n . J . N u c l . P h y s . 3, 47 (1981) The Measurement of Fragment Angular Distributions f o r a38U(n,F) n e a r T h r e s h o l d Fission Reaction K.Yoshihara, A.Hibino, I.Yamoto, H.Kaji - Radiochem.Radioanal.Lett. 48, 303 (1981) Chemical E f f e c t of Tc K(fl) X - R a y I n t e n s i t y i n t h e D e c a y 9°Mo -* s9mTc ~ 99Tc Y u a n R o n g f a n g , W a n g Z h i f u , Ye B i n q i , S u n Z u x u n , Y u a n J i a n - C h i n . J . N u c l . P h y s . 3, 155 (1981) The Reactions Induced by Deuteron Bombardment o n SLi a t E n e r g y 9.05 MeV Yu Banshui, Liu Fengying, L u X i a n e , Li S h e n g g a n g , Y a n g C h u n x i a n g - Chin.J.Nucl.Phys. 3, 312 (1981) T h e D e c a y o f t44Ce Yung Guanjun, Cheng Shiping, Nan Behua, Zhou Ling, Weng Peikun - Chin.J.Nucl.Phys. 3, 316 (198t) The Decay of 44Sc and 44mSc Yu.G.Zdesenko, V.N.Kuts, I.A.Mytsyk, A.S.Nikolaiko - Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1856 (1981) Search for Neutrinoless Double fl-Decay of 9SZr Zhao Kui, Cheng Yehao, Zhu Guanghua, Lu Xiuqin, Yang Zhuqing, Jiang Chenglie - Chin.J.NucI.Phys. 3, 32 (1981) S t u d i e s o f ( ~ , p ) R e a c t i o n s I n d u c e d b y 18 MeV <~ Zhou Shuhua, G u o S h i l u n , M e n g Wu, S u n S h e n g f e n , Hao X i u h o n g - C h i n . J . N u c l , P h y s . 3, 39 (1981) Angular Distributions of Fission Fragments at the aSSU(n,2n'f) Threshold Zhang Huanqiao, Liu Zuhua, Ding Shengyue, Liu Shaoming - Chin.J.NucI.Phys. 3, 149 (1981) T h e A v e r a g e N u m b e r of P r o m p t N e u t r o n s a n d t h e D i s t r i b u t i o n of P r o m p t N e u t r o n E m i s s i o n N u m b e r s for Spontanous Fission of e4°Pu,a*2Cm,e44Cm

163

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81Zi01

81Zi02 82Aa04

82Ab02 82Ab03 82Ad02

82Ah01 8RAh04 82Ah05 82Ak03

82A101 82A103

82AI05

8~A107

82A108

82A109

82A110

82Alll 82Al13

U.Yu.Zhovliev, M.F.Kudoyarov, I.Kh.Lemberg, A.A.Pasternak Izv.Akad.Nauk SSSR, S e r . F i z . 45, 1879 (1981) L i f e T i m e s o f S t a t e s i n 66Zn b y D o p p l e r S h i f t A t t e n u a t i o n and pT-coincidence Measurements H.J.Ziock, R.J.Ellis, K.O.H.Ziock, J.Bolger, E.Boschitz, J.Arvieux, R.Corfu, J.Piffaretti P h y s . R e v . C24, 2 6 7 4 (1981) Quasifree Scattering of Positive Pions on Carbon K.Zitter, J.Schmand, R.Sehollhorn - P h y s . L e t t . 87A, 130 (1981) I s o m e r S h i f t o f t h e 6.2 k e V N u c l e a r T r a n s i t i o n o f lSlTa i n C u 3 T a S 4 B.Aas, E . B l e s z y n s k i , M.Bleszynski, M.Haji-Saeid, G.Igo, F . I r o m , G . P a u l e t t a , A.Rahbar, A.T.M.Wang, J.F.Amann, T.A.Carey, W.D.Cornelius, J.B.McClelland, C.Glashausser, S.Nanda, M.Barlett, G.W.Hoffmann, M . G a z z a l y - P h y s . R e v . C26, 1770 (1982) Observed Relations between Proton Spin Observables in Natural Parity Transitions i n 4°Ca(p, p')4OCa a n d 2 ° s P b ( p , p ' ) 2 ° s p b R e a c t i o n s a t 500 MeV K . M . A b d o , L . C . D e n n i s , A . D . F r a w l e y , K . W . K e m p e r - N u c l . P h y s . A377, 281 (1982) Direct and Compound Nuclear Contributions t o t h e l a c ( s L i , t ) R e a c t i o n a t E = 25 MeV O.A.Abou-zeid, W.R.Falk, S.K.Datta, S.P.Kwan, J.Campbell - N u c l . P h y s . A 3 8 2 , 185 (1982 ) T h e 46,4a,SOTi(p,c~)4a,45,47Sc R e a c t i o n s a t 4 0 . 3 5 MeV I.Adam, N.M.Antoneva, V.B.Brudanin, M.Budzynski, Ts.Vylov, V.A.Dzhashi, A.Zhumamuratov, A.I.Ivanov, V.G.Kalinnikov, A.Kugler, V.V.Kuznetsov, Li Z o n S i k , T . M . M u m i n o v , A.F.Novgorodov, Yu.N.Podkopaev, Z.D.Shavgulidze, V.L.Chikhladze - Izv.Akad.Nauk SSSR, S e r . F i z . 46, 2 ( 1 9 8 2 ) Study of the Radioactive D e c a y o f I s o b a r s w i t h M a s s A = 140 I . A h m a d , E . P . H o r w i t z - N u e l . P h y s . A 373, 4 3 4 (1982) A l p h a D e c a y o f z57100Fm I.Ahmad - Nucl.Instrum.Methods 193, 9 ( 1 9 8 2 ) Alpha-Emitting Nuclides as Absolute Efficiency Calibration Sources for Germanium Detectors S . P . A h l e n , P . B . P r i c e , M . T i n c k n e l l - P h y s . R e v . C25, 1996 (1982) Heavy Fragment Production through Electropion Excitation of 56Fe H.Akcay, G.Mouze, D.Maillard, Ch.Ythier - Radioehem.Radioanal.Lett. 51, 1 (1982) Analyse du Rayonnement G a m m a d ' u n e S o u r c e de R a d i u m 226 e n E q u i l i b r e a v e c s e s D e r i v e s e n t r e 150 e t 100O k e V K.Aleklett, G.Rudstam - N u c l . S c i . E n g . 80, 74 (1982) Average Beta-Ray Energies of Short-lived Fission Products V.P.Alfimenkov, S.B.Borzakov, J.Wierzbicki, A.I.Ivanenko, Yu.D.Mareev, O.N.Ovchinnikov, L . B . P i k e l n e r , E . I . S h a r a p o v - N u e l . P h y s . A 376, 229 (1982) Investigation of Spin Dependence of Neutron Cross Sections and of Strength Functions for Rare Earth Nuclei in Experiments with Polarized Neutrons and Nuclei A.Alzner, E.Bodenstedt, C.Herrmann, P.Herzog, H.Munning, H.Reif, R.Vianden, U.Wrede - Z.Phys. A305, 157 (1982) Gyromagnetic Ratios of the 4 + and 0 + Rotational S t a t e s o f lS4w G.D.Alkhazov, K.A.MezJlev, Yu.N.Novikov, V.N.Panteleyev, A.G.Polyakov, V.P.Afanasyev, N.Ganbaatar, K.Ya.Gromov, V.G.Kalinnikov, J.Kormicki, A.Latuszynski, A.Potempa, J.Sieniawski, F.Tarkanyi, Yu.V.Yushkevich - Z . P h y s . A 305, 185 (1982) New N e u t r o n D e f i c i e n t I s o t o p e s w i t h Mass N u m b e r s A = 138 a n d 145 D.V.Aleksandrov, Yu.A.Glukhov, A.S.Demyanova, V.I.Dukhanov, l.B.Mazurov, B.G.Novatsky, A . A . O g l o b l i n , S . B . S a k u t a , D . N . S t e p a n o v - Y a d . F i z . 35, 277 ( 1 9 0 2 ) S t u d y o f (6Li,SB) a n d (TLi,eB) R e a c t i o n s o n L i g h t N u c l e i A.S.Aleksanyan, T.L.Asatiani, N.V.Vladimirsky, A.O.Gasparyan, M.I.Dayon, V.A.lvanov, S.P.Karavaev, S.N.Karapetyan, F.F.Kayumov, G.K.Megrabyan, N.A.Nalbandyan, E.M.Oganesyan, R.N.Pikhtelev, V . M . R a p p o p o r t - Y a d . F i z . 35, 360 (1982) Measurement of 7 r ° - M e s o n P h o t o p r o d u c t i o n C r o s s S e c t i o n o n 4He a t t h e E n e r g i e s E7 = 1 . 5 - 4 . 5 GeV i n the Region of Small Momentum Transfers V.L.Alekseev, A.I.Egorov, L.P.Kabina, I.A.Kondurov, E.K.Leushkin, Yu.E.Loginov, V.V.Martynov, S.L.Sakharov, V.L.Rumyantsev, Yu.L.Khazov - Izv.Akad.Nauk SSSR, S e r . F i z . 46, 52 (1982) L e v e l s o f '2sI A.L.Allsop, S.Hornung, K.S.Krane, N.J.Stone - J.Phys.(London) 0 8 , 857 (1982) The Nuclear Magnetic Moment of '86It E.Allaert, C.Wagemans, G.Wegener-Penning, A.J.Deruytter, R.Barthelemy Nucl.Phys. A380, 61

(1902) 82AI14 82AI15

E n e r g y a n d Mass D i s t r i b u t i o n s for 241Pu(n(th),f),24epu(s.f.) and e44pu(s.f) Fragments L.Alvarez, G.Palla - J.Phys.(London) G8, 987 (1982) Elastic Scattering o f 3He b y 12C a n d lSo a t a n E n e r g y o f 4 0 . 9 MeV T.K.Alexander, G.C.Ball, W.G.Davies, J.S.Forster, I.V.Mitchell, H.-B.Mak Phys.Lett.

l13B,

132

(1982) 82Al16

Lifetime Measurements of L e v e l s i n 2SSi a n d t h e R a t i o of N e u t r o n t o P r o t o n for Mirror Nuclei V.P.Alfimenkov, S . B . B o r z a k o v , Vo V a n T k h u a n , Yu.D.Mareev, L.B.Pikelner, E . I . S h a r a p o v - Y a d . F i z . 35, 5 4 2 (1982) Spin Dependence of s-Wave Neutron Scattering C r o s s S e c t i o n o f 7Li

164

Transition D.Rubin,

Amplitudes A.S.Khrykin,

REFERENCES

82Al17 82Al18

82Al19 82A120

82A121

82A122

82A123 82A124

82A127 82A128 82A129 82Am02 82An01 82An02 82An06

82An07 82An08

82An09

82An10

82Anll 82Ao01

82Ao02

82Ao04 82Ao05

82Ap01

82Ar04

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82Ba49

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82Be19

82Be20

H.W.Baer, R . B o l t o n , J.D.Bowman, M.D.Cooper, F.Cverna, N.S.P.King, M.Leitch, H.S.Matis, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blaekmore, E . R . S i c i l i a n o - P h y s . R e v . L e t t . 49, 1376 ( 1 9 8 2 ) Observation of Analogs of the Giant-Dipole R e s o n a n c e i n P i o n S i n g l e C h a r g e E x c h a n g e o n 4°Ca N . B . B a d a l o v , A . B u d z y a k , T s . V y l o v , K i m Zai Te, V . V . K u z n e t s o v , Li S u C he rt , A . A . M a r c h u k , S h . O m a n o v - A c t a P h y s . P o l . B13, 89 (1 982) E x c i t e d S t a t e s o f 151Gd f r o m t h e D e c a y o f ~51Tb (T1/z = 16.4 h ) M.Behar, A.Ferrero, A.Filevich, G.Garcia Bermudez, M . A . J . M a r i s c o t t i - N u c l . P h y s . A 373 , 4 8 3 ( 1 9 8 2 ) High-Spin S t a t e s i n 94Tc M.Bernheim, A.Bussiere, J.Mougey, D.Royer, D.Tarnowski, S.Turck-Chieze, S.Frullani, S.Boffi, C . G i u s t i , F . D . P a c a t i , G . P . C a p i t a n i , E.De S a n c t i s , G . J . W a g n e r - N u c l . P h y s . A 375, 381 (19 8 2 ) T h e I n f l u e n c e of B o u n d S t a t e s a n d O p t i c a l P o t e n t i a l s o n l p M o m e n t u m Distributions Obtained from 12C a n d 1 6 0 ( e , e ' p ) R e a c t i o n s M.Behar, D.Abriola, A.Filevich, G.Garcia Bermudez, A.J.Kreiner, M.A.J.Mariscotti J.A.Pinston, D.Barneoud - N u c l . P h y s . A3 76, 131 (1982) In-Beam S t u d y o f 78Br Z.W.Bell, L . S . C a r d m a n , P . A x e l - P h y s . R e v . C25, 791 (1982) Fine Structure i n t h e Z°sPb P h o t o n e u t r o n C r o s s S e c t i o n b e t w e e n 9.9 a n d 11.2 MeV M.Beckerman, M . S a l o m a a , A . S p e r d u t o , J . D . M o l i t o r i s , A . D i R i e n z o - P h y s . R e v . C25, 837 ( 1 9 8 2 ) Sub-Barrier F u s i o n o f 58,64Ni w i t h 64Ni a n d 74Ge G . B e n e d e t t i , A . C e s a n a , V . S a n g i u s t , M . T e r r a n i , G . S a n d r e l l i - N u c l . S c i . E n g . 80, 379 (1982 ) Delayed Neutron Yields from Fission of Uranium-233,Neptunium~237,Plutonium-238,-240,-241,and Americium-241 J . W . B e h r e n s , J . C . B r o w n e , J . C . W a l d e n - N u c l . S c i . E n g . 80, 393 (1982) Measurement of the Neutron-lnduced Fission Cross Section of Neptunium-237 Relative to Uranium-235 f r o m 20 k e V t o 30 MeV B . B e n g t s o n , H . L . N i e l s e n , N . R u d , K . W i l s k y - N u c l . P h y s . A 378, 1 (1982) Half-Life of the a-Emitting E x c i t e d 0 + S t a t e i n 21ZPo D . H . B e c k , J . A s a i , D . M . S k o p i k - P h y s . R e v . C25, 1152 (1982) T r i t o n F o r m F a c t o r f r o m 0.29 t o 1.O0 f m -z J.C.Bergstrom, S.B.Kowalski, R.Neuhausen - P h y s . R e v . C25, 1156 (1982) E l a s t i c M a g n e t i c F o r m F a c t o r o f 6Li C.E.Bemis,Jr., F.K.McGowan, J.L.C.Ford,Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Phys.Rev. C25, 1637 (1982) Coulomb Excitation of Ground Band Rotational S t a t e s i n Z49Bk A.Becker, E.A.Bakkum, R.Kamermans - P h y s . L e t t . IlOB, 199 (1982) A Microscopic Description of the (p,t) Reaction to Low-Lying 0 + S t a t e s i n t h e E v e n Ge I s o t o p e s G.P.A.Berg, W.Hurlimann, I.Katayama, S.A.Martin, J.Meissburger, J.Romer, B.Styczen, F.Osterfeld, G.Gaul, R.Santo, G.Sondermann - P h y s . R e v . C25, 2100 (1982) Excitation o f t h e 10.212 MeV 1 + S t a t e i n 4 8 C a ( p , p ' ) a t E(p) = 4 4 . 4 MeV G . P . A . B e r g , B . B e r t h i e r - Z . P h y s . A 305, 235 (1982) Exact Finite-Range DWBA D e s c r i p t i o n o f t h e 6°Ni(160,12C)64Zn R e a c t i o n a t 60 MeV I n c i d e n t Energy R.B.Begzhanov, S.M.Akhrarov, O.Sh.Kobilov, G.A.Kulabdullaev - Izv.Akad.Nauk SSSR, S e r . F i z . 46, 57 ( 1 9 8 2 ) Investigation of Highly Excited States of 9°Zr,llSSn using Resonance Scattering of 7-Radiation G.P.A.Berg, M.DeMarteau, A.Hardt, W.Hurlimann, S.A.Martin, J.Meissburger, W.Oelert, H.Seyfarth, B.Styczen, M.Kohler, I.Oelrieh, J.Scheerer - N u c l . P h y s . A 379, 93 (1982) High Resolution Spectroscopy of l°2Ru(d,p)l°ZRu and l°4Ru(p,d)l°3Ru Reactions E.Bellotti, E.Fiorini, C.Liguori, A.Pullia, A.Sarraeino, L.Zanotti Lett.Nuovo Cim. 33, 2 7 3

(198Z) 82Be21

82Be22

82Be24

82Be27 82Be29 82Be30

An Experimental Investigation on Lepton Number Conservation in Double-Beta Processes. G.Berrier-Ronsin, M.Vergnes, G.Rotbard, J.Vernotte, S.Fortier, J.M.Maison, R.Tamisier P h y s . R e v . C25, 2 8 4 8 ( 1 9 8 2 ) M a s s o f 197Hg U.Bechstedt, H.Machner, A.Budzanowski, P.Jahn, C.Mayer-Boricke - P h y s . R e v . C25, 3221 ( 1 9 8 2 ) Evidence for Local Excitations of the Nucleus from 58Ni(a,a'p) Coincidence Measurements at E a ( l a b ) = 140 MeV A.A.Belyaev, V.A.Getman, V.G.Gorbenko, V.A.Gushchin, A.Ya. Derkaeh, Yu.V.Zhebrovsky, I.M.Karnaukhov, L.Ya.Kolesnikov, A.A.Lukhanin, A.L.Rubashkin, P.V.Sorokin, E.A.Sporov, Y u . N . T e l e g i n - Y a d . F i z . 35, 693 (1982) Polarization Parameters E,T,R f o r t h e R e a c t i o n "TP -* P 7r° n e a r t h e F i r s t R e s o n a n c e M . B e r n a s , P h . D e s s a g n e , M . L a n g e v i n , J . P a y e t , F . P o u g h e o n , P . R o u s s e l - P h y s . L e t t . l 13B , 2 7 9 ( 1 9 8 2 ) Magic Features o f 6eNi H.W.Becker, W.E.Kieser, C.Rolfs, H.P.Trautvetter, M . W i e s c h e r - Z . P h y s . A 305, 319 ( 1 9 8 2 ) Resonances Strengths of Some Light Nuclei P.Berthet, R.Frascaria, M.P.Combes, Ch.F.Perdrisat, B.Tatischeff, J.Banaigs, J.Berger, A.Codino, J.Duflo, L.Goldzahl, F.Plouin, F.Fabbri, G.Picozza, L.Satta, M.Boivin - J.Phys.(London) G8, L i l t (1982) Elastic Proton-Deuteron Backward Scattering a t E n e r g i e s f r o m 0.6 t o 2.7 GeV

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82Bh03

82Bi03

82Bi04 82Bi06

82BjOl

82Bj02

82B101

82B102

J . W . B e h r e n s , J . C . B r o w n e , E . A b l e s - N u c l . S c i . E n g . 81, 512 (1982) Mesurement of t h e N e u t r o n - I n d u c e d F i s s i o n C r o s s S e c t i o n o f 232Th R e l a t i v e t o 235U f r o m 0.7 t o 30 MeV A.M.Bernstein, R.A.Miskimen, B . Q u i n n , S.A.Wood, M . V . H y n e s , G . S . B l a n p i e d , B . G . R i t c h i e , V . R . B r o w n - Phys.Rev.Lett. 49, 451 (19 82) Determination of Relative Signs of Neutron and Proton Transition Matrix Elements: Strong cancellation observed f o r t h e 34S(0+ ~ 22 + ) t r a n s i t i o n K.B.Beard, J.Kasagi, E.Kashy, B.H.Wildenthal, D.L.Freisel, H.Nann, R.E.Warner Phys.Rev. C26, 720 ( 1 9 8 2 ) (d,ZHe) R e a c t i o n a t E ( d ) = 99 MeV V.Bernard, C . G r e g o i r e , C . M a z u r , C.Ngo, M . R i b r a g , G . Y . F a n , P . G o n t h i e r , H.Ho, W . K u h n , J . P . W u r m N u c i . P h y s . A 3 8 5 , 319 (1982) Further Experimental S t u d y o f F a s t F i s s i o n w i t h t h e C1 + A u S y s t e m R.B.Begzhanov, S.M.Akhrarov, D . A . G l a d y s h e v , O . S h . K o b i l o v - Y a d . F i z . 35, 1361 (1982) Resonance Scattering of 7 Rays from Neutron Capture in Copper by Tin Nuclei A.Berdoz, B.Favier, F.Foroughi, J.Hoftiezer, G.S.Mutchler, Ch.Weddingen J.Phys.(London) G8, 1363 ( 1 9 8 2 ) The Relative Cross Section for Elastic Proton-Proton Scattering b e t w e e n 500 a n d 600 MeV J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, K.H.Maier, L.Ussery, W.Stoffl, T . N a i l , R . K . S h e l i n e , J . A . C i z e w s k i - P h y s . R e v . C26, 914 (1982) 2 . 1 0 2 - M e V L e v e l i n 2°SHg a n d t h e S p i n G y r o m a g n e t i e Ratio of the 3-s Proton M . B e r n a s , J . C . P e n g , N . S t e i n - P h y s . 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L . M a c k l i n - P h y s . R e v . C26, 1 4 0 4 (1982) ~e,179,1SOHf a n d 1 8 ° T a ( n , T ) C r o s s S e c t i o n s a n d T h e i r C o n t r i b u t i o n to Stellar Nucleosynthesis M.Behar, A.Filevich, A.O.Macchiavelli, L.Szybisz, P.Thieberger - P h y s . R e v . C26, 1417 ( 1 9 8 2 ) High-Spin S t a t e s i n 79Kr P o p u l a t e d by the 7SSe(a,3n) Reaction and Interpreted in Terms of a Quasipar ticle-Plus-Rotor Model T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens, B.E.Bonner, J.E.Simmons, C . L . H o l l a s , C . R . N e w s o m , P . J . R i l e y , R . D . R a n s o m e - P h y s . R e v . 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W i l k i n - P h y s . L e t t . I I 4 B , 311 (1982) Experimental Study of Coherent Pion Production i n 4He(3He,Tr+)TLi a n d a 'Pest o f t h e R e a c t i o n Mechanism C.Bjarle, N.-Y.Herrstrom, R.Kullberg, A.Oskarsson, I.Otterlund - N u c l . P h y s . A381, 5 4 4 ( 1 9 8 2 ) T h e B r e a k u p o f 1So i n t o He: A n e v e n t - b y - e v e n t study of nucleus-nucleus c o l l i s i o n s a t 75,175 a n d 2000 M e V / A T.Bjornstad, J.Blomqvist, G.T.Ewan, B.Jonson, K.Kawade, A.Kerek, S.Mattsson, K.Sistemich Z . P h y s . A 3 0 6 , 95 ( 1 9 8 2 ) E x c i t e d S t a t e s i n t h e D o u b l y C l o s e d S h e l l N u c l e u s 1325oSn82 G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray P h y s . R e v . C25, 4 2 2 ( 1 9 8 2 ) Elastic and Inelastic Scattering o f 0.8 GeV P r o t o n s f r o m 24Mg a n d 26Mg R . C . B l o c k , D . R . 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82B110

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82BI19

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82Bo07 82Bo09

82Bo12 82Bo14

82Bo15

82Bo17

B.Bleaney, J.F.Gregg, M.R.Wells - J.Phys.(London) C15, L 3 4 9 (1982) The Ratio of the Nuclear Electric Quadrupole M o m e n t s o f 5°V a n d 51V i n S m V O 4 Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, D.Ardouin, M.Lattuada P h y s . R e v . C25, 2116 (1982) Investigation of the Nuclear Continuum b y 4°Ca I n e l a s t i c S c a t t e r i n g o n 4°Ca a t 160 MeV G.Blessing, R.Weinreich, S.M.Qaim, G.Stocklin - Int.J.Appl.Radiat.lsotop. 33, 333 (1982) Production o f ~hBr a n d 77Br v i a t h e 75As(3He,3n)75Br a n d 7 5 A s ( a , 2 n ) 7 7 B r R e a c t i o n s u s i n g C u 3 A s - a l l o y as a High-Current Target Material G.S.Blanpied, M.L.Barlett, G.W.Hoffmann, J . A . M c G i l l - P h y s . R e v . C25, 2 5 5 0 ( 1 9 8 2 ) Scattering o f 0.8 GeV P r o t o n s from 14N M.Blecher, K.Gotow, R.Ng, R . L . B u r m a n , R.Carlini, S.Dam, M.V.Hynes, M.JHynes, M.J.Leitch, V.Sandberg, R.Auble, F.E.Bertrand, E.E.Gross, F.E.Obenshain, J.Wu, G.S.Blanpied, B.M.Preedom, B . G . R i t c h i e , W . B e r t o z z i , M . A . K o v a s h , R . P . R e d w i n e - P h y s . R e v . C25, 2 5 5 4 (1982) Pion-Nucleus Inelastic Scattering a t 80 MeV E.Bleszynski, M.Bleszynski, S.Hajisaeid, G.J.Igo, F.Irom, J.B.McClelland, G.Pauletta, A.Rahbar, A.T.Wang, C.A.Whitten,Jr., G.Adams, M.Barlett, G.W.Hoffmann, J.A.McGill, R.Boudrie, G.Kyle P h y s . R e v . C25, 2 5 6 3 ( 1 9 8 2 ) Large Angle Elastic and Inelastic Scattering o f P r o t o n s f r o m 4°Ca a t 800 MeV L.A.Bloomfield, B.Couillaud, Ph.Dabkiewicz, H.Gerhardt, T . W . H a n s c h - P h y s . R e v . A26, 713 (1982) Hyperfine Structure of the 23S-53p Transition i n 3He b y H i g h - R e s o l u t i o n uv-Laser Spectroscopy M.V.Blinov, V.A.Vitenko, V.N.Dushin, V.I.Yurevich - Nucl.lnstrum.Methods 198, 4 5 5 (1982) T h e E f f e c t of S c a t t e r i n g i n F i s s i o n N e u t r o n S p e c t r u m M e a s u r e m e n t s b y t h e T i m e - o f - F l i g h t Technique H.P.Block, J.J.Kraushaar, P.A.Batay-Csorba, F . E . C e c i l - N u c l . P h y s . A 386, 61 (1982) Inelastic Proton Scattering o n 5SNi a t 27 MeV a n d t h e M i c r o s c o p i c M o d e l N.Blasi, R.Bijker, M.N.Harakeh, Y.lwasaki, W.A.Sterrenburg, S.Y.Van Der Werf, M.Vergnes N u c l . P h y s . A388, 77 (1982) S t u d y o f t h e 1 9 3 I r ( a H e , d ) 1 9 4 p t a n d l a a I r ( d , a H e ) ' 9 2 0 s R e a c t i o n s : T e s t of a s u p e r s y m m e t r i c coupling scheme M.Blann, D.Akers, T.A.Komoto, F.S.Dietrich, L.F.Hansen, J.G.Woodworth, W.Scobel, J.Bisplinghoff, B . S i k o r a , F . P l a s i l , R . L . F e r g u s o n - P h y s . R e v . C26, 1471 (1982) Saturation Analysis as a Test of Statistical Fission in Heavy Ion Reactions R.Bonetti, L.Colli Milazzo, M.Melanotte, A.De R o s a , G . I n g l i m a , E.Perillo, M.Sandoli, V.Russo, N.Saunier, F.Shahin - P h y s . R e v . C25, 717 (1982) Fluctuations Due to Statistical Multistep Compound Emission i n t h e 25Mg(3He,p) a n d 25Mg(3He,a) Reactions J . D . B o w m a n , R . E . E p p l e y , E . K . H y d e - P h y s . R e v . C25, 941 (1982) A l p h a S p e c t r o s c o p y of N u c l i d e s P r o d u c e d i n t h e I n t e r a c t i o n of 5 GeV P r o t o n s w i t h H e a v y E l e m e n t Targets V.A.Bondarenko, P.T.Prokofjev - Z . P h y s . A 3 0 4 , 257 (1982) Study of Low-Lying States in 'hlEu via (n,n'T) Reaction T.J.Bowles, R.J.Holt, H.E.Jackson, R.D.McKeown, A.M.Nathan, J.R.Specht - Phys.Rev.Lett. 48, 986 (1982) Isospin Splitting o f t h e G i a n t D i p o l e R e s o n a n c e i n a°Ni U . B o n s e , U . K i s c h k o - Z . P h y s . A 305, 171 (1982) Neutron-lnterferometric Measurement of the Coherent Scattering Length of the Isotopes of Silver W.Bohne, K.D.Buchs, H.Fuchs, K.Grabisch, D.Hilscher, U.Jaknke, H.Kluge, T.G.Masterson, H.Morgenstern - N u c l . P h y s . A 378, 525 (1982) S t u d y o f t h e R e a c t i o n s 24,2aMg(3He,n)2e,28Si a n d 2 a S i ( a H e , n ) 3 ° S A.Bol, P . L e l e u x , P . M a c q - C z e c h . J . P h y s . B32, 319 (1982) A Measurement of t h e N e u t r o n - P r o t o n Differential Cross Section at Extreme Forward and Backward A n g l e s b e t w e e n 4 5 a n d 75 MeV J.Boswell, R.Altemus, R.Minehart, L.Orphanos, H.J.Ziock, E.A.Wadlinger Phys.Rev. C25, 2 5 4 0

(1982) 82Bo18

82Bo19

82Bo21

82Bo25

Differential C r o s s S e c t i o n f o r t h e 7r+d -~ p p R e a c t i o n f r o m 80 t o 417 MeV J.Bolger, E.Boschitz, E.L.Mathie, G.R.Smith, M.Meyer, F.Vogler, S.Mango, J.A.Konter, G.S.Mutchler, J.Arvieux - Phys.Rev.Lett. 48, 1667 (1982) Further Measurements of i T t l i n ~r - d ( p o l ) S c a t t e r i n g a s a n I n v e s t i g a t i o n of Dibaryon Resonance Effects S.B.Borzakov, H.Maletski, L.B.Pikelner, M.Stempinski, E . I . S h a r a p o v - Y a d . F i z . 35, 532 ( 1 9 8 2 ) Peculiarities in Deviation from t h e v -1 L a w f o r 3 H e ( n , p ) T R e a c t i o n C r o s s S e c t i o n . E x c i t e d L e v e l o f t h e 4He N u c l e u s D.D.Bogdanov, M.P.Ivanov, C.S.Popeko, A.M.Rodin, G.M.Ter-Akopian, V.I.Vakatov, A.S.Voronin P h y s . L e t t . l13B, 213 (1982) The Spontaneous Fission of 244Fm and a4eFm P.D.Bond, O.Hansen, C.E.Thorn, M . J . L e V i n e , P.R. C h r i s t e n s e n , S.Pontoppidan, F.Videbaek, Jiang Cheng-Lie, M.J.Rhoades-Brown - P h y s . L e t t . I14B , 4 2 3 (1982) Mutual Inelastic Excitation o f aSSi + e°Ni

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A386,

308

(1982) 82Bo39

82Br03 82Br04

82Br05 82Br06

D e c a y s of *8~m+gHg: L o w - s p i n l e v e l s o f lSSAu a s a t e s t o f n u c l e a r models R.Bock, Y.T.Chu, M.Dakowski, A.Gobbi, E.Grosse, A.Olmi, H.Sann, D.Schwalm, U.Lynen, W.Muller, S.Bjornholm, H . E s b e n s e n , W . W o l f l i , E . M o r e n z o n i - N u c l . P h y s . A 388, 3 3 4 (1982) Dynamics of the Fusion Process A . B r o n d i , R . M o r o , V . R o c a , F . T e r r a s i , B . G o n s i o r - L e t t . N u o v o C i m . 33, 25 (1982) Gamma-Decay o f g g / a I s o b a r i c A n a l o g R e s o n a n c e s i n 51Mn F.P.Brady, C.M.Castaneda, G.A.Needham, J.L.Ullmann, J.L.Romero, T.Ford, M.L.Johnson, N.S.P.King, C.M.Morris, F.Petrovich, R . H . H o w e l l - P h y s . R e v . L e t t . 48, 860 (1982) Isovector and Gamow-Teller Strength from Small-Angle ( n , p ) R e a c t i o n s a t 60 MeV S.Brussermann, J.Keinonen, H.P.Hellmeister, K . P . L i e b - Z . P h y s . A 3 0 4 , 335 (1982) Recoil Distance Lifetime Measurements i n 82Kr A.S.Bratashevsky, A.I.Derebchinsky, A.A.Zybalov, S.P.Karasev, O.G.Konovalov, P.V.Sorokin, A . E . T e n i s h e v - Y a d . F i z . 35, 56 (1983) P o l a r i z a t i o n o f t h e R e c o i l P r o t o n s i n 7 + P -~ P + rr° R e a c t i o n f o r E7 = 0 . 6 5 - 1 . 4 GeV a t e(rr) = 700 c.m.

82Br07

82Br09 82BrlO 82Br12

82Br13 82Br14 82Br15

82Br16

82Br17

82Br18 82Br19 82Br21 82BuO1 82Bu03

82Bu04 82Bu05

82Bu06 82Bu07 82Bu08 82Bu09 82Bu13

V.B.Brudanin, N.A.Golovkov, B.S.Dzhelepov, R.B.lvanov, M.A.Mikhailova, A.V.Saulsky Izv.Akad.Nauk SSSR, S e r . F i z . 48, 45 (1982) Certain Observations o n t h e D e c a y o f 2° 6A t M.Bruno, F.Cannata, M.D'Agostino, C.Maroni, I.Massa, M.Lombardi - N u o v o C i m . 68A , 35 (1982) Experimental Study on Low-Energy ZH(a,a)2H Elastic Scattering W.Bruchle, G.Herrmann - Radiochim.Acta 30, 1 (1982) Decay Properties of Neutron-Rich Silver Isotopes W.J.Briscoe, D.H.Fitzgerald, B.M.K.Nefkens, H.Crannell, D.I.Sober, R.Goloskie, W.W.Sapp,Jr. Phys.Rev.Lett. 49, 187 (1982) Two-Body Photodisintegration o f 3He b e t w e e n 150 a n d 350 MeV R.Broda, P.Kleinheinz, S.Lunardi, J.Styczen, J.Blomqvist - Z . P h y s . A 305, 281 (1982) T h e D e c a y o f t h e 560 n s I s o m e r a t 8.6 MeV i n 14~64Gd83 J.E.Brock, A.Chisholm, J . C . D u d e r , R . G a r r e t t - N u c l . P h y s . A 382, 221 (1982) The Analysing Power in the Elastic Scattering o f 14 MeV N e u t r o n s by Deuterons H.Bruchertseifer, B.Eichler, J.Estevez, T.Cruz, I.Zvara Radiochem.Radioanal.Lett. 51, 319 (1982) Untersuchung der Produkte der Reaktion 151Eu + 2°Re V.Brabec, M.Rysavy, O.Dragoun, M.Fiser, A.Kovalik, Cs.Ujhelyi, D.Berenyi Z . P h y s . A306, 347 (1982) Nuclear Structure and Chemical Effects in Internal C o n v e r s i o n of t h e 35 k e V M1 + E2 T r a n s i t i o n i n 125Te M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Frisoni, G.Vannini, M.Lombardi Nucl.Phys. A386, 269 (1982) The Low Energy 2H(a,ap)n Reaction J . C . B r o w n e , B . L . B e r m a n - P h y s . R e v . C26, 969 (1982) Neutron-Capture R e s o n a n c e s f o r BaSe R . A . B r a g a , R . W . F i n k - P h y s . R e v . C26, 1302 (1982) Lifetime of the 724.3-keV Level and Shell-Model Intruder S t a t e s i n *°gAg R.Broda, C.Gunther, B.V.Thirumala R a o - N u c l . P h y s . A 389, 366 (1982) High-Spin S t a t e s i n 2°lBi P o p u l a t e d in the (a,6n) Reaction B . L . B u r k s , R . R . C a d m u s , J r . , T.B.Clegg, E . J . L u d w i g - N u c l . P h y s . A377, 105 (1982) Spins and Parities of Low-Lying S t a t e s i n ~gKr f r o m the 7SKr(d(pol),p)79Kr Reaction B.L.Burks, R.E.Anderson, T.B.Clegg, H . P a e t z g e n . S e h i e c k , E.J.Ludwig, R.L.Varner, J.F.Wilkerson P h y s . R e v . C25, 1168 (1982) T e s t of t h e P o l a r i z a t i o n - A n a l y z i n g Power Equality in Two (p(pol),d) Reactions and Their Inverses B . B u d i c k , R . A n i g s t e i n , J . W . K a s t - P h y s . L e t t . l l 0 B , 375 (1982) Nuclear Excitation in the Reaction a°TPb(/z-,u6n)2°lTl P.E.Burt, L.W.Fagg, H . C r a n n e l l , D.I.Sober, W.Stapor, J.T.O'Brien, X.K.Maruyama, J.W.Lightbody, R . A . L i n d g r e n - P h y s . R e v . C25, 2 8 0 5 (1982) Electron Scattering S t u d y o f t h e 10.32 MeV T r a n s i t i o n i n 4°Ca V.N.Bugrov, S.A.Karamyan - Y a d . F i z . 35, 558 (1982) Study of Time Components o f N u c l e a r F i s s i o n R e a c t i o n s 238U + ~aC a n d W + 2ZNe V.S.Butsev, D.Chultem, I . N . Z h i v o t o v - N u c l . P h y s . A 382, 501 (1982) Negative Pion Capture in Atomic Nuclei near the Closed Neutron S h e l l a t N = 82 C.Budtz-Jorgensen, P.T.Guenther, A . B . S m i t h , J . F . W h a l e n - Z . P h y s . A306, 265 (1982) Fast-Neutron Total and Scattering C r o s s S e c t i o n s o f 5BNi P . E . B u r t , L.W.Fagg, H . C r a n n e l l - P h y s . R e v . C26, 713 (1982) Magnetic Electroexcitation o f t h e 0 . 4 7 8 MeV S t a t e i n 7Li a t L o w M o m e n t u m Transfer J . B u r d e , V . R i c h t e r , J . T s a l i a h , I . L a b a t o n - N u c l . P h y s . A385, 29 (1982) T h e E x c i t e d S t a t e s i n t h e O d d - O d d 124I N u c l e u s P r o d u c e d by the (p,n) Reaction

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82Ca15

82Ca16

82Ce01 82Ce02

82Ch01

82Ch02

82Ch05 82Ch06

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82Co05 82Co08

82Co09

82Coli 82Co12

82Co15 82CrO1 82Cr02

82CsO1 82CuOl 82Cu02

82DaO1

Y.-D.Chan, D.E.DiGregorio, J.L.C.Ford,Jr, J.Gomez del Campo, M.E.Oritz, D.Shapira Phys.Rev. C25, 1 4 1 0 ( 1 9 8 2 ) 1°B + 170 F u s i o n C r o s s S e c t i o n s l.Chiodi, S.Lunardi, M.Morando, C.Signorini, G.Fortuna, W.Starzecki, A.M.Stefanini, O.Korschinek, H.Morinaga, E.Nolte, W.Schollmeier - L e t t . N u o v o C i m . 33, 159 (1982) Multinucleon Transfer in the Interaction of 5SNi w i t h l a 4 S n a r o u n d the Coulomb Barrier J . S . C h a n g , V . K . C . C h e n g , H . H . L i n , C.C.Hsu - P h y s . R e v . 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C 2 6 , 1544 (1982) R e a c t i o n s leC(Tr+,~r±d)l°B a n d lZC(~r±,Tr+t)SB J . M . E n a g o n i o , F . P . C a l a p r i e e , R . W . D u n f o r d , M . M . L o w r y - P h y s . R e v . C25, 1047 (1982) P a i r D e c a y o f t h e 15.1 MeV L e v e l o f laC

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82Ew01 82Fa01 82Fa05 82Fa06

82Fa07 82Fa08 82Fa09 82FalO 82Fa11 82Fa12 82FeO1 82Fe02 82FiO1

82Fi02 82Fi03 82Fi06

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(IL982) 82Fi07

82Fi08

82Fi09 82Fi10

Interacting Negative-Parity B a n d s i n 164Er C . A . F i e l d s , F.W.N.De B o e r , R . A . R i s t i n e n , E . S u g a r b a k e r - P h y s . L e t t . l 1 4 B , 81 ( 1 9 8 2 ) B r e a k d o w n of t h e T h e r m a l M o v i n g - S o u r c e D e s c r i p t i o n of F a s t N e u t r o n P r o d u c t i o n i n ( a , x n ) a n d (3He, xn) Reactions R.W.Finlay, C.E.Brient, D.E.Carter, A.Marcinkowski, S.Mellema, G.Randers-Pehrson, J.Rapaport Nuel.Instrum.Methods 198, 197 (1982) The Ohio University Beam Swinger Facility C . A . F i e l d s , R . A . R i s t i n e n , L . E . S a m u e l s o n , P . A . S m i t h - N u c l . P h y s . A 385, 4 4 9 (1983) A S t u d y o f t h e 9 ° Z r ( a H e , t ) R e a c t i o n a t 4 3 . 4 MeV L.K.Fifield, J.L.Durell, M.A.C.Hotehkis, J.R.Leigh, T.R.Ophel, D.C.Weisser Nucl.Phys. A385,

505 (198e) The

Mass

of

tSC f r o m

a Heavy

Ion

Double-Charge-Exchange

177

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82Fu04

82Fu06

82Fu07 82Fu08

82Fu09

82Ga02

82Ga05 82Ga06

R.Fischer, C.Derndorfer, B.Strohmaier, H.Vonach - Ann.Nucl.Energy 9, 4 0 9 (1982) Investigation of the a-Particle Emission from t h e R e a c t i o n ~3Nb + n a t E ( n ) = 14.1 MeV D.Fink, E.Friedman, M . P a u l , A . M o a l e m - N u c l . P h y s . A 389, 18 (1982) Experimental Determination of t h e N o r m a l i z a t i o n Constant of the (a,t) Reaction C.A.Fields, K.H.Hicks, R.A.Ristinen, F.W.N.De Boer, P.M.Walker, J.Borggreen, L.P.Peker N u c l . P h y s . A389, 218 (1982) A Study of the Rotational Side-Bands i n l~2Dy C.E.Floyd, P.P.Guss, K.Murphy, C.R.Howell, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg - P h y s . R e v . C25, 1682 ( 1 9 8 2 ) Analyzing Powers for Neutron Elastic Scattering at Forward Angles D . G . F l e m i n g - C a n . J . P h y s . 60, 4 2 8 (1982) A 20 MeV ( p , d ) S t u d y o f N u c l e a r S t r u c t u r e in the Even and Odd Tin Isotopes D . S . F l y n , R . L . H e r s h b e r g e r , F . G a b b a r d - P h y s . R e v . 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8 2GeO3 82Ge04 82Ge05

8 2GeO6

82Gi01

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82G101

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82G103

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82Gr17 82Gr19

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82Ha17

82Ha21

82Ha22

82Ha25

82Ha26

82Ha27

82Ha28 82Ha31

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82Hill 82Ho01

82Ho02

82Ho04

82Ho06 82Ho07 82Ho08 82Ho09

E.Hagberg, J.C.Hardy. H.Schmeing, H.C.Evans, U.J.Schrewe, V.T.Koslowsky, K.S.Sharma, E . T . H . C l i f f o r d - N u c l . P h y s . A 383, 109 (1982) T h e D e c a y o f a N e w N u c l i d e : 7*Br G.Haouat, J.Lachkar, C h . L a g r a n g e , J . J a r y , J . S i g a u d , Y . P a t i n - N u c l . S c i . E n g . 81, 491 (1982) Neutron Scattering C r o s s S e c t i o n s f o r 232Th,233U,235U,23eU,239pu,and 2~2Pu b e t w e e n 0.6 a n d 3.4 MeV G.Hardie, S.A.Gronemeyer, L.Meyer-Schutzmeister, A . J . E l w y n - P h y s . R e v . C26, 4 5 6 (1 9 8 2 ) 7 D e c a y o f S t a t e s i n 4~Cr A.Hachem - Nucl.Instrum.Methods 198, 305 (1982) Un S p e c t r o m e t e r a Somme et Coincidence Hybride a Deux Voies d'Observation E . H a g n , E . Z e c h - Z . P h y s . A307 , 159 (1982) NMR-ON M e a s u r e m e n t of the Electric Quadrupole Interaction o f 199Au i n Fe E.E.Habib, J . A . C a m e r o n , G.U.Din, V . J a n z e n , R . S c h u b a n k - P h y s . R e v . C26, 8 3 4 (1982) Determination of t h e S p i n s a n d P a r i t i e s o f L o w - L y i n g S t a t e s i n ggMo b y M e a n s of t h e l ° ° M o ( d ( p o l ) , t)99Mo a n d 9 8 M o ( d ( p o l ) , p ) 9 9 M o R e a c t i o n s J.Hattula, H.Helppi, A.Luukko - P h y s . S e r . 26, 205 (1982) In-Beam S t u d y o f 122,124,12°Xe U.Hagemann, L . K a u b l e r , H . - J . K e l l e r , F . R . M a y , H . P r a d e , F . S t a r y - N u c l . P h y s . A 389, 341 ( 1 9 8 2 ) Investigation o f t21I L e v e l s O b s e r v e d i n t h e ( 3 H e , 3 n ) R e a c t i o n R . W . H a r p e r , T . W . G o d f r e y , J . L . W e i l - P h y s . R e v . C26, 1 4 3 2 (1982) Interaction of Neutrons w i t h E v e n - A T i n I s o t o p e s . I. T o t a l C r o s s S e c t i o n f o r E ( n ) = 0 . 3 - 5 . 0 MeV He Y o u f e n g , S . M . Q a i m , G . S t o c k l i n - I n t . J . A p p l . R a d i a t . I s o t o p . 33, 13 (1982) Excitation Functions for 3He-Particle Induced Nuclear Reactions o n 76Se,77Se a n d (nat)Se: Possibilities of production of ~Kr R.G.Helmer, C.W.Reich, R.J.Gehrke, J.D.Baker - Int.J.Appl.Radiat.Isotop. 33, 23 (1982) Emission Probabilities and Energies of 7-Ray Transitions f r o m t h e 239pu D e c a y J.Heisenberg, J.Lichtenstadt, C . N . P a p a n i c o l a s , J . S . M c C a r t h y - P h y s . R e v . C25, 2 2 9 2 (1982 ) Excitation o f Low L y i n g N a t u r a l P a r i t y Levels in 2°sPb by Inelastic Electron Scattering A . M . H e r n a n d e z , W . W . D a e h n i c k - P h y s . R e v . C25, 2 9 5 7 (1982) fl+ D e c a y o f 18Ne a n d t h e f t V a l u e o f t h e 0 + ~ O- B r a n c h B.Heusch, C.Beck, J.P.Coffin, P.Engelstein, R.M.Freeman, G.Guillaume, F.Haas, P.Wagner P h y s . R e v . 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18~

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82Is04 82Is05 82Is06

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82Ja08

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82Ka07 82Ka08 82Ka09 82Ka10 82Ka12 82Kai5 82Ka17 82Ka21 82Ka22

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82Ki04

82Ki05 82Ki06

Neutron-Proton Scattering C r o s s S e c t i o n s b e t w e e n 200 a n d 500 MeV S.A.Kerr, P.Hungerford, K.Schreckenbaeh - Nucl.Instrum.Methods 195, 505 (1982) Precise Intensity Measurement of Primary ~/-Rays from the 197Au(n(th),-y)~98Au Reaction E.D.Kern, K.Sistemich, W . - D . L a u p p e , H . L a w i i . - Z . P h y s . A 306, 161 ( 1 9 8 2 ) T h e B e t a D e c a y o f l ° 4 N b a n d t h e L e v e l S c h e m e of '°4Mo C.Keveloh, K.P.Lieb, H.P.Hellmeister - P h y s . R e v . C26, 716 (1982) Lifetime Measurements o f H i g h S p i n S t a t e s i n S~Fe J.Keinonen, A.Anttila, A.Luukkainen - N u c l . P h y s . A385, 461 (1983) A n a l o g u e E2 T r a n s i t i o n s i n t h e A = 26 N u c l e i K.U.Kettner, H.W.Becker, L.Buchmann, J.Gorres, H.Krawinkel, C.Rolfs, P.Schmalbrock, H.P.Trautvetter, A . V l i e k s - Z . P h y s . A 3 0 8 , 73 (1982) T h e 4He(12C,'y)160 R e a c t i o n a t S t e l l a r E n e r g i e s A.E.Khalil, F.T.Avignonne IIlP h y s . R e v . A36, 770 (1982) Absolute Pair-Production Cross-Section Measurements i n T a r g e t s o f Z = 2 6 , 2 9 , 5 0 , 8 2 , a n d 92 w i t h 1.119-MeV Photons R.Kirchner, O.Klepper, W.Kurcewicz, E.Roeekl, E.F.Zganjar, E.Runte, W.-D.Schmidt-Ott, P.Tidemand-Petersson, N.Kaffrell, P.Peuser, K.Rykaczewski - N u c l . p b . y s . A 378, 5 4 9 (1982) New Neutron-Rich ~gYb and lel,lS2Lu Isotopes Produced i n R e a c t i o n s o I ~ M ~ V / u 136Xe I o n s o n Tantalum and Tungsten Targets S . E . K i n g , M . P o t o k a r , N . R . R o b e r s o n , H . R . W e l l e r , D . R . T i l l e y - N l c l . P h y s . A 3 8 4 , 129 (1982) Neutron Capture i n t h e G i a n t R e s o n a n c e R e g i o n o f 2° gP b M.Kildir, D.Logan, M.Kaplan, M.S.Zisman, D.Guerreau, J.M.Alexander, L.C.Vaz - Z . P h y s . A 3 0 6 , 323

(1982) 82Ki07 82K102

S t u d i e s o f ~He E m i s s i o n in Both Fusion-Like a n d I n e l a s t i c R e a c t i o n s o f 3 4 0 - M e V 4 ° A t + 238U U . K i s e h k o , J . S c h w e i z e r , F . T a s s e t - Z . P h y s . A 307, 163 (1982) Neutron Interferol~etric Measurement of the Coherent Scattering Length of Cobalt ~'/.Klamra, K.Fransson, B.Sundstrom, M.Brenner, S.Engman, R.Kvarnstrom - N u c l . P h y s . A376, 4 6 3

(1982) 82K103

82K104 82K106 82Kn03

82Ko03

82Ko05 82Ko06 82Ko08

82Ko16 82Ko17

82Ko20 82Ko24 82Kr02 82Kr03 82Kr04

High Spin Collective Excitations i n ~°tRu O.Klepper, T.Batsch, S.Hofmann, R.Kirchner, W.Kurcewiez, W.Reisdorf, E.Roeckl, D.Schardt, ? , . N y m a n - Z . P h y s . A305, 125 ( 1 9 8 2 ) Direct and Beta-Delayed Proton Decay of Very Neutron-Deficient Rare-Earth Isotopes Produced in [ h e R e a c t i o n SgNi + 92Mo P.Kleinheinz, J.Styczen, M.Piiparinen, J.Blomqvist, M.Kortelahti - P h y s . R e v . L e t t . 48, 1 4 5 7 ( 1 9 8 2 ) Two-Phonon Octupole Excitation i n 147Gd PKleinwachter, I.Rotter - J.Phys.(London) Gg, 955 (1982) On R e s o n a n c e P h e n o m e n a in Nuclear Reaction Cross Sections J.W.Knowles, W.F.Mills, R.N.King, B.O.Pich, S.Yen, R.Sobie, L.Watt, T.E.Drake, L.S.Cardman, R.L.Gulbranson - P h y s . L e t t . l16B, 315 (1982) A High-Resolution Measurement of the Photofission Spectrum o f 232Th n e a r T h r e s h o l d J.Konijn, J.B.R.Berkhout, W.H.A.Hesselink, J.J.Van Ruijven, P .V .N e s , H . V e r h e u l , F.W.N.De B o e r , C.A.Yields, E.Sugarbaker, P . M . W a l k e r , R . B i j k e r - N u c l . P h y s . A 373, 397 (1983) Rotational Bands in lSaSm Observed following the (a,2n3,) Reaction M.Kortelahti, A.Pakkanen, M.Piiparinen, T . K o m p p a , R . K o m u - N u c l . P h y s . A 376, 1 (198 2 ) Medium-Spin L e v e l s a n d a 3 6 0 n s Iw = 1 9 / 2 - I s o m e r i n t h e N = 80 N u c l e u s ~aTLa R . T . K o u z e s , M . M . L o w r y , C . L . B e n n e t t - P h y s . R e v . C25, 1076 (1982) G~cound S t a t e M a s s o f 81Kr a n d t h e S o l a r N e u t r i n o Problem L.K.Kostov, H.Rotter, C.Heiser, H.Prade, F.Stary, W.Andrejtscheff - N u e l . P h y s . A 376, 451 ( 1 9 8 2 ) A b s o l u t e E1,AK = 1 T r a n s i t i o n Probabilities between Multi-Quasiparticle High-Spin S t a t e s i n 17SHf a n d 17SHf K.Kobayashi, I.Kimura, W.Mannhart - J.Nucl.Sci.Technol.(Tokyo) 19, 341 (1982) Measurement and Covariance Analysis of Californium-252 Spectrum Averaged Cross Sections S.Kohmoto, M.Ishihara, H.Kamitsubo, T.Nomura, Y.Gono, H.Utsunomiya, T.Sugitate, K.Ieki P h y s . L e t t . l 1 4 B , 107 ( 1 9 8 2 ) Final-State Interaction and Time Information in 14N-Induced Reactions Studied by a-a Correlations I.A.Korzh, V.A.Mizhehenko, E.N.Mozhzhukhin, N.M.Pravdivy - Y a d . F i z . 35, 1097 (1982) Investigation of Scattering of Fast Neutrons o n SaCr J.J.Kolata, E.G.Funk, J.D.Hinnefeld - P h y s . R e v . C26, 1750 (1983) Lifetime of the 4848-keV S t a t e i n lSF H.-D.Kronfeldt, J.-R.Kropp, R . W i n k l e r - P h y s i c a 112C, 138 (1988) The Isotope Shift of the a ~°D-Term of the Configuration 4f75d6s in Eu 1 A.J.Kreiner, P.D.Bond, C.Baktash, J.Barrette, C . E . T h o r n , M . T . C o l l i n s - P h y s . R e v . C25, 866 ( 1 9 8 2 ) Structure a n d D e c a y o f t h e H i g h l y M i x e d 1 3 / 2 + S t a t e s i n 17~Er K . S . K r a n e - N u c l . P h y s . A 3 7 7 , 176 ( 1 9 8 2 ) Nuclear Orientation o f ~S°Tb i n Tb M e t a l

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(1982) 83La15

83LeOl

82Le02

82Le03 82LeO4 83Le05

82Le06

83Le07

Deuteron Breakup b y 140 MeV A l p h a P a r t i c l e s a t Q u a s i f r e e S c a t t e r i n g Conditions M.C.Lagunas-Solar, F.E.Little, H.A.Moore Jr. - Int.J.Appl.Radiat.Isotop. 33, 619 ( 1 9 8 3 ) Cyclotron Production of 128Cs (3.62 r a i n ) . A N e w P o s i t r o n - E m i t t i n g Radionuclide for Medical Applications D.Lee, H . v o n G u n t e n , B.Jacak, M.Nurmia, Yuan-fang Liu, C h e n g Luo, G.T.Seaborg, D . C . H o f f m a n P h y s . R e v . C25, 286 (1982) Production of Heavy Actinides from Interactions o f 160,1eO,2°Ne,and 22Ne w i t h 248Cm R.Levy, N . T s o u p a s , N.K.B.Shu, A . L o p e z - G a r c i a , W.Andrejtscheff, N.Benczer-Koller - P h y s . R e v . C25, 293 (1983) Magnetic Moment Measurements in Osmium and Platinum Nuclei P . M . S . L e s s e r , C . C . T r a i l , C . C . P e r n g , M . K . L i o u - P h y s . R e v . L e t t . 48, 308 (1982) Bremsstrahlung from 12C + p n e a r t h e 4 6 1 - k e V R e s o n a n e e K.T.Lesko, D.-K.Lock, A.Lazzarini, R.Vandenbosch, V . M e t a g , H . D o u b r e - P h y s . R e v . C35, 8 7 3 ( 1 9 8 2 ) E n e r g y D e p e n d e n c e o f F u s i o n C r o s s S e c t i o n f o r 28Si + 12C b y E v a p o r a t i o n Residue Measurements J . R . L e i g h , D . J . H i n d e , J . O . N e w t o n , W . G a l s t e r , S.H.Sie - P h y s . R e v . L e t t . 48, 537 ( 1 9 8 2 ) F i s s i o n - l m p o s e d L i m i t s to t h e A n g u l a r M o m e n t u m C a r r i e d b y E v a p o r a t i o n R e s i d u e s f r o m t h e C o m p o u n d Nucleus 2°°Pb J.J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, E.J.Winhold, P.P.Yergin, A.M.Bernstein, K.I.Blomqvist, S.Dytman, G.Franklin, M . P a u l i - P h y s . R e v . C25, 1703 (1982) Anomalously L o w C r o s s S e c t i o n i n 13C(7,Tr-)laN(g.s.) I.Y.Lee, N.R.Johnson, P.K.McGowan, R.L.Robinson, M.W.Guidry, L.L.Riedinger, S.W.Yates P h y s . R e v . C25, 1865 (1982) Structure of M u l t i p h o n o n Vibrational States in l°e,ilspd

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(1982) 82Lu05

82LyOl

82Ly02 82MaOl

Y i e l d s a n d R e c o i l P r o p e r t i e s of P r o d u c t s f r o m t h e R e a c t i o n b e t w e e n N a t u r a l C o p p e r a n d 86 M e V / A IZC I o n s T.Lund, D.Molzahn, B.Bergersen, T.Bjornstad, E.Hagebo, l.R.Haldorsen, C.Richard-Serre, the ISOLDE C o l l a b o r a t i o n - P h y s . L e t t . 116B, 325 (1982) Momentum Transfer and Product Kinetic Energies in the Interaction o f S i l v e r w i t h 86 M e V / A ~2C W.G.Lynch, L.W.Richardson, M.B.Tsang, R.E.Ellis, C.K.Gelbke, R.E.Warner Phys.Lett. 108B, 2 7 4 (1982) I n - P l a n e C o r r e l a t i o n s b e t w e e n P r o t o n s a n d D e u t e r o n s f o r ( 6 e - I n d u c e d R e a c t i o n s o n 27Al a n d 197Au a t 310 MeV W.G.Lynch, M.B.Tsang, H.C.Bhang, J.G.Cramer, R.J.Puigh - Phys.Rev.Lett. 48, 979 (1982 ) Relativity,Nuclear Polarizability,and Screening in Sub-Coulomb Elastic Scattering G.J.Mathews, J.B.Moulton, G.J.Wozniak, B.Cauvin, R.P.Schmitt, J.S.Sventek, L.G.Moretto P h y s . R e v . C35, 300 ( 1 9 8 2 ) a°Ne-Induced R e a c t i o n s w i t h Cu a n d 197Au a t 8.6 a n d 12.6 M e V / N u c l e o n

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82Ma04

82Ma05

82Ma07 82Mall

82Ma13 82Ma16

82Ma18

82Ma19

82Ma20 82Ma22

82Ma23 82Ma24 82Ma25

82Ma27 82Ma28

82Ma29 82Ma30

82Ma31 82Ma33 82Ma39

82Mc02

82Mc03 82Mc04

82Mc05

82Mc07

N.Matsuoka, K.Hatanaka, M.Fujiwara, Y.Fujita, T.Saito, K.Hosono, A.Shimizu, M.Kondo, F.Ohtani, H . S a k a g u c h i , A . G o t o , N . N a k a n i s h i , T . T o b a - N u c l . P h y s . A 373, 377 (1982) DWBA A n a l y s i s o f (SHe,d) R e a c t i o n s a t 90 MeV a n d C o n t r i b u t i o n s from the Nuclear Interior K.H.Maier, J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, T.Nail, R.K.Sheline, W . S t o f f l , L . U s s e r y - P h y s . R e v . L e t t . 48, 4 6 6 ( 1 9 8 2 ) g F a c t o r o f t h e JTr = 2 5 / 2 + I s o m e r i n 2°5T1 a n d t h e A n o m a l o u s O r b i t a l M a g n e t i s m of t h e P r o t o n C . P . M a s s o l o , S . F o r t i e r , J . M . M a i s o n , M.N.Rao - J . P h y s . ( L o n d o n ) G8, 361 (1982) The Fragmentation of the f-p Neutron-Hole Strength i n 91Mo b e l o w 6 MeV E x c i t a t i o n Energy R.Madey, A.Fazely, B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.J.McCarthy, P.C.Tandy, J.W.Watson, W . B e r t o z z i , T . B u t i , M . F i n n , M . K o v a s h , B . P u g h , C . C . F o s t e r - P h y s . R e v . C25, 1715 (1982) Analyzing P o w e r f o r t h e 1 6 0 ( p ( p o l ) , n ) ' 6 F ( 4 - , 6 . 3 7 MeV) R e a c t i o n a t 134 MeV H.Maria, J.Dalmasso, G.Ardisson - Nucl.Instrum.Methods 195, 621 (1982) S u r l ' E n e r g i e d e la T r a n s i t i o n E1 d e l ° a m A g D.Marlow, P.D.Barnes, N.J.Colella, S.A.Dytman, R.A.Eisenstein, R.Grace, F.Takeutchi, W.R.Wharton, S.Bart, D.Hancock, R.Hackenberg, E.Hungerford, W.Mayes, L.Pinsky, T.Williams, R.Chrien, H . P a l e v s k y , R . S u t t e r - P h y s . R e v . C25, 2619 (1982) Kaon Scattering f r o m C a n d Ca a t 800 M e V / c S . M a t s u k i , K.Ogino, Y.Kadota, N . S a k a m o t o , T.Tanabe, M.Yasue, A.Yokomizo, S.Kubono, Y.Okuma P h y s . L e t t . l l 3 B , 21 (1982) Splitting of Low-Lying Octupole Vibrational Strength i n 76 78,80,82Kr D.J.Margaziotis, M.B.Epstein, W.T.H.van Oers, D.K.Hasell, R.Abegg, G.A.Moss, L.G.Greeniaus, J . 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P h y s . A 382, 173 ( 1 9 8 2 ) Spin Determination of States with Stretched Configurations i n 16N a n d S2p V i a t h e ( d ( p o l ) , a ) R e a c t i o n a t 52 Mev R . L . M a c k l i n - N u c l . S c i . E n g . 81, 520 (1982) Technetium-99 Neutron Capture Cross Section H . M a c h n e r , U . B e c h s t e d t , A . D j a l o e i s , P . J a h n - P h y s . R e v . C26, 411 (1982) Mechanisms for Composite Particle Production in Nuclear Reactions using (a,a'X) Reactions up to 40 M e V / N u c l e o n H . - E . M a h n k e , E . D a f n i , M . H . R a f a i l o v i c h , G . D . S p r o u s e , E . V a p i r e v - P h y s . R e v . C26, 4 9 3 (1 9 8 2 ) Quadrupole M o m e n t o f t h e 8 - I s o m e r i n Xl2Sb W.Mayer, D.Pereira, K.E.Rehm, H.J.Scheerer, H.J.Korner, G.Korschinek, W.Mayer, P.Sperr, S . C . P i e p e r , R . D . L a w s o n - P h y s . R e v . C26, 500 (1982) Strong Population o f E x c i t e d 0 + S t a t e s i n E v e n Zr I s o t o p e s O b s e r v e d w i t h t h e (14C,160) R e a c t i o n R.M.Macfarlane, D.P.Burum, R.M.Shelby - Phys.Rev.Lett. 49, 636 (1982) New D e t e r m i n a t i o n o f t h e N u c l e a r M a g n e t i c M o m e n t o f 141Pr R.L.Macklin, D.M.Drake, J.J.Malanify, E . D . A r t h u r , P . G . Y o u n g - N u c l . S c i . E n g . 82, 143 (19 8 2 ) Cross Section of the 169Tin(n,7) Reaction from 2.6 k e V t o 2 MeV D.W.MacArthur, F.P.Calaprice, A.L.Hallin, M.B.Schneider, D.F.Schreiber Phys.Rev. C26, 1753 (1982) N u c l e a r M a g n e t i c M o m e n t o f 'gNe w i t h P o s s i b l e A p p l i c a t i o n s to Other Radioactive G as I s o t o p e s R.J.McDonald, A.J.Pacheeo, O.J.Wozniak, H.H.Bolotin, L.O.Moretto, C.Schuck, S.Shih, R.M.Diamond, F . S . S t e p h e n s - N u c l . P h y s . A 3 7 3 , 54 (1982) Evidence for Spin Fluctuations in the Deep-lnelastic R e a c t i o n leSHo + '65Ho a t 8.5 M e V / a m u R . C . M c B r o o m , H . R . W e l l e r , N . R . R o b e r s o n , D . R . T i l l e y - P h y s . R e v . C25, 1 6 4 4 (1982) SH(p,-y)4He R e a c t i o n b e l o w E( p) = 30 MeV M.W.McNaughton, B.E.Bonner, W.D.Cornelius, E.W.Hoffman, O.B.van Dyck, R.L.York, R.D.Ransome, C . L . H o l l a s , P . J . R i l e y , K . T o s h i o k a - P h y s . R e v . C25, 1967 (1982) Spin Transfer Measurements f o r p p ~ p p a t 800 MeV M.W.McNaughton, E.P.Chamberlin, J.J.Jarmer, N.S.P.King, H . B . W i l l a r d , E . W i n k e l m a n - P h y s . R e v . C25, 2107 (1982) Spin Correlation A(nn) and Analyzing P o w e r A i n p p ~ p p a t 6 4 3 MeV M.W.McNaughton, B.E.Bonner, E.W.Hoffman, O.B.van Dyck, C.L.Hollas, P.J.Riley, K.H.McNaughton, K . l m a i , K . T o s h i o k a , J . R o b e r t s , S . E . T u r p i n , B.Aas, A . R a h b a r - P h y s . R e v . C26, 2 4 9 (198 2 ) Spin Transfer Measurements f o r p p ~ p p a t 6 4 7 MeV

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82Me01

82Me02

82Me03 82Me04 82Me05 82Me06 82MelO

82Mi01

82Mi03 82Mi06

82Mi08

83Mo01

82Mo02

82Mo04

82Mo05 82Mo06

82Mo09

82Mo10

82Moli

82Mo12

82Mo13

82Mo15 82Mo16

D.K.MeDaniels, P.Varghese, D.M.Drake, E.Arthur, A.Lindholm, I.Bergqvist, J.Krumtinde N u c l . P h y s . A384, 88 (1982) R a d i a t i v e C a p t u r e o f F a s t N e u t r o n s b y 16Silo a n d 238U R A . M e y e r , O.G.Lien III, E . A . H e n r y - P h y s . R a v . C25, 682 (1982) Coexisting Intruder B a n d s i n 83Se a n d E v i d e n c e f o r t h e Role of P r o t o n S u b s h e l l Closure in Inhibiting Formation of Odd-Neutron Intruder Bands 3.P.M.G.Melssen, P.J.Van Hall, S.D.Wassenaar, O.J.Poppen]a, G.J.Nijgh, S.S.Klein Nucl.Phys. A376, 183 (1982) S c a t t e r i n g o f 21.1 MeV P o l a r i z e d P r o t o n s f r o m 89y D . F . M e a s d a y - C z e c h . J . P h y s . B32, 138 (1982) Experiments o n P i o n R e a c t i o n s b e l o w 50 MeV J.S.Merritt, A.R.Rutledge, L.V.Smith - Int.J.Appl.Radiat.lsotop. 33, 77 (1982) Measurement of the Probability f o r 9 0 9 - k e V - y - R a y E m i s s i o n f o l l o w i n g t h e D e c a y of 89Sr V.Metag, A . L a z z a r i n i , K . L e s k o , R . V a n d e n b o s c h - P h y s . R e v . C25, 1486 (1982) Search for 7 Rays from the Quasimolecular 12C + 1~C S y s t e m M . O . M e r m a z , A . G r e i n e r , M.LeVine, F . J u n d t , J . - P . C o f f i n , A . A d o u n - P h y s . R e v . C25, 2815 (1982) Cross-Section Fluctuations i n t h e Z4Mg,12C S c a t t e r i n g s a t H i g h I n c i d e n t E n e r g y R . A . M e y e r , J . W . T . M e a d o w s , E.S.Macias - J . P h y s . ( L o n d o n ) G8, 1413 (1982) Opposing Properties of Partic le -Hole a nd Intrude r-Hole B a n d s i n N = 87 N u c l e i a n d 149Sin L e v e l s P o p u l a t e d b y 1 4 9 P m ( f l - ) a n d 149Eu(EC) E.Michelakakis, W.D.Hamilton, P.Hungerford, G . J u n g , P . P f e i f f e r , S.M.Scott - J . P h y s . ( L o n d o n } G8, l J J (1982) Levels and Transitions i n 14z,t44Ce P o p u l a t e d f o l l o w i n g t h e fl D e c a y o f 142,~4~La E . M i c h e l a k a k i s , W . D . 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N u o v o C i m . 33, 407 (1982) On ~he L i f e t i m e o f t h e 1.701 MeV L e v e l i n ~SF D.M.:.~Ioltz, K . S . T o t h , F . T . A v i g n o n e III, H . N o m a , B . G . R i t c h i e , B . D . K e r n - P h y a . L e t t . 113B, 16 (1982) Precision Mass D i f f e r e n c e Measurements in Light Rubidium and Krypton Isotopes Utilizing Beta-Endpoints H.P.Morsch, M.Rogge, P.Turek, C.Mayer-Boricke, P.Decowski - Phys.Rev. C25, 2939 (1982) E x c i t a t i o n of Isoscalar Giant Resonances and Monopole Giant Resonance S p l i t t i n g i n A e t i n i d e Nuclei C.L.Morris, H.T.Fortune, L.C.Bland, R.Gilman, S.J.Oreene, W.B.Cottingame, D.B.Holtkamp, G . R . B u r l e s o n , C.F.Moore - P h y s . R e v . C25, 3218 (1982) T a r g e t Mass D e p e n d e n c e o f I s o t e n s o r D o u b l e C h a r g e E x c h a n g e : E v i d e n c e f o r d e l t a s i n n u c l e i Z.Moroz, P.Zupranski, R.Bottger, P.Egelhof, K.-H.Mobius, G.Tungate, E.Steffens, W.Dreves, I . K o e n i g , D . F i e k - N u c l . P h y s . A381, 294 (1982) The Interaction of A l i g n e d 7Li w i t h SSNi H . M o r g e n s t e r n , W . B o h n e , K . G r a b i s c h , D . G . K o v a r , H . L e h r - P h y s . L e t t . 113B, 463 (1982) Incomplete Momentum Transfer in Heavy-Ion F u s i o n a t 14.5 M e V / N u c l e o n E.Monnand, J.A.Pinston, F.Schussler, B.Pfeiffer, H.Lawin, G.Battistuzzi, K.Shizuma, K.Sistemich Z . P h y s . A306, 183 (1982) E v i d e n c e f o r a R o t a t i o n a l B a n d i n 99y K.-H.Mobius, R . B o t t g e r , P . E g e l h o l f , Z.Moroz, E . S t e f f e n s , G.Tungate, I.Koenig, D.Fiek - Z.Phys, A306, 335 (1982) The Influence of the Spectroscopic Deformation of L i - I s o t o p e s on T h e i r I n t e r a c t i o n w i t h 5IV D.M.Moltz, K . S . T o t h , Y . A . E l l i s - A k o v a l i , J.D.Cole - P h y s . R e v . C26, 1316 (1982) D e c a y o f lS°Er -

82Mo17

82Mo19

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82Mu02 82Mu08 82NAB2 82Na0}4

82NaO5

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82Na10

82Na17 82NeOl

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82Ne04

82Ni01 82No0}1

82No02

82No0}3 82No04

82No06 82No0}7

82No08

82No09 82No10

82NuOl 82Nu02

D.J.Morrissey, G.J.Wozniak, L.G.Sobotka, A.J.Pacheco, R.J.McDonald, C.C.Hsu, L.G.Moretto N u c l . P h y s . A389, 120 (1982) I n t r i n s i c F r a g m e n t S p i n s G e n e r a t e d i n t h e R e a c t i o n s o f 2°Ne w i t h 197AU a n d 23au at 12.6 M e V / N u c l e o n T.Murakami, S . N i s h i h a r a , T . N a k a g a w a , S . M o r i t a , H . O r i h a r a , K.Maeda, K . M i u r a - N u c l . P h y s . A377, 163 (1982) The (p,n) Reaction on Cadmium I s o t o p e s L e a d i n g to t h e G r o u n d and Excited-State Analogs P.Mukherjee, S.Bhattacharya, S . S a r k a r , I . M u k h e r j e e , B . K . D a s m a h a p a t r a - P h y s . R e v . C25, 2120} (1982) A n o m a l o u s M4 C o n v e r s i o n C o e f f i c i e n t i n 125rn52Te M . J . M u r p h y , T . J . M . S y m o n s , G . D . W e s t f a l l , H . J . C r a w f o r d - P h y s . R e v . L e t t . 49, 455 (1982) Beta-Decay Half-Lives of Is otope s P roduc e d in P roje c tile F ra gm e nta tion H . 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A . R a y , C . D . H o y l e , E . C . A d e l b e r g e r - N u c l . P h y s . A 378, 29 (1982) B e t a D e c a y o f 24A1 a n d 24mA1 M.Rajagopalan, D.Logan, J.W.Ball, M.Kaplan, H.Delagrange, M.F.Rivet, J.M.Alexander, L.C.Vaz, M . S . Z i s m a n - P h y s . R e v . C25, 2417 (1982) Charged P a r t i c l e E m i s s i o n f r o m ' 9 4 H g Compound Nuclei: Energy and s p i n d e p e n d e n c e of f i s s i o n - e v a p o r a t i o nc o m p e t i t i o n A.Ramaswami, K.Raghuraman, B.K.Srivastava, R.H.lyer - Radiochim.Acta 30, 11 (1982) Absolute Yields of Fission P r o d u c t s in the T h e r m a l - N e u t r o n Induced Fission of 245Cm A.Ramaswami, B.K.Srivastava, S.B.Manohar, Satya Prakash, M.V.Ramaniah - Radiochim.Acta 30, 15 (1982) Charge Distribution in the Spontaneous F i s s i o n o f 252Cf: D e t e r m i n a t i o n of fractional cumulative y i e l d s o f ~3SXe a n d 139Cs C.Rangacharyulu, M.B.Chatterjee, C.Pruneau, C.St-Pierre - C a n . J . 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M e t h o d s 201, 315 (1982) M e a s u r e m e n t of t h e p - C A n a l y z i n g P o w e r b e t w e e n 109 a n d 750 MeV a n d t h e p - B e A n a l y z i n g P o w e r a t 780 MeV R.Ratzek, W.Wilke, J.Drexler, R.Fischer, R.Heil, K.Huber, U.Kneissl, H.Ries, H.Stroher, R.Stock, K.Wienhard - Z . P h y s . A308, 63 (1982) Photofission with Linearly Polarized Photons K.E.Rehm, W.Henning, J.R.Erskine, D.G.Kovar, M.H.Macfarlane, S.C.Pieper, M.Rhoades-Brown P h y s . R e v . C25, 1915 ( 1 9 8 2 ) Inelastic Scattering o f ' 6 0 f r o m 4°,4z,4~,4BCa G . R e f f o , F . F a b b r i , K . W i s s h a k , F . K a p p e l e r - N u c l . S c i . E n g . 80, 630 (1982) F a s t N e u t r o n C a p t u r e Cross S e c t i o n s a n d R e l a t e d G a m m a - R a y S p e c t r a of N i o b i u m - 9 3 , R h o d i u m - 1 0 3 , and Tantalum-181 A.Redder, H.W.Becker, H.Lorenz-Wirzba, C.Rolfs, P.Schmalbrock, H.P.Trautvetter - Z . P h y s . 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82Ri06

82Ro03

82Ro04

82Ro05 82Ro07

82Ro08

83Ro10

82Ro12

82Ro13

82Ro15 82Ro16

83Ru03

82Ru04 82RyOl

82Ry02 82SaOl 82Sa05

82Sa08

82Sa09 82Sa15

82Sa18

82Sa19

L.Rikus, S.F.Collins, K.A.Amos, B.M.Spicer, G.G.Shute, l.Morrison, V.C.Officer, R.Smith, D.W.Devins, D.L.Friesel, W.P.Jones - Aust.J.Phys. 35, 9 (1982); C o r r i g e n d u m Aust.J.Phys. 35, 351 (1982) Excitation o f t h e 9.50 MeV ( 9 / 2 + ) S t a t e s o f 13C i n I n t e r m e d i a t e Energy Scattering Experiments M.F.Rivet, B.Gatty, H.Guillemot, B.Borderie, R.Bimbot, I.Forest, J.Galin, D.Gardes, D.Guerreau, M . L e f o r t , X . T a r r a g o , B . T a m a i n , L . N o v i e k i - Z . P h y s . A 307, 365 (1982) Correlations between Fission Fragments and Light Charged-Particles i n t h e R e a c t i o n 2°Ne + *9~Au a t 13 M e V / N u c l e o n J.L.Romero, J.L.Ullmann, F.P.Brady, J.D.Carlson, D.H.Fitzgerald, A.L.Sagle, T.S.Subramanian, C . I . Z a n e l l i , N . S . P . K i n g , M . W . M c N a u g h t o n , B . E . B o n n e r - P h y s . R e v . C25, 2214 (1982) Neutron-Deuteron Analyzing Power Measurements a t 50 MeV. I. 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82Sa21

82Sa22 82Sa24 82Sc02 82Sc03

82Sc05

82Sc07

82Sc08

82Sc09

82Sc12

82Sc13

82Sc14

82Sc15

82Sc17

82Sc18 82Sc21 82SeO1 82Se02

82Se03 82Se04

82Se05 82Se06 82Se07 82Se08

82Se09

D.G.Sarantites, M.Jaaskelainen, R.Woodward, F.A.Dilmanian, D.C.Hensley, J.H.Barker, J.R.Beene, M . L . H a l b e r t , W . T . M i l n e r - P h y s + L e t t . 1158, 4 4 1 (1982) Population of the Entry States in Heavy-Ion Fusion Reactions H . S . S a h o t a - J . P h y s + S o c . J p n . 51, 2 4 0 0 (1982) N a t u r e o f t h e 153 a n d 270 k e V T r a n s i t i o n s i n l l g S b f r o m 119mTe C . S a m a n t a , N . S . C h a n t , P.G.Roos, A . N a d a s e n , A . A . C o w l e y - P h y s . R e v . C26, 1379 (1982) Discrepancy between Protonand Alpha-Induced Cluster Knockout R e a c t i o n s o n 160 B . S c h o c h , H . G o r i n g e r - P h y s . L e t t . 1098, 11 (1982) Excitation o f t h e ( p z / z ) -1 H o l e S t a t e i n t h e 1 6 0 ( 7 , n ) 1 5 0 R e a c t i o n K.Schreckenbach, A.I.Namenson, W.F.Davidson, T.Von Egidy, H.G.Borner, J.A+Pinston, R.K.Smither, D . D . W a r n e r , R . F . C a s t e n , M . L . S t e l t s , D . H . W h i t e , W . 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H o f m e y r , K.P.Lieb - Phys.Rev. C25, 2888 (1982) Levels a n d G a m m a Energies of 28AI Studied b y T h e r m a l N e u t r o n C a p t u r e U.J.Schrewe, E.Hagberg, H . S c h m e i n g , J.C.Hardy, V . T . K o s l o w s k y , K.S.Sharma, E.T.H.Clifford Phys.Rev. C25, 3091 (1982) D e c a y Studies of the N e w Isotopes *62,*SSHf P.Schwandt, H.O.Meyer, W.W.Jacobs, A.D.Bacher, S+E.Vigdor, M . D . K a i t c h u c k , T.R.Donoghue P h y s . R e v + C26, 55 ( 1 9 8 2 ) Analyzing Power of Proton-Nucleus Elastic Scattering b e t w e e n 80 a n d 180 MeV R.Scherwinski, A . A l e v r a , J . F r i e s e , R . L a n g k a u , W . S c o b e l - P h y s . R e v . C26, 113 (1982) Entrance Channel Effects in Nucleon and a Particle Preequilibrium D e c a y o f 63Cu a n d 64Zn P.Schwandt, R . E . B r o w n , F . D . C o r r e l l , R . A . H a r d e k o p f , G . G . O h l s e n - P h y s . R e v . 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A 386, 4 4 7 (1982) S p e c t r o s c o p y o f Two C o i n c i d e n t C h a r g e d P a r t i c l e s E m i t t e d f o l l o w i n g B o u n d P i o n A b s o r p t i o n i n lZC,

59Co and I97Au

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82Sell 82Sg01 82Sh01 82Sh04 82Sh05 82Sh07

82Sh10

82Sh12 82Sh13

82Sh16

82Sh19 82Sh20 82Sh21 82Sh22 82Si01

82Si03 82Si04 82Si05

82Si07 82Si08 82Si10

82Sj01

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82Va07

83Va08 82Va09 82ValO 82Va12 82Va13 82Va16

K.S.Toth, Y.A.Ellis-Akovali, D.M.Moltz, R . L . M l e k o d a j - P h y s . L e t t . I17B, 11 (1982) Low L y i n g 1 + a n d 2 - S t a t e s i n D o u b l y - O d d Terbium,Holmium, and Thulium Nuclei W.Trautmann, J.F.Sharpey-Sehafer, H . R . A n d r e w s , B.Haas, O . H a u s s e r , P . T a r a s , D.Ward - N u c l . P h y s . A 3 7 8 , 141 ( 1 9 8 2 ) M e a s u r e m e n t of t h e L i n e a r P o l a r i z a t i o n of C o n t i n u u m G a m m a R a y s f r o m (32S,xn) R e a c t i o n s to P r o l a t e and Oblate Rare-Earth Nuclei H.Tricoire, C.Gerschel, N.Perin, H.Sergolle, L.Valentin, D.Bachelier, H.Doubre, J.Gizon Z . P h y s . A 3 0 6 , 127 ( 1 9 8 2 ) Direct a Particle Emission in Incomplete Fusion Reaction on a Spherical T a r g e t lZ4Sn V.G.Tsinoev, Yu.P.Chertov, S.G.Danengirsh, Yu.l.Shcherbina, E.P.Stepanov, A.A.Voronin P h y s . L e t t . l l 0 B , 369 (1982) Mossbauer Test of T-Invariance i n ~gVAu Tsan Ung Chan, M.Agard, J.F.Bruandet, B.Chambon, A.Dauchy, D.Drain, A.Giorni, F.Glasser, C . M o r a n d - P h y s . R e v . C26, 4 2 4 (1982) High-Spin S t a t e s i n 6°Cu J.L.Ullmann, F.P.Brady, D.H.Fitzgerald, G.A.Needham, J.L.Romero, C.M.Castaneda, N.S.P.King N u c l . P h y s . A386, 179 (1982) Analog Giant Dipole Excitation i n S i ( n , p ) a t 59.6 MeV W.Urban, T.Rzaea, Ch.Droste, L.Goettig, T.Morek, J.Srebrny - Z . P h y s . A305, 335 (1982) T h e D e c a y o f 13°La t o L e v e l s i n 13°Ba W.T.H.van Oers, B.T.Murdoch, B.K.S.Koene, D.K.Hasell, R.AbeRg, D.J.Margaziotis, M.B.Epstein, G.A.Moss, L . G . G r e e n i a u s , J.M.Greben, J.M.Cameron, J.G.Rogers, A.W.Stetz Phys.Rev. C25, 390 (1982) 4He(p,2p)3H Reaction at Intermediate Energies C.J.Van Der Poel, G.A.P.Engelbertink, H.J.M.Aarts, D.E.C.Scherpenzeel, H.F.R.Arciszewski, B . C . M e t s c h - N u e l . P h y s . A373, 81 (1982) High-Spin S t a t e s i n 34C1 R.Vaninbroukx, B.Denecke - Nucl.Instrum.Methods 193, 191 (1982) Determination of Gamma-Ray Emission Probabilities i n t h e D e c a y o f 235U a n d 231Th L.T.van der Bijl, H.P.Blok, R.Frey, D.Meuer, A.Richter, P.K.A.de W i t t H u b e r t s - Z . P h y s . A305, 231 ( 1 9 8 2 ) Quenching of the Electron Scattering F o r m F a c t o r o f t h e 1 + S t a t e a t 3 . 4 8 MeV i n SSSr a n d t h e Influence of the A(1232)-Isobar P . V a n Nes, W . H . A . H e s s e l i n k , W . H . D i c k h o f f , J . J . V a n R u y v e n , M.J.A.DeVoigt, H.Verheul - Nucl.Phys. A379, 35 (1982) A Neutron Decoupled from a R o t a t i n g O dd C o r e i n 114Sb a n d l l 6 S b A . M . V a n D e n B e r g , R . V . F . J a n s s e n s , G . T . E m e r y , A . S a h a , R . H . S i e m s s e n - N u c l . P h y s . A 379 , 2 3 9 (1982) First Excited 0 + States in the Germanium Isotopes Via the Se(d,6Li) Reaction J . R . V a n H i s e , D . E . M a r t z , R . A . J a c k s o n , D . Y . K u n i h i r a , E . B o l t o n - P h y s . R e v . C25, 2 8 0 2 ( 1 9 8 2 ) 218po H a l f - L i f e J.J.Van Ruyven, W.H.A.Hesselink, J.Akkermans, P . V a n Nes, H . V e r h e u l - N u c l . P h y s . A380, 125 (1982) Band Structures i n li8,1a°Te M.Varnagy, J.Csikai - Nucl.Instrum.Methods 196, 4 6 5 (1982) A New A p p r o a c h to Measuring Fission Cross-Section Ratios C.Van Der Leun, C.Alderliesten - N u c l . P h y s . A 380, 261 (1982) The Deuteron Binding Energy S.S.Vasilev, M.S.Golovkov, T.N.Mikhaleva, D.L.Chuprunov - Izv.Akad.Nauk SEER, S e r . F i z . 46, 9 4 0

(1982) 82Va17

82Va20 82Va21

82Ve03

82Ve04 82Ve05

Spin and Parity of Resonant S t a t e s i n a4Mg E x c i t e d i n t h e R e a c t i o n s a a N a ( p , a ) 2 ° N e a n d 23Na(p, p')23Na a t E ( p ) = 6 . 2 7 , 6 . 3 7 a n d 6.52 MeV G.V.Valsky, T.K.Zvezdkina, D.V.Nikolaev, V.I.Petrova, G.A.Petrov, A.K.Petukhov, Yu.S.Pleva, V.A.Tyukavin - Y a d . F i z . 36, 4 4 (1982) E n e r g y D e p e n d e n c e of t h e S p a c e - P a r i t y Violating Asymmetry in the Fragment Emission from Fission o f a39Pu I n d u c e d by Slow Polarized Neutrons C . W . E . v a n E i j k , J . P . W a g e n a a r , F . B e r g s m a , W . L o u r e n s - P h y s . R e v . A26, 2 7 4 9 (1982) Double K-Shell-Vacancy Production i n t h e D e c a y s o f 181W a n d 16SEr D.Vandeplassche, E.van Walle, C.Nuytten, L.Vanneste - Phys.Rev.Lett. 49, 1390 (1982) On-Line Nuclear-Orientation S t u d i e s o f S p i n s a n d M a g n e t i c M o m e n t s of N e u t r o n - D e f i c i e n t Indium Isotopes G.N.Veliehko, A.A.Vorobyev, Yu.K.Zalite, G.A.Korolev, E.M.Maev, N.K.Terentev, Y.Terien, A.V.Khanzadeev - Y a d . F i z . 35, 270 (1982) Small-Angle E l a s t i c p4He S c a t t e r i n g a t t h e E n e r g y o f 992 MeV W.J.Vermeer, A.R.Poletti - J.Phys.(London) GS, 7 4 3 ( 1 9 8 2 ) ]Determination of Partial D e c a y W i d t h s f o r t h e 2 - , 8 . 8 7 MeV L e v e l i n 160 W.J.Vermeer, A.R.Poletti - J.Phys.(London) G8, 851 (1983) Branching Ratio for the Isoscalar Transition 2+,T=1,1.95 MeV ~ 0+,T=1,0.66 MeV i n aaNa

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82Ve09 82VelO

82Vi02

82Vi05

82Vo03 82Vo04 82Vo05

82Vy02

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Linear M o m e n t u m Transfer in Nonrelativistic N u c l e u s - N u c l e u s Collisions S.E.Vigdor, H.J.Karwowski, W.W.Jacobs, S.Kailas, P.P.Singh, F.Soga, T . G . T h r o w e - Phys.Rev. C26, 1035 (1982) Decay of H o t , H i g h - S p i n Nuclei P r o d u c e d in S L i - i n d u c e d Fusion Reactions S.E.Vigdor, T . G . T h r o w e , M.C.Green, W.W.Jacobs, R.D.Bent, J.J.Kehayias, W.K.Pitts, T.E.Ward Phys.Rev.Lett. 49, 1314 (1982) Dominance of H i g h - S p i n T w o - P a r t i c l e , O n e - H o l e Transitions in (p,~r-) Reactions W . v o n Oertzen, M.Bernas, F.Pougheon, P.Roussel - Phys.Lett. II5B, 184 (1982) Inelastic Scattering of 12C a n d 13C on S3Cu Leading to Core-Excited States W . V o n Oertzen - Nucl.Phys. A387, 93c (1982) Direct Processes in H e a v y Ion Collisions at E -< 20 M e V / u B.B.Voitsekhovsky, D.M.Nikolenko, S.G.Popov, V.N.Rotaev, D.K.Toporkov, E.P.Tsentalovich - P i s m a Zh.Eksp.Teor.Fiz. 35, 299; J E T P Lett.(USSR) 35, 371 (1982) Electroexcitation of the Nucleus 'SO with Coincidence Detection of the Electron a n d the Secondary Particles. Ts.Vylov, V . M . G o r o z h a n k i n , K . Y a . G r o m o v , V.G.Kalinnikov, T.Kretsu, V . V . K u z n e t s o v - I z v . A k a d . N a u k SSSR, S e r . F i z . 46, 16 (1982) S t u d y of t h e D i s i n t e g r a t i o n 159No - lSgDy Ts.Vylov, V.M.Gorozhankin, K.Ya.Gromov, V.V.Kuznetsov - Izv.Akad.Nauk SSSR, S e r . F i z . 46, 8 3 4

(1982) 82WaOl 82WaO2 82WaO3 82WaO5 82Wa08 82Wa0 9

82Wa10 82Wa12 82Wa14

82Wa15 82Wa16 82Wa17

S t u d y o f t h e l e S T m -. leSEr D e c a y O . A . W a s s o n , A . D . C a r l s o n , K . C . D u v a l l - N u c l . S c i . E n g . 80, 282 (1982) Measurement o f t h e a3SU N e u t r o n - I n d u c e d F i s s i o n C r o s s S e c t i o n a t 14.1 MeV T.E.Ward, C.C.Foster, G.E.Walker, J.Rapaport, C . A . G o u l d i n g - P h y s . R e v . C25, 762 (1982) 1/E Dependence o f t h e 7 L i ( p , n ) T B e ( g . s . + 0 . 4 3 MeV) T o t a l R e a c t i o n C r o s s S e c t i o n S.Wald, I.Tserruya, Z.Fraenkel, G.Doukellis, H.Gemmeke, H . L . H a r n e y - P h y s . R e v . C25, 1118 ( 1 9 8 2 ) Neutron,Proton,and A l p h a E m i s s i o n i n D e e p I n e l a s t i c C o l l i s i o n s o f lSO o n 4SCa a t 14 2 MeV E.K.Warburton, D . E . A l b u r g e r , J . W . O l n e s s - N u c l . P h y s . A 378, 397 (1982) B e t a D e c a y o f asp O . A . W a s s o n , M . M . M e i e r , K . C . D u v a l l - N u c l . S c i . E n g . 81, 196 (1982) Absolute Measurement of the Uranium-235 F i s s i o n C r o s s S e c t i o n f r o m 0.2 t o 1.2 MeV J.W.Watson, R.Garrett, F.P.Brady, D.H.Fitzgerald, J.L.Romero, J.L.Ullmann, C.I.Zanelli P h y s . R e v . C25, 2219 (1982) Neutron-Deuteron Analyzing Power Measurements a t 50 MeV. II. Forward Angles E . W a r d e , R . S e l t z , D . M a g n a c , H . L . S h a r m a - P h y s . R e v . C25, 2 3 5 3 (1982) lalTa(p,t)lVgTa Reaction: Evidence for particle-core coupling P.H.Wallace, H.J.Hausman, J . N . M c K a m y , H . R . S u i t e r - P h y s . R e v . C26, 107 ( 1 9 8 2 ) Proton Partial Decay Widths from the Intermediate Structure i n 41Sc C.Wasilevsky, R.Montenegro, M. d e l a V e g a V e d o y a , S . J . N a s s i f f - R a d i o c h e m . R a d i o a n a l . L e t t . 50, 307 (1982) Cross-Sections a n d I s o m e r i c R a t i o s f o r t h e I s o m e r i c P a i r 133mxe/133gXe F o r m e d i n the 13°Te(fx,n) Reaction W.H.Warren, W.L.Alford - Ann.Nucl.Energy 9, 369 (1982) C r o s s S e c t i o n s f o r 5 1 V ( n , p ) S t T i a n d 5 1 V ( n , a ) 4 S S c a t 14.2 MeV E.K.Warburton, D . E : A l b u r g e r - N u c l . P h y s . A 385, 189 (1982) E n e r g y o f t h e 14N F i r s t - E x c i t e d S t a t e a n d t h e 140 0 + ~ 14N 0 + f t V a l u e J.W.Watson, M.Ahmad, D.W.Devins, B.S.Flanders, D.L.Friesel, N.S.Chant, P.G.Roos, J.Wastell P h y s . R e v . C26, 961 (1982) 4°Ca(p,pn)agCa and 48Ca(p,pn)4~Ca Neutron Knockout R e a c t i o n s a t 149.5 MeV

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82ZuO1

82Zu02 82Zu03 82ZwO1

L . Z e m l o , W . D r e n c k h a h n , A.Feigel, E . F i n c k h , K . R u s k a m p , P . U r b a i n s k y , M . W a n g l e r - N u c l . P h y s . A380, 493 (1982) T h e Z°gBi(d,3')211,211mpo R e a c t i o n A.Zemel, C.Broude, E.Dafni, A.Gelberg, M.B.Goldberg, J.Gerber, G.J.Kumbartzki, K.-H.Speidel N u c l . P h y s . A383, 165 (1982) M a g n e t i c M o m e n t s a t B a c k b e n d i n g a n d S p e c t r o s c o p y o f 134Ce U.Zurmuhl, P.Rullhusen, F.Smend, M.Schumacher, H . G . B o r n e r - P h y s . L e t t . I I 4 B , 99 (1982) T h e D i s t r i b u t i o n of E1 S t r e n g t h b e l o w P a r t i c l e T h r e s h o l d S t u d i e d b y R e s o n a n t S c a t t e r i n g o f G a m m a Rays J . D . Z u m b r o , C . P . B r o w n e , J . F . M a t e j a , H . T . F o r t u n e , R . M i d d l e t o n - P h y s . R e v . C26, 965 (1982) 176Yb(t,p)178Yb R e a c t i o n B . W . Z u l k o s k e y , R . M . S e a l o c k , H . S . C a p l a n , J . C . B e r g s t r o m - P h y s . R e v . C26, 1610 (1982) Electroproduction o f ~r+ f r o m S°B a n d I t s R e l a t i o n to E l e c t r o n S c a t t e r i n g F . Z w a r t s , K . v a n d e r Borg, A . G . D r e n t j e , M . N . H a r a k e h , W . A . S t e r r e n b u r g , A . v a n d e r W o u d e - P h y s . R e v .

C25, 2139 (1982)

82Zw02

O r i g i n of t h e F o r w a r d - B a c k w a r d A s y m m e t r y in t h e Decay o f t h e G i a n t R e s o n a n c e S t r u c t u r e s a n d 4°Ca B . Z w i e g l i n s k i , W . B e n e n s o n , G . M . C r a w l e y , S.Gales, D . W e b e r - N u c l . P h y s . A389, 301 (1982) S t u d y o f lib a t H i g h E x c i t a t i o n s w i t h t h e 9Be(3He,p)llB a n d 9Be(c~,d)tlB R e a c t i o n s

202

of

24Mg

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 1n

J

B1GrZX:

R

81KaZT: 82FiZV: 82KrZZ 82RoZW

J

82GeZZ

R

82AaZY 82GuZX 82KrZZ:

J

82GeZZ

R

82AaZX 82StZZ

R 81CIZY

5Li

R 8IC1ZY

R 81RoZT

6Li

R 80BiZU

6Be

R 81NeZY:

R 81DiZT:

81PeZT:

=

4

=

5

=

6

NUCLEAR REACTIONS 6 L i , l Z C , a s S i ( n , p ) , E = 6 0 MeV; m e a s u r e d ate=0°); deduced effective interaction p r o p e r t i e s . 6He,laB,aSA1 d e d u c e d g i a n t m a g n e t i c d i p o l e a n a l o g s . BAPSA 26 1128, BE5,Romero. NUCLEAR REACTIONS 3He(p,rr+),E=180-190,301 MeV; aHe(3He,~+),E=270,283 MeV; m e a s u r e d at0), a(E(~r)). 6Li d e d u c e d s t r o n g e x c i t a t i o n probability. REPT IPN 1980 A n n u a l , P N 5 7 , B i m b o t . NUCLEAR REACTIONS 6,TLi,SBe?aC,14N,laO,19F,a?Al(n,p),(n,d),E=60 MeV; m e a s u r e d ~(Ep),cr(O); deduced reaction mechanism. 6,TBe,aB d e d u c e d GDR f r a g m e n t a t i o n . DWBA a n a l y s i s , Goldhaber-Teller f o r m f a c t o r . DABBB 43 1 0 6 8 , N e e d h a m .

A VLi

3

NUCLEAR REACTIONS 3 H ( p o l a r i z e d d , n ) , 3 H e ( p o l a r i z e d d , p ) , E = 3 - 6 MeV; m e a s u r e d o ( O ) , v e e t o r , t e n s o r a n a l y z i n g p o w e r s . 5He,SLi d e d u c e d l e v e l s t r u c t u r e . DABBB 42 6 7 3 , C l a r k . NUCLEAR REACTIONS 3 H ( p o l a r i z e d d , n ) , 3 H e ( p o l a r i z e d d , p ) , E = 3 - 6 MeV; m e a s u r e d (z(0),vector, t e n s o r a n a l y z i n g p o w e r s . 5He,SLi d e d u e e d l e v e l s t r u c t u r e . DABBB 42 6 7 3 , C l a r k .

A

6He

=

NUCLEAR MOMENTS 3,drier m e a s u r e d hfs,fine structure. High resolution cw d y e l a s e r s p e c t r o s c o p y . BAPSA 27 4 4 , K E 1 0 , G e r h a r d t . NUCLEAR REACTIONS ~ S S i ( a , 3 H e ) , E = 6 5 MeV; m e a s u r e d cr(0,E(3He)); d e d u c e d breakup ( Q ) - d e p e n d e n c e . 4He d e d u c e d s m a l l d i r e c t b r e a k u p e f f e c t s . REPT KVI 1981 A n n , P 3 3 , A a r t s . NUCLEAR REACTIONS 4He(e,e),E n o t given; m e a s u r e d or. 4He deduced r m s charge radius. BAPSA 27 5 2 9 , G E 6 , S t a p o r .

A

5He

2

NUCLEAR MOMENTS 3,drier m e a s u r e d hfs,fine structure. High resolution cw d y e l a s e r s p e c t r o s c o p y . BAPSA 27 4 4 , K E t 0 , G e r h a r d t . NUCLEAR REACTIONS aSSi(3He,2p),E=52 MeV; m e a s u r e d a(Ei,E2,01,0a),totaI k i n e t i c e n e r g y . 3He deduced breakup p r o c e s s . REPT KVI 1981 A n n , P 3 1 , A a r t s . NUCLEAR REACTIONS 3 H e ( p , 2 p ) , E = 2 5 0 , 4 0 0 MeV; m e a s u r e d r e c o i l s y s t e m t o t a l e n e r g y . 3He deduced two-nucleon c o r r e l a t i o n s . P W I A , F a d d e e v c a l c u l a t i o n s . BAPSA 27 5 6 9 , K E 3 , G u b l e r . NUCLEAR REACTIONS 2H,3He(p,p),E n o t g i v e n ; m e a s u r e d p n - e o i n , aH,3He d e d u c e d n e u t r o n momentum distribution. Nonsymmetrical g e o m e t r y . DABBB 42 4 1 0 3 , K r e b s .

A

4He

=

NUCLEAR REACTIONS a°aPb,a°SBi,lSTAu(polarized d,d),E=5 MeV; m e a s u r e d T20(0). 2H d e d u c e d quadrupole moment. BAPSA 26 l l l 4 , A C 6 , K a m m e r a a d . NUCLEAR REACTIONS S i ( d , p n ) , E = l T . 8 MeV; m e a s u r e d pn-coin,total kinetic energy distribution. ~H d e d u c e d b r e a k u p m o d e s . BAPSA 27 5 6 1 , H X a 1 0 , F i e l d s . NUCLEAR REACTIONS 2H,3He(p,p),E n o t g i v e n ; m e a s u r e d p n - c o i n . 2H,3He d e d u c e d n e u t r o n momentum distribution. Nonsymmetrieal g e o m e t r y . DABBB 42 4 1 9 3 , K r e b s . NUCLEAR REACTIONS 2 ° s P b ( d , d ) , E = 3 . 5 - 7 MeV; m e a s u r e d cr(0,E); d e d u c e d d e v i a t i o n from Rutherford s c a t t e r i n g . ZH d e d u c e d e l e c t r o n p o l a r i z a b i l i t y . BAPSA 27 5 6 9 , K E 8 , R o d n i n g .

A

3He

I

NUCLEAR MOMENTS in; m e a s u r e d /z. Magnetic r e s o n a n c e s p e c t r o m e t e r , i m p r o v e d accuracy. REPT CON F - 8 1 0 6 9 5 - 1 , G r e e n e .

A

eH

=

ONLY)

=

7

NUCLEAR REACTIONS 7 L i ( a , a ) , ( a , a ' ) , E = 3 5 . 3 MeV; m e a s u r e d a(EcU),cr(O). 7Li l e v e l s d e d u c e d deformation parameter fla- O p t i c a l m o d e l , D W B A , c o u p t e d - c h a n n e l s a n a l y s e s . REPT D O E / E R / 40014-3,P29,Dickey. NUCLEAR REACTIONS 7 L i ( T r + , T r + ) , ( ~ + , ~ r + ' ) , ( ~ r - , ~ - ) , ( ~ - , T r - ' ) , E = 1 4 3 MeV; m e a s u r e d cr(0(Tr)), cr(E(Tr')). 7Li l e v e l s d e d u c e d d e f o r m a t i o n p a r a m e t e r s . DWBA a n a l y s i s . REPT L A - 8 7 6 8 - P R , P 3 2 , Peterson.

203

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 7Li

R 82CoZU: 8RFiZY

?Be

R 81NeZY

R 80RaZK 80NeZU 81BeZJ 81HeZT:

8B

R 80WiZM:

D 80DeZF:

9Be

D 80DeZF:

R 79BuZD: ~E

R 81NeZY:

D 80DeZF:

Io B

R 80MAZE: 80RaZK: 80WeZU: 81AbZX:

D 80DeZF:

JIBe

D 80DeZF:

R 82MiZT:

8

=

9

=

i0

R A D I O A C T I V I T Y 9,11Li [ f r o m on-line mass spectroscopy]; measured Efl,Ifl,fl-delayed (partiele)(particle)-coin. i°,l~Be d e d u c e d new decay modes. 9,'1Be l e v e l s deduced fl-branching. Tof,two-dimensional e n e r g y s p e c t r a . REPT IPN 1980 A n n u a l , P N 2 8 , D e t r a z . NUCLEAR REACTIONS ' S o , i Z c , a 4 S ( p o l a r i z e d d , a ) , E = 5 ~ MeV; m e a s u r e d iTlt(0 ). i°B,a2P,16N l e v e l s deduced L,J,Tr,stretched configuration. DWBA a n a l y s i s . REPT K f K - 3 0 6 8 , P 2 9 , M a i r l e . NUCLEAR REACTIONS 9Be,lO,'lB,la,laC,14N(p,aHe),E=41,45 MeV; m e a s u r e d a ( 8 ) . . SBe,l°,llB,12C l e v e l s d e d u c e d S. L e g e n d r e p o l y n o m i a l , D W B A a n a l y s e s . REPT J U L - S p e z - 7 2 , P l l , R a p p . NUCLEAR REACTIONS SBe,l°B,13C,14N(p,a),E=22.5-45 MeV; 11B,laC(p,a),E=41,45 MeV; m e a s u r e d a(O). l°B,llC,SBe l e v e l s d e d u c e d L , t r a n s f e r - j . A E - E t e l e s c o p e . REPT J U L - S p e z - 7 2 , P l ~ , W e n g . NUCLEAR REACTIONS lac(p,a),E=22.5-45 MeV; m e a s u r e d (T(0); d e d u c e d r e a c t i o n m e c h a n i s m , l°B levels deduced spectroscopic strengths. REPT J U L - S p e z - 9 9 , P 1 6 , A b d e l Kariem.

A '~Li

=

R A D I O A C T I V I T Y 9,11Li [ f r o m on-line mass spectroscopy]; measured Efl,Ifl,fl-delayed (particle)(particle)-coin. i°,llBe deduced new decay modes. 9,11Be l e v e l s deduced fl-branching. Tof,two-dimensional e n e r g y s p e c t r a . REPT IPN 1980 A n n u a l , P N 2 8 , D e t r a z . R A D I O A C T I V I T Y 9,ULi [ f r o m on-line mass spectroscopy]; measured Efl,Ifl,fl-delayed (particle)(particle)-coin. l°,l'Be deduced new decay modes. 9,HBe levels deduced fl-branching. Tof,two-dimensional e n e r g y s p e c t r a . REPT IPN 1980 A n n u a l , P N 2 8 , D e t r a z . NUCLEAR REACTIONS 9Be(e,e'),E n o t g i v e n ; m e a s u r e d a ( E , 0 ) ; d e d u c e d f o r m f a c t o r s . 9Be deduced resonances,widths. CONF R i g a , P 5 9 9 , B u k i . NUCLEAR REACTIONS 6,?Li,gBe,laC,14N,160,19F,aTAl(n,p),(n,d),E=60 MeV; m e a s u r e d a(Ep),(r(0); deduced reaction mechanism. 6,?Be,gB d e d u c e d GDR f r a g m e n t a t i o n . DWBA a n a l y s i s , Goldhaber-Teller f o r m f a c t o r . DABBB 42 1 0 6 8 , N e e d h a m .

A ~OBe

continued

NUCLEAR REACTIONS 9 B e , l ° , U B , ' 2 , 1 a c , 1 4 N ( p , a H e ) , E = 4 1 , 4 5 MeV; m e a s u r e d a ( 0 ) . aBe,I°,I1B,t2c l e v e l s d e d u c e d S. L e g e n d r e p o l y n o m i a l , D W B A a n a l y s e s . REPT J U L - S p e z - 7 2 , P l l , R a p p . NUCLEAR REACTIONS 9 B e , l ° H , l a C , 1 4 N ( p , a ) , E = 2 2 . 5 - 4 5 MeV; itB,12C(p,a),E=41,45 MeV; m e a s u r e d a ( 0 ) . l°B,llC,eBe l e v e l s d e d u c e d L , t r a n s f e r - j . A E - E t e l e s c o p e . REPT J U L - S p e z - 7 2 , P 1 2 , W e n g . NUCLEAR REACTIONS 9Be(p,d),E=14.3,26.E MeV; m e a s u r e d a(0); d e d u c e d n a t u r e o f a n o m a l y . SEe levels deduced F,neutron spectroscopic f a c t o r s . B A P S A 26 l l l 5 , A C 1 4 , B e c c h e t t i . NUCLEAR REACTIONS mO(Tr+,p),E=66 MeV; 9Be(Tr+,p),E=50 MeV; m e a s u r e d a(0); d e d u c e d a n g u l a r momentum mismatch e f f e c t . 1So,aBe d e d u c e d h i g h - s p i n state selective excitation. One-, two-nucleon m o d e l s . REPT l P N O - T - 8 1 - 0 1 , H e n n i n o . NUCLEAR REACTIONS 6Li,gBe,19B(d,~-),E=600 MeV; % i ( d j r - ) , E = 3 0 0 MeV; m e a s u r e d a(0) v s p i o n momentum, eB l e v e l s d e d u c e d a ( 0 ) . REPT IPN 1980 A n n u a l , P N 5 9 , W i l l i s .

A 9Li

7

NUCLEAR REACTIONS 6 L i ( n , t ) , E = 0 . 2 - 3 MeV; aH(a,SLi),E=ll.5-16.7 MeV; m e a s u r e d a(0). aH(~,a), E = 1 1 . 5 - 1 7 MeV; m e a s u r e d a ( 0 ) . 7Li d e d u c e d r e s o n a n c e s . REPT N E A N D C ( O R ) - 1 5 7 / U , P 3 0 , C o n d e . NUCLEAR REACTIONS ' Z ° S n ( p o l a r i z e d VLi,?Li'),E n o t g i v e n ; m e a s u r e d t e n s o r a n a l y z i n g p o w e r . ~Li d e d u c e d e l e c t r i c q u a d r u p o l e moment. Coulomb scattering,semiclassical approximation. B A P S A 27 4 9 2 , D X a T , F i c k . NUCLEAR REACTIONS 6,TLi,gBe,leC,14N,160,19F,eTAl(n,p),(n,d),E=60 MeV; m e a s u r e d a(Ep),a(0); deduced reaction mechanism. 6,TBe,gB d e d u c e d GDR f r a g m e n t a t i o n . DWBA a n a l y s i s , Goldhaber-Teller f o r m f a c t o r . DABBB 42 1 0 6 8 , N e e d h a m .

A eBe

=

ONLY)

--- I I

R A D I O A C T I V I T Y 9,11Li [ f r o m on-line mass spectroscopy]; measured Efl,Ifl,fl-delayed (partiele)(particle)-coin. l°,l~Be d e d u c e d new decay modes. 9,JiBe l e v e l s deduced fl-branching. Tof,two-dimensional e n e r g y s p e c t r a . REPT IPN 1980 A n n u a l , P N 2 8 , D e t r a z . R A D I O A C T I V I T Y 9,11Li [ f r o m on-line mass spectroscopy]; measured Efl,lfl,fl-delayed (particle)(partic/e)-coin. io,11Be d e d u c e d new decay modes. 9,11Be l e v e l s deduced fl-branching. Tof,two-dimensional e n e r g y s p e c t r a . REPT IPN 1980 A n n u a l , P N 2 8 , D e t r a z . NUCLEAR REACTIONS 9Be(t,pT),aH(gBe,p-y),E n o t g i v e n ; m e a s u r e d DSA. 11Be l e v e l d e d u c e d T1/a. S h e l l m o d e l . B A P S A 27 6 9 6 , A C 1 , M i l l e n e r .

204

SECONDARY SOURCES ( R e p o r t s , A b s t r a c t s , e t c .

A ii B

R 80RaZK: 81MoZP: 82RaZU: 82ZeZZ:

H C

R 80WeZU: 82McZZ: 82WiZZ:

D 82PrZZ: R 81RoZT:

82KoZU: ~C

R 79BaXX: 79FeZZ: 79PaZO:

80BuZF: 80DjZX: 80RaZK: 81BaZQ:

81BiZX: 81FoZV: 811gZX: 81KaZS: 81KeZY:

81PeZO: 82HaZT:

82NeZY: 82PaZT: 82RaZP: 82ReZZ:

Ii

continued

NUCLEAR REACTIONS 9Be,19,11B,la,~ac,i*N(p,aHe),E=41,45 MeV; m e a s u r e d ~(0). 8Be,*°,l:B,laC l e v e l s d e d u c e d S. L e g e n d r e p o l y n o m i a l , D W B A a n a l y s e s . REPT J U L - S p e z - 7 2 , P l l , R a p p . NUCLEAR REACTIONS l°,liB,laN(rr+,rr+'),(Tr-,Tr-'),E=162 MeV; m e a s u r e d a ( E ( r r ) ) . ~4N d e d u c e d l e v e l , J , r r . '~B l e v e l s d e d u c e d l a r g e r r + / r r - d i f f e r e n c e s . REPT L A - 8 7 6 8 - P R , P 3 1 , M o r r i s o n . NUCLEAR REACTIONS 'ac,15N,160(p,aHe),E=45 MeV; m e a s u r e d a(O). uB l e v e l s d e d u e e d S. DWBA a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 2 3 , R a p p . NUCLEAR REACTIONS i°,'iB(Tr+,Tr+),(~r+,zr+'),(rr-,zr-),(?r-,rr-'),E=162 MeV; m e a s u r e d ~(E(rr)),o'(O). ~B levels deduced ~(~r-)/cr(rr+). REPT ANL-81-79,P16,Zeidman. NUCLEAR REACTIONS ~Be,~°B,lac,14N(p,(x),E=22.5-45 MeV; lIB,teC(p,a),E=41,45 MeV; measured ~r(0). ~°B,lIc,SBe levels deduced L , t r a n s f e r - j . AE-E telescope. REPT JUL-Spez-72,P12,Weng. NUCLEAR REACTIONS 9Be(3He,nv),E=2.5 MeV; measured nv-coin, tiC level deduced negligible F% Tof,NE-224 detector. BAPSA 27 561,HXall,McKamy. NUCLEAR REACTIONS mB(p,T),E=0.3-2 MeV; measured a(Ev),T(0). UC deduced resonance. BAPSA 27 460,AYa9,Wiescher.

A ~2B

=

ONLY)

=

12

RADIOACTIVITY lZB [ f r o m i l B ( d , p ) ] ; m e a s u r e d I f l ( 0 ) , o r i e n t e d n u c l e i ; d e d u c e d a s y m m e t r y coefficient. Second class current s e a r c h . BAPSA 27 4 9 1 , D X a l , P r o n k o . NUCLEAR REACTIONS 6Li,12C,asSi(n,p),E=60 MeV; m e a s u r e d or(0=0°); d e d u c e d effective i n t e r a c t i o n p r o p e r t i e s . 6He,12B,2SA1 d e d u c e d g i a n t m a g n e t i c d i p o l e a n a l o g s . BAPSA 26 1138, BE5,Romero. NUCLEAR REACTIONS l l B ( n , n ) , ( n , n ' ) , E = 4 . 8 - 7 . 6 MeV; m e a s u r e d a ( 0 ) v s E. leB d e d u c e d resonances,J,rr,redueed widths. R-matrix,shell m o d e l a n a l y s e s . BAPSA 27 6 9 6 , A C 2 , K o e h l e r . NUCLEAR REACTIONS ~aC(e,e),E=25-85 MeV; m e a s u r e d ~. laC d e d u c e d c h a r g e r m s r a d i u s . Model-independent m e t h o d . CONF R i g a , P 2 8 2 , B a t y u n i n . NUCLEAR REACTIONS 12C(a,a'),E=23.9,24.2 MeV,1~C(a,a'),E=22.6-24.2 MeV; m e a s u r e d a(E). IaC level deduced polarization v s (0). S i - L i d e t e c t o r s . CONF R i g a , P 3 3 8 , F e o f i l o v . NUCLEAR REACTIONS l a C , 5 4 , 5 6 , 5 S F e , 5 e , 6 ° , 6 a N i , 6 4 , 6 6 , 6 8 , ~ ° Z n ( a , a ) , ( ( ~ , a ' ) , E = 2 9 , 4 0 , 4 5 , 5 0 MeV; measured a(E,0). 12C,54,se,°SFe,SS,6°,62Ni,64,66,6s,T°Zn d e d u c e d deformation parameter BB l a i r p h a s e m e t h o d . CONF R i g a , P 3 3 0 , P a v l o v a . NUCLEAR REACTIONS lZc(aHe,aHe'),E=108.5 MeV; leC(p,p'),E=57.5 MeV; m e a s u r e d (~(O),g(E(aHe)), a ( E p ) . 12C d e d u c e d g i a n t m o n o p o l e r e s o n a n e e , E W S R . REPT ISN 8 0 - 0 1 , P 4 1 , B u e n e r d . NUCLEAR REACTIONS laC(p,p'),E=201 MeV; 12C(d,d'),E=108 MeV; leC(a,a'),E=218 MeV; m e a s u r e d ~ ( E p ' ) , a ( E d ' ) , c r ( E a ' ) . laC d e d u c e d l e v e l s , J j r , T , P . REPT IPN 1980 A n n u a l , P N 7 , D j a l a l i . NUCLEAR REACTIONS 9Be,l°,llB,lz,lac,14N(p,3He),E=41,45 MeV; m e a s u r e d or(0). SBe,I°,I1B,IzC l e v e l s d e d u c e d S. L e g e n d r e p o l y n o m i a l , D W B A a n a l y s e s . REPT J U L - S p e z - 7 2 , P l l , R a p p . NUCLEAR REACTIONS 1,ZH,lzC,d°Ca(p,p'),E=800 MeV; m e a s u r e d a ( 0 p ' ) v s p r o t o n m o m e n t u m ; deduced quasielastic processes. I~C,49Ca d e d u c e d ff(quasielastic),a(reaetion). REPT L A - 8 7 6 8 - P R , P 2 4 , B a r l e t t. NUCLEAR REACTIONS a°spb(laC,3a),E=132-230 MeV; m e a s u r e d a a ~ - , a a - c o i n , lZC d e d u c e d (~ f o r sequential d e c a y . BAPSA 26 lldl,BB1,Bice. NUCLEAR REACTIONS JeC(rr+,rr+'),(rr-,rr-'),E n o t g i v e n ; m e a s u r e d or(0). IUC d e d u c e d l e v e l s , i s o s c a l a r GDR c o m p o n e n t . BAPSA 26 l 1 2 4 , B C 1 0 , F o r t u n e . NUCLEAR REACTIONS l a C ( p , p ' ) , E = 8 0 0 MeV; m e a s u r e d G(Ep'),c*(0). lac l e v e l d e d u c e d no critical opalescence,precursor e f f e c t s . REPT L A - 8 7 6 8 - P R , P 2 8 , I g o . NUCLEAR REACTIONS mB(aHe,p),nB(aHe,d),E=19 MeV; 14N(d,a),E=18 MeV; m e a s u r e d p a - c o i n . 12C resonances deduced decay characteristics. BAPSA 26 l l l 5 , A C 9 , K a r p . NUCLEAR REACTIONS 9Be,laC(6Li,t),E=30,34,38 MeV; m e a s u r e d cr(Et),a(0). 12C l e v e l s d e d u c e d low population probability. 160 l e v e l s d e d u c e d L,tentative J,rr. BAPSA 26 1115,AC10, Kemper. NUCLEAR REACTIONS lZC(a,a'),E n o t g i v e n ; m e a s u r e d a ( 0 ) . laC l e v e l s d e d u c e d e x c i t a t i o n mechanism,K. Coupled-channels a n a l y s i s . REPT D O E / E R / 4 0 0 1 4 - 3 , P 2 5 , P e t e r s o n . NUCLEAR REACTIONS 15N,16,17,180(p,a),E=45 MeV; m e a s u r e d o'(0); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 13N,12C l e v e l s d e d u c e d j - t r a n s f e r . Zero-range DWBA,microscopic form factors. REPT J U L - S p e z - 1 4 6 , P 2 7 , H a u s e r . NUCLEAR REACTIONS llB,27Al(d,n),E=10,12 MeV; m e a s u r e d or(0). 12C d e d u c e d l e v e l s , p o s s i b l e J, ~ r , c o n f i g u r a t i o n . T o f . DWBA a n a l y s i s . BAPSA 27 5 6 1 , H X a 1 3 , N e u s c h a e f e r . NUCLEAR REACTIONS l ~ C ( e , e ' v ) , E = 6 7 MeV; m e a s u r e d y(O),e'~-coin. ~C level deduced transverse,longitudinal interference amplitudes. BAPSA 27 7 1 9 , D C 3 , P a p a n i c o l a s . NUCLEAR REACTIONS 9Be(c~,n),E=0.51-0.65 MeV; m e a s u r e d (~(E). 1~C d e d u c e d r e s o n a n c e . REPT NEANDC(OR)-157/U,PI5,Ramstrom. NUCLEAR REACTIONS 4 ° C a ( p o l a r i z e d p,2p), 12 C, 16O ( p o l a r i z e d p,2d),E=150 MeV; m e a s u r e d cr(Ep Ez). 4°Ca d e d u c e d s t r o n g l y b o u n d p r o t o n s h e l l e f f e c t s . ~ZC,~O d e d u c e d d e u t e r o n c l u s t e r effects. Energy-sharing,quasifree g e o m e t r i e s . DWIA a n a l y s i s . BAPSA 27 509,EFS,Rees.

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82StZW:

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82MiZR:

81SeZX: 81WeZX: 82AnZW:

82BhZY: 82PeZY:

82SaZU:

13 N

R

82HaZT:

82PeZY:

82SaZU:

130

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82MiZW:

R 81BeYZ:

81NaZQ:

14 C

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81BaZR:

81MuZU: 82BhZY: 82C1ZX: 82JeZZ: 82P1ZZ:

continued

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NUCLEAR REACTIONS laC(e,e'~r+),E=195 MeV; m e a s u r e d a(E(Tr)),a(0). 13B l e v e l s d e d u c e d s t r o n g spin-flip excitation. B A P S A 27 719,DCS,Min. NUCLEAR REACTIONS * Z C , l S O ( n , X ) , E = 3 - 3 0 MeV; m e a s u r e d ( ; ( t o t a l ) v s E. 13C,*?0 d e d u c e d resonance parameters,T,isospin mixing matrix elements. Tof. S-matrix a n a l y s i s . REPT Kf K-3263-B,Cier jacks. NUCLEAR REACTIONS 13C(Tr+,lr+'),(Tr-jr-'),E=162 MeV; m e a s u r e d ~(0); d e d u c e d a(Tr-)/a(~r+). 13C l e v e l s d e d u c e d B(E2). O p t i c a l , c o l l e c t i v e m o d e l a n a l y s e s . REPT L A - 8 9 1 6 - T , S e e s t r o m - M o r r i s . NUCLEAR REACTIONS 13C(13C,13C'),E=42 MeV; m e a s u r e d a ( E ( l a c ' ) ) , l a c T - c o i n , lac l e v e l s d e d u c e d single,mutual excitation probabilities. B A P S A 26 1152,EBS,Wells. NUCLEAR REACTIONS 12,13C(~r+jr+),(~r+,Tr+'),(Tr-,Tr-),(~r-,Tr-'),E=t00 MeV; m e a s u r e d ~ ( 0 ) . 13C level deduced a(Tr-)/a(Tr+),configuration. First-order optical model,isobar-hole calculations. B A P S A 27 7 2 1 , D D S , A n t o n u k . NUCLEAR REACTIONS 12,13C(d,p),E=17.6 MeV; m e a s u r e d a(0). 13,~4C l e v e l s d e d u c e d e x c i t a t i o n mechanism. B A P S A 27 5 6 1 , H X a S , B h a n g . NUCLEAR REACTIONS ~aC(p,p'),(p,n),E=26 MeV; m e a s u r e d (r(0); d e d u c e d r e a c t i o n m e c h a n i s m . *3C,laN l e v e l s d e d u c e d yield ratios. Microscopic DWBA a n a l y s i s . B A P S A 27 4 6 1 , A Y a 1 3 , Peterson. NUCLEAR REACTIONS 1 6 0 , 4 ° C a ( a , p a ) , ( a , d a ) , ( ( x , t a ) , ( a , a H e ( x ) , ( a , 2 ( ~ ) , E = 1 3 9 . 2 MeV; l ~ 0 , 4 ° C a ( p , 2 p ) , (p,pd),(p,pt),E=101.3 MeV; 4 °Ca (p,2p),(p,pd),(p,pt),E=76.1 MeV; measured (particle)(particle)-coin,q(E~,E2,0~,0~). ~5,14,13N,3s,as,aTK,~ac,a?Ar l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree geometry. DABBB 4 2 3 7 3 7 , S a m a n t a . NUCLEAR REACTIONS *5N,~,~?,~aO(p,(x),E=45 MeV; m e a s u r e d (r(0); d e d u c e d optical model parameters. *3N,~C l e v e l s d e d u c e d j - t r a n s f e r . Zero-range DWBA,microscopic form factors. REPT J U L - S p e z - 1 4 6 , P 2 7 , H a u s e r . NUCLEAR REACTIONS ~3C(p,p'),(p,n),E=26 MeV; m e a s u r e d (~(0); d e d u c e d r e a c t i o n m e c h a n i s m . 13C,13N l e v e l s d e d u c e d yield ratios. Microscopic DWBA a n a l y s i s . B A P S A 27 4 6 1 , A Y a 1 3 , Peterson. NUCLEAR REACTIONS 1 6 0 , 4 ° C a ( ( ~ , p ( ~ ) , ( ( x , d a ) , ( ( x , t a ) , ( a , a H e a ) , ( a , 2 a ) , E = 1 3 9 . 2 MeV; *60,4°Ca(p,2p), (p,pd),(p,pt),E=101.3 MeV; 4°Ca(p,2p),(p,pd),(p,pt),E=76.1 MeV; measured (particle)(particle)-coin,a(Ei,E~,0~,02). 15,14,13N,aa,as,aTK,laC,aTAr l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree geometry. DABBB 4 2 3 7 3 7 , S a m a n t a . R A D I O A C T I V I T Y ~aO(fl+) [ f r o m ~4N(p,2n),E=45 MeV3; m e a s u r e d f l - d e l a y e d Ep,lp; d e d u c e d TI/~. REPT RCNP O s a k a , 1 9 8 1 A n n , P 1 3 3 , M i n a m i s o n o .

A 14 B

12

R A D I O A C T I V I T Y ~UN [ f r o m *ZC(aHe,t),E=75,81 MeV3; m e a s u r e d pt-coin,pt(0),total energy spectrum. REPT KVI 1981 A n n , P 2 4 , S t e r r e n b u r g . NUCLEAR REACTIONS ~C(aHe,tp),E=81 MeV; m e a s u r e d a(O),pt(O). ~2N d e d u c e d b r o a d s t r u c t u r e s , p o s s i b l e J,~r. M i c r o s c o p i c DWBA a n a l y s i s . REPT KVI 1981 A n n , P 2 4 , S t e r r e n b u r g .

A 13 B

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ONLY)

=

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NUCLEAR REACTIONS 48Ca(14C,14Be),E=87.4 MeV; lSO(laO,a20),E=96 MeV; m e a s u r e d u p p e r l i m i t for production o f 14Be,220. 14C(i4C,14B),E=87.4 MeV; laO(leO,lSN),(leO,19N),48Ca(laO,IeC),E=100 MeV; m e a s u r e d a(E(14B)),a(E(leN)),a(E(~SN)),cr(E(IeC)), i4B,laC,le,lSN,210 d e d u c e d m a s s e x c e s s , l e v e l s . REPT IPN 1981 A n n u a l , P N 2 0 , B e r n a s . NUCLEAR REACTIONS 14C(14C,14B),E=87.4 MeV; 48Ca(laO,16C),(lSO,17C),(IaO,12C),ISo(180,18N), *eO(iSO,*SN),E=100 MeV; m e a s u r e d (;(fragment) v s (Q); 4SCa(14C,14Be),E=87.4 MeV; laO(leO,zzO), E=lO0 MeV; m e a s u r e d production ~ u p p e r l i m i t . 14B,IsC,lS,lgN d e d u c e d m a s s . CONF H e l s i n g o r V o l 2 P376, CERN 8 1 - 0 9 . NUCLEAR REACTIONS 14C(w+,Tr+'),(Tr-,w-'),E=164 MeV; m e a s u r e d a(E(~),O); d e d u c e d p r o t o n , neutron transition amplitude cancellation. 14C l e v e l s deduced g(~¢+)/a(Tv-). REPT LA-8768-PR,P40,Baer. NUCLEAR REACTIONS 1 2 , 1 3 C ( n , 7 ) , E = t h e r m a l ; m e a s u r e d a(capture),ratio. 14C l e v e l d e d u c e d spectroscopic factor. Lane-Lynn t h e o r y . B A P S A 26 l 1 3 8 , C E 2 , M u g h a b g h a b . NUCLEAR REACTIONS 12,13C(d,p),E=lT.6 MeV; m e a s u r e d ~(0). 13,14C l e v e l s d e d u c e d e x c i t a t i o n mechanism. B A P S A 27 5 6 1 , H X a 9 , B h a n g . NUCLEAR REACTIONS llB(SLi,3He),(SLi,t),E n o t g i v e n ; m e a s u r e d a(E(3He)),a(Et),G(0), t4C d e d u c e d l e v e l s . 14N d e d u c e d a n a l o g s t a t e s . B A P S A 27 6 9 6 , A C 3 , C l a r k . NUCLEAR REACTIONS 13C(n,7),E=5.6-14 MeV; m e a s u r e d (7(0),analyzing p o w e r v s 0. 14C d e d u c e d T=0,E2 resonance. Direct-semidireet m o d e l . DABBB 42 4 4 6 8 , J e n s e n . NUCLEAR REACTIONS 14C(e,e'),E=135,195 MeV; m e a s u r e d G(0=1806). 14C l e v e l s d e d u c e d J,Tr,T, transition multipolarity. B A P S A 27 5 3 0 , G E S , P l u m .

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82HuZZ 82MaZZ 82RiZY 82SaZU

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D 82HoZY R 82HaZM

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81JuZX 82HAZY

82KyZZ 828aZU:

82WaZT: 82WeZU 150

R 81HeZT

D 82GaZY R 80MaZD 80MAZE 81HaZG

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15

NUCLEAR REACTIONS 15N,~60(a,~'),(a,2a),(a,ta),lSN(a,pa),E=155 MeV; m e a s u r e d a(Ea'),a~-, a(particle)-coin. 15N,160 d e d u c e d T=0,GQR d e c a y c h a r a c t e r i s t i c s . REPT J U L - S p e z - 9 9 , P S , Gerhardt. NUCLEAR REACTIONS 1 5 N ( v , n ) , ( v , 2 n ) , E = t h r e s h o l d - 3 8 MeV; m e a s u r e d ~ ( t o t a l ) . 15N d e d u c e d resonances,giant resonance,T(<),T(>) components. BAPSA 26 l 1 2 8 , B E 2 , J u r y . NUCLEAR REACTIONS l e , l a c ( a , p ) , l a C ( a , d ) , E = 3 5 MeV; m e a s u r e d ( p a r t i c l e ) ( p a r t i c l e ) - c o i n . 15N levels deduced a-,d-,t-decay m o d e s . 16N d e d u c e d n o c h a r g e d p a r t i c l e d e c a y . BAPSA 27 492, DXa8,Hamill. NUCLEAR REACTIONS 160(Tr+,Tr+p),(Tr-,rr-p),E=163,240 MeV; m e a s u r e d r r p - c o i n . 15N levels d e d u c e d a(Tr+)/a(rr-). Kinematically complete experiment. BAPSA 27 721,DD12,Kyle. NUCLEAR REACTIONS 160,4°Ca(a,p~),(a,da),(~,t~),(~,aHea),(~,2~),E=139.2 MeV; 160,4°Ca(p~gp), (p,pd),(p,pt),E=101.3 MeV; 46Ca(p,3 p),(p,pd),(p,pt),E= 76.1 MeV; measured (particle)(particle)-coin,a(Ei,E2,01,0e). 15,14jaN,aa,as,a~K,laC,aTAr l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a . NUCLEAR REACTIONS mN('y,n),E=lS-25 MeV b r e m s s t r a h l u n g ; m e a s u r e d or(0). 15N d e d u c e d GDR i s o s p i n s p l i t t i n g . PHCAA 38 3 4 , E A 7 , W a t s o n . NUCLEAR REACTIONS 12C(polarized t,y),E=2.3,3.3 MeV; m e a s u r e d a n a l y z i n g p o w e r ; d e d u c e d reaction mechanism. 15N l e v e l d e d u c e d J,rr. BAPSA 27 708,BE2,Weller. NUCLEAR REACTIONS 160(lr+,p),E=66 MeV; 9Be(rr+,p),E=50 MeV; m e a s u r e d or(0); d e d u c e d a n g u l a r momentum mismatch e f f e c t . *50,SBe d e d u c e d h i g h - s p i n state selective excitation. One-, two-nucleon m o d e l s . REPT I P N O - T - 8 1 - 0 1 , H e n n i n o .

A 16 N

14

NUCLEAR REACTIONS 13C(n,n'),E=4.55-8.25 MeV; m e a s u r e d or(0). 14C level d e d u c e d J,~r. BAPSA 27 6 2 8 , H 4 , R e s l e r . NUCLEAR REACTIONS *4N(a,a),(a,a'),E=34.7 MeV; m e a s u r e d ff(E~'),cr(8). ~4N l e v e l s d e d u c e d L-transfer. O p t i c a l m o d e l , D W B A a n a l y s e s . REPT D O E / E R / 4 0 0 1 4 - 3 , P g 6 , E v a n e t i c h . NUCLEAR REACTIONS l°,l~B,14N(Tr+,rr+'),(~r-,~r-'),E=162 MeV; m e a s u r e d cr(E(Tr)). I4N d e d u c e d level,J,Tr. 11B l e v e l s d e d u c e d l a r g e 7r+/rr - d i f f e r e n c e s . REPT L A - 8 7 6 8 - P R , P 3 1 , M o r r i s o n . NUCLEAR REACTIONS ~4C(p,n)E=26.3 MeV; m e a s u r e d cr(En). *4N d e d u c e d levels. Tof. REPT DOS/ ER/40014-3,P23,Ullmann. NUCLEAR REACTIONS l l B ( % i , a H e ) , ( 6 L i , t ) , E n o t g i v e n ; m e a s u r e d a ( E ( 3 H e ) ) , a ( E t ) , a ( O ) . 14C d e d u c e d l e v e l s . 14N d e d u c e d a n a l o g s t a t e s . BAPSA 27 6 9 6 , A C 3 , C l a r k . NUCLEAR REACTIONS ~4N(rr+,rr+),(~r+,Tr+'),(rr-,rr-),(rr-,rr-'),E=162 MeV; m e a s u r e d a(O). *4N deduced level,possible J,~r,a(rr-)/a(rr+),isospin mixing effects,L. Optical model, m i c r o s c o p i c DWIA a n a l y s e s . REPT A N L - 8 1 - 7 9 , P 1 6 , G e e s a m a n . NUCLEAR REACTIONS ~4N(e,e),(e,e'),E=165-225 MeV; m e a s u r e d a(O=180°). 14N l e v e l d e d u c e d transverse M1 f o r m f a c t o r . BAPSA 27 5 3 0 , G E 8 , H u f f m a n . NUCLEAR REACTIONS *4C(polarized p,n),E=120,160 MeV; m e a s u r e d ~ ( O ) , a s y m m e t r y . l~N d e d u c e d l e v e l s . Tof. DWBA a n a l y s i s . BAPSA 27 2 6 , D F 8 , M a s t e r s o n . NUCLEAR REACTIONS '60(rr+,2p),E=60 MeV; m e a s u r e d p p - c o i n , m i s s i n g m a s s s p e c t r u m . 14N deduced possible T=l,level. Kinematically complete experiment. BAPSA 27 4 6 8 , B F 1 4 , R i e d e r . NUCLEAR REACTIONS l°O,4°Ca(a,pa),(a,da),(a,ta),(a,aHea),(a,2~),E=139.2 MeV; l~0,4°Ca(p,2p), (p,pd),(p,pt),E=101.3 MeV; 4°Ca(p,gp),(p,pd),(p,pt),E= 76.1 MeV; measured (particle)(particle)-coin,a(EpEe,Ol,Oz). 15,14,~aN,ag,as,a~K,*aC,37Ar l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a . RADIOACTIVITY a4,aSAl,140; m e a s u r e d fly CP c o r r e l a t i o n a s y m m e t r y . ~4Mg l e v e l s d e d u c e d isospin mixing,charge dependent matrix e l e m e n t . DABBB 42 4 8 4 8 , H o y l e . NUCLEAR REACTIONS *4N,e~Mg(aHe,t),E n o t g i v e n ; m e a s u r e d Q - v a l u e d i f f e r e n c e . *~0,z6mA1 d e d u c e d Q ( E C ) , s u p e r a l l o w e d f l - d e e a y f t . BAPSA 27 6 9 6 , A C 4 , H a r d y .

A i5 N

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R A D I O A C T I V I T Y 16N; m e a s u r e d f l - b r a n e h i n g r a t i o ; d e d u c e d c o u p l i n g c o n s t a n t r a t i o ( g p / g A ) , meson exchange current e f f e c t s . BAPSA 27 4 9 2 , D X a 9 , G a g l i a r d i . NUCLEAR REACTIONS 1 7 0 ( p o l a r i z e d d , t ) , ( p o l a r i z e d d,aHe),E n o t g i v e n ; m e a s u r e d i%1(0). 160, 16N l e v e l s d e d u c e d p a r t i c l e - h o l e c h a r a c t e r . DWBA c a l c u l a t i o n . REPT KfK-3068,Pal,Mairle. NUCLEAR REACTIONS 180,12C,a4S(polarized d,cQ,E=52 MeV; m e a s u r e d iT11(0), l°B,aeP,16N l e v e l s d e d u c e d L,J,~,stretched c o n f i g u r a t i o n . DWBA a n a l y s i s . REPT K f K - 3 0 6 8 , P 2 9 , M a i r l e . NUCLEAR REACTIONS *eC(~,p),E=35 MeV; m e a s u r e d ~(0). 16N d e d u c e d levels. DWBA a n a l y s i s . REPT DOE/ER/4OO14-3,P18,HamiI1.

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81JaZV: 81KeZY:

81RaZP: 81TaZU: 82CrZY: 82KaZV: 82KuZL: 82LeZU:

82ReZZ:

82StZS: tsF

R 82StZV:

t6Ne

R 82WoZX:

R 81CiZZ:

82RaZX:

17F

R 82RoZU:

R 81BeYZ:

81NaZQ:

18 N

R 80BeYR:

continued

=

17

NUCLEAR REACTIONS t S C , 1 8 0 ( n , X ) , E = 3 - 3 0 MeV; m e a s u r e d a(total) v s E. 13C,lV0 d e d u c e d resonance parameters,T,isospin mixing matrix elements. Tof. S - m a t r i x a n a l y s i s . REPT Kf K-3263-B,Cier jacks. NUCLEAR REACTIONS 170(e,e'),E n o t g i v e n ; m e a s u r e d f o r m f a c t o r s . 170 l e v e l s d e d u c e d B(M2). BAPSA 27 4 9 2 , D X a 1 0 , R a n g a c h a r y u l u . NUCLEAR REACTIONS 2 0 N e ( p , c ( ) , E = 2 2 . 5 , 2 7 , 3 5 , 4 0 MeV; m e a s u r e d (T(0). tTF l e v e l s d e d u c e d normalization factor. DWBA,coupled-chanels a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 2 4 , R o h w e r .

A

~eC

16

NUCLEAR R E A C T I O N S t2,13C(cx,p),13C((x,d),E=35 MeV; m e a s u r e d (particle)(particle)-eoin. tSN levels deduced a-,d-,t-decay modes. 18N deduced no charged particle decay. B A P S A 27 492, DXa8,Hamill. NUCLEAR R E A C T I O N S 170(polarized d,t),(polarized d,3He),E not given; m e a s u r e d iTn(0), re0, I~N levels d e d u c e d particle-hole character. D W B A calculation. R E P T KfK-3068,P31,Mairle. NUCLEAR R E A C T I O N S 24,28Mg,Zs,38Si(ISO,t2C),E=100 MeV; m e a s u r e d a(Ec(),residual nucleus disintegration, tSO d e d u c e d K=0-,0 + b a n d selective population,nuclear polarization. R E P T IPN 1981 Annual,PN30,Bernas. NUCLEAR R E A C T I O N S ISN,IsO((x,(x'),((x,2(x),((x,t(x),ISN(c(,p(x),E=iG5MeV; m e a s u r e d (7(E(x'),cxcx-, cx(particle)-coin, tSN,tsO d e d u c e d T = 0 , G Q R decay characteristics. R E P T JUL-Spez-99,P5, Gerhardt. NUCLEAR R E A C T I O N S 2°,22Ne(d,SLi),E=55 MeV; m e a s u r e d (7(0). Is,tSO levels d e d u c e d Sex, (x-reduced widths,cluster structure. B A P S A 26 l126,BD3,Janecke. NUCLEAR R E A C T I O N S 8Be,t3C(%i,t),E=30,34,38 MeV; m e a s u r e d cr(Et),a(0), t2C levels deduced low population probability. 180 levels d e d u c e d L,tentative J,~. B A P S A 26 III5,ACI0, Kemper. NUCLEAR R E A C T I O N S t2,13C,2aSi(ISO,cxX),E=I40 MeV; m e a s u r e d c~X-coin, t60 deduced b r e a k u p characteristics. B A P S A 26 II21,BB3,Rae. NUCLEAR R E A C T I O N S 48Ca(1°0,12C(x),E=310 MeV; m e a s u r e d 12Cc(-coin. 180 deduced b r e a k u p characteristics. B A P S A 26 l122,BB10,Takada. NUCLEAR R E A C T I O N S 13C(cx,n),E=35 MeV; m e a s u r e d (7(En),cr(0). t60 d e d u c e d possible T=I states. DWBA,cluster transfer,knockout m e c h a n i s m s . B A P S A 27 561,HXa14,Craig. NUCLEAR R E A C T I O N S 180(12C,(xi2C),E=I30 MeV; m e a s u r e d (12C)(1~C)-coin. 180 levels deduced excitation m e c h a n i s m . B A P S A 27 698,AD7,Karp. NUCLEAR R E A C T I O N S ts0(%n),E=30-35 MeV; measured or(0), m O deduced T=I,GQR. P H C A A 38 34, EA8,Kuo. NUCLEAR R E A C T I O N S tSN(p,p),(p,(x),E ~, resonance; m e a s u r e d or(0) vs E. 160 resonances d e d u c e d rp,r(x,isospin mixing. R - m a t r i x analysis. P H C A A 38 21,CA5,Leavitt. NUCLEAR R E A C T I O N S 48Ca(polarized p,2p),12C,160(polarized p,2d),E=150 MeV; m e a s u r e d a(E I, E2). 4°Ca d e d u c e d strongly b o u n d proton shell effects. 12C,160 d e d u c e d deuteron cluster effects. Energy-sharing,quasifree geometries. D W I A analysis. B A P S A 27 509,EF8,Rees. NUCLEAR R E A C T I O N S 12C(IsO,(xX),E=I00-150 MeV; measured a(Ea). 160 deduced sequential decay. K i n e m a t i c analysis. B A P S A 27 699,AD9,Stwertka. NUCLEAR R E A C T I O N S ISO(3He,t),E=81 MeV; m e a s u r e d (7(Et),a(0). 16F levels d e d u c e d Jjr, configuration. Microscopic D W B A analysis. R E P T KVI 1981 Ann,P25,Sterrenburg. NUCLEAR R E A C T I O N S 2°Ne(c~,SHe),E=129 MeV; measured a(reaction). 16Ne deduced mass. Enriched gas target,split-pole spectrograph. B A P S A 27 561,HXa15,Woodward.

A t'~ 0

=

ONLY)

=

18

NUCLEAR REACTIONS 4SCa(14C,14Be),E=87.4 MeV; teO(taO,220),E=96 MeV; m e a s u r e d

upper

limit

for production of '4Be,220. 14C(14C,*4B),E=87.4 MeV; *eO(IsO,teN),(teO,19N),4eCa(tSO,*sC),E=100 MeV; m e a s u r e d a(E(14B)),a(E(ISN)),(7(E(19N)),cT(E(IsC)). 14B,IsC,IS,tgN,210 d e d u c e d m a s s excess, levels. R E P T IPN 1981 Annual,PN20,Bernas. NUCLEAR REACTIONS t4C(t4C,14B),E=87.4 MeV; 4SCa(tSO,IsC),(ieO,t~C),(tSO,t2C),leO(180,tSN), ISO(tsO,iSN),E=100 MeV; m e a s u r e d (7(fragment) vs (Q); 4SCa(t4C,14Be),E=87.4 MeV; ISO(tsO,220), E=I00 MeV; m e a s u r e d production (~ upper limit. 14B,tsC,le,19N deduced mass. C O N F Helsingor Vol2 P376, C E R N 81-09. NUCLEAR R E A C T I O N S ISo(tS0,tgN),E=100 MeV; m e a s u r e d (z(E(19N)). 14C(tsO,leN),E not given. 19 'aN deduced levels,mass excess. 14C(14C,14B),E not given; m e a s u r e d t4B mass. R E P T IPN 1980 Annual,PN31,Bernas.

208

SECONDARY

SOURCES

(Reporks,Abstracts,etc.

A 18 N

R 81BeYZ:

81NaZQ:

~S0

R 81GrZT:

81JaZV: 82GaZT: 82RuZZ: 18F

D 82DaZZ:

leNe

D 82DaZZ: 82VoZY:

R 80EeYR:

81BeYZ:

81NaZL:

81NaZQ:

~90

R 82KoZS: 82KoZV:

19F

D 82LoZZ:

19Ne

D 82LoZZ: 82MaZY: 82ScZZ:

D 82QuZY: R 82QuZY:

ZONe

D 81HoZ0:

continued

=

19

NUCLEAR REACTIONS iSO(1sO,19N),E=100 MeV; m e a s u r e d ct(E(19N)). 14C(180,18N),E n o t g i v e n . 19 lSN d e d u c e d l e v e l s , m a s s e x c e s s . 14C(14C,14B),E n o t g i v e n ; m e a s u r e d 14B m a s s . REPT tPN 1980 Annual,PN31,Bernas. NUCLEAR REACTIONS 4SCa(14C,14Be),E=87.4 MeV; 180(180,220),E=96 MeV; m e a s u r e d u p p e r l i m i t for production o f 14Be,ZZO. 14C(14C,14B),E=87.4 MeV; I80(LB0,1SN),(IB0,19N),48Ca(180,18C),E=100 MeV; m e a s u r e d a(E(14B)),a(E(18N)),a(E(19N)),a(E(IsC)). 14B,lsC,18,19N,ZI0 d e d u c e d m a s s e x c e s s , l e v e l s . REPT IPN 1981 A n n u a l , P N 2 0 , B e r n a s . NUCLEAR REACTIONS 1SO(180,19N),E=100 MeV; 180(180,aIO),E=92 MeV; m e a s u r e d a(E(tSN)), a(E(zlO)). 19N d e d u c e d levels,mass. 210 d e d u c e d l e v e l s .~ S e l f - s u p p o r t i n g AlzO 3 t a r g e t , magnetic spectrometer. REPT I P N O - P h N - 8 1 - 2 0 , N a u l i n . NUCLEAR REACTIONS 14C(14C,14B),E=87.4 MeV; 48Ca(lS0,16C),(ISO,17C),(ISO,IzC),I80(180,18N), 1BO(IS0,19N),E=100 MeV; m e a s u r e d o ' ( f r a g m e n t ) v s (Q); 4BCa(14C,14Be),E=87.4 MeV; 180(180,2z0), E=100 MeV; m e a s u r e d p r o d u c t i o n a u p p e r l i m i t . 14B,18C,IS,19N d e d u c e d m a s s . CONF H e l s i n g o r Vol2 P376, CERN 8 1 - 0 9 . NUCLEAR REACTIONS 1 8 0 ( n , n ) , ( n , n ' ) , E = 6 - 7 . 2 MeV; m e a s u r e d o ' ( 0 ) , a ( t o t a l ) v s E. 190 d e d u c e d levels,fT/2 strength fragmentation. BAPSA 27 7 1 5 , C E 1 , K o e h l e r . NUCLEAR REACTIONS 1 8 0 ( n , n ) , ( n , n ' ) , E = 6 - 6 . 4 MeV; m e a s u r e d a(O). 190 d e d u c e d r e s o n a n c e s . BAPSA 27 6 2 8 , H 3 , K o e h l e r . R A D I O A C T I V I T Y 19Ne [ f r o m F(p,N),E=22 MeV]; m e a s u r e d Y'y-,fly3'-coin. 19F level d e d u c e d Ifl. BAPSA 27 4 9 2 , D X a 4 , L o w r y . R A D I O A C T I V I T Y 19Ne [ f r o m F(p,N),E=22 MeV]; m e a s u r e d y-y-,fl'y3,-coin. 19F level d e d u c e d Ifl. BAPSA 27 4 9 2 , D X a 4 , L o w r y . R A D I O A C T I V I T Y ruNe; m e a s u r e d f l - a s y m m e t r y ; deduced /z. Polarized source. BAPSA 27 493,DXall, Macarthur. R A D I O A C T I V I T Y 19Ne; m e a s u r e d f l - a s y m m e t r y ; d e d u c e d d e p o l a r i z a t i o n c o r r e c t i o n s . S o u r c e in t h i n cell. BAPSA 27 4 9 2 , D X a 6 , S c h r e i b e r .

A ao F

18

NUCLEAR REACTIONS 48Ca(14C,14Be),E=87.4 MeV; 180(IBO,2zO),E=96 MeV; m e a s u r e d u p p e r l i m i t for production o f 14Be,a20. 14C(14C,~4B),E=87.4 MeV; 1SO(190,~SN),(IBO,"9N),4eCa(190,19C),E=lO0 MeV; m e a s u r e d a(E(14B)),a(E(ISN)),cr(E(19N)),a(E(lsC)). 14B,19C,Ie,19N,210 d e d u c e d m a s s e x c e s s , l e v e l s . REPT IPN 1981 A n n u a l , P N 2 0 , B e r n a s . NUCLEAR REACTIONS 14C(14C,14B),E=87.4 MeV; 4SCa(180,ISC),(Is0,17C),(IZO,IgC),lBO(lsO,18N), 190(180,19N),E=100 MeV; m e a s u r e d o r ( f r a g m e n t ) v s (Q); 48Ca(14C,14Be),E=87.4 MeV; 180(180,ZeO), E=100 MeV; m e a s u r e d p r o d u c t i o n a u p p e r l i m i t . HB,lsC,IS,19N d e d u c e d m a s s . CONF H e l s i n g o r Vol2 P376, CERN 8 1 - 0 9 . NUCLEAR REACTIONS ZoSpb(180,Is0),(180,180'),E=120 MeV; m e a s u r e d c~(O). 180 l e v e l d e d u c e d m a g n e t i c s u b s t a t e p o p u l a t i o n . L i n e s h a p e m e a s u r e m e n t s , Q 3 D s p e c t r o g r a p h . BAPSA 26 1152, EBT,Gross. NUCLEAR REACTIONS z°,aZNe(d,SLi),E=55 MeV; m e a s u r e d ~r(O). 1s,190 l e v e l s d e d u c e d Sa, a-reduced widths,cluster structure. BAPSA 26 l 1 2 6 , B D 3 , J a n e c k e . NUCLEAR REACTIONS 1 4 C ( a , 7 ) , E = l . l - 2 . 7 MeV; m e a s u r e d r e s o n a n c e c a p t u r e . ~80 r e s o n a n c e s d e d u c e d d e c a y m e c h a n i s m , B ( X ) . BAPSA 27 697,AD1,Gai. NUCLEAR REACTIONS 14C(7Li,t),E=15 MeV; m e a s u r e d t T - c o i n . 180 levels deduced B(X). BAPSA 27 698,AD2,Ruscev. R A D I O A C T I V I T Y lSNe; m e a s u r e d E3',I7 f o l l o w i n g f l - d e e a y ; d e d u c e d log f t , w e a k p i o n c o u p l i n g c o n s t a n t . 19F l e v e l s d e d u c e d Ifl. BAPSA 27 4 9 2 , D X a 3 , D a e h n i c k . R A D I O A C T I V I T Y IBNe; m e a s u r e d Ey,I7 f o l l o w i n g f l - d e c a y ; d e d u c e d log f t , w e a k p i o n c o u p l i n g c o n s t a n t . ISF l e v e l s d e d u c e d Ifl. BAPSA 27 4 9 2 , D X a 3 , D a e h n i c k . R A D I O A C T I V I T Y 21Ne; m e a s u r e d 3' CP. 18Ne; m e a s u r e d f l - d e c a y . DABBB 42 4 8 4 8 , V o n L i n t i g .

A ~9 N

=

ONLY)

=

20

R A D I O A C T I V I T Y z°F [ - f r o m 1 9 F ( p o l a r i z e d d , p ) ] ; m e a s u r e d fl-asymmetry,Iy(0); deduced polarization transfer,alignment. BAPSA 27 5 2 5 , E Y b 1 4 , Q u i n . NUCLEAR REACTIONS 1 9 F ( p o l a r i z e d d,p),E n o t g i v e n ; m e a s u r e d iy(0); d e d u c e d p o l a r i z a t i o n transfer. Z°F d e d u c e d a l i g n m e n t . BAPSA 27 5 2 5 , E Y b 1 4 , Q u i n . R A D I O A C T I V I T Y a°Na,24Al,ZsP,3zC1,36K,4°Sc; m e a s u r e d f l - d e l a y e d Ep,Ip,Ea,ta; d e d u c e d logft. 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J , r r , T , a - r e d u e e d w i d t h s . Z4Mg l e v e l s deduced J,rr,a-redueed w i d t h s . 3aS,zzSi,aSAr,4°Ca l e v e l s d e d u c e d J , r r , F a / F p , p - , a - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n .

209

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A 2ONe

D 82C1ZY:

R 800eZZ: 80SuZV: 81KaZN:

810sZX:

82CaZW: 82HiZY: ZONa

D 81HoZ0:

82ClZY:

R 81BeYZ:

81NaZL:

Z~Ne

D 82VoZY:

R 800eZZ:

22No

D 79DaZD: 81NeZX:

81SkZY: 82GiZY:

R

81MaZL: 82HoZU:

=

21

=

22

NUCLEAR REACTIONS 24,26Mg(d,6Li),E=80 MeV; m e a s u r e d a(E(6Li)),(~(0), e°,eZNe l e v e l s d e d u c e d So. F i n i t e - r a n g e DWBA a n a l y s i s . REPT J U L - S p e z - 7 2 , P 2 3 , 0 e l e r t . R A D I O A C T I V I T Y 22Na; m e a s u r e d pair production. CONF R i g a , P 4 6 1 , D a n i l e n k o . R A D I O A C T I V I T Y 22Na [ f r o m lOF(a,n),E=3.73 MeV]; m e a s u r e d DSA. 22Na l e v e l d e d u c e d TI/2,M1 transition strength. High resolution,precision plunger,Si-Li d e t e c t o r . BAPSA 26 1126,BD7, Neyer. R A D I O A C T I V I T Y 22Na; m e a s u r e d fl+ s p i n - p o l a r i z a t i o n . H i g h p r e c i s i o n . BAPSA 26 1126,BD6, Skalsey. R A D I O A C T I V I T Y 22Na(fl+); m e a s u r e d fl+ p o l a r i z a t i o n . Forbidden transition,68Ga standard. B A P S A 27 6 9 7 , A C 9 , G i r a r d .

A 2aNa

continued

NUCLEAR REACTIONS 48Ca(laC,14Be),E=87.4 MeV; lSO(~sO,zzO),E=96 MeV; m e a s u r e d u p p e r l i m i t for production o f 14Be,ZeO. ~4C(t4C,14B),E=87.4 MeV; ls0(ISO,ISN),(ISO,19N),4eCa(iSO,IsC),E=100 MeV; m e a s u r e d (;(E(14B)),a(E(18N)),a(E(19N)),a(E(lsC)). 14B,leC,la,iON,elO d e d u c e d m a s s e x c e s s , l e v e l s . REPT IPN 1981 A n n u a l , P N 2 0 , B e r n a s . NUCLEAR REACTIONS 180(lSO,lON),E=100 MeV; 180(lSO,210),E=92 MeV; m e a s u r e d a(E(lON)), or(E(210)). 19N d e d u c e d levels,mass. ZlO d e d u c e d levels. Self-supporting Al~O 3 t a r g e t , magnetic spectrometer. REPT I P N O - P h N - 8 1 - 2 0 , N a u l i n . R A D I O A C T I V I T Y Z'Ne; m e a s u r e d 7 CP. laNe; m e a s u r e d f l - d e c a y . DABBB 42 4 8 4 8 , V o n L i n t i g .

A 22Ne

20

R A D I O A C T I V I T Y a°Na; m e a s u r e d f l - d e l a y e d a - p a r t i c l e e n e r g y shifts,T1/z,Ifl; d e d u c e d log f t , vector to a x i a l v e c t o r component ratios,vector weak coupling constant. ZONe l e v e l s deduced isospin mixing w i t h IAS. DABBB 42 4103,Clifford. NUCLEAR REACTIONS z4,Z°Mg(d,6Li),E=80 MeV; m e a s u r e d cr(E(°Li)),(;(0). 2°,CaNe l e v e l s d e d u c e d So. F i n i t e - r a n g e DWBA a n a l y s i s . REPT J U L - S p e z - 7 2 , P 2 3 , 0 e l e r t . NUCLEAR REACTIONS Z6Ne(a,a'),(a,2a),E=155 MeV; m e a s u r e d a ( E a ' ) , a a - c o i n . ZONe d e d u c e d T=0, GQR s p l i t t i n g . REPT J U L - S p e z - 7 2 , P 4 , S u k o s d . NUCLEAR REACTIONS 12C(l°O,a),E=142 MeV; m e a s u r e d a ' Z C ( 0 ) , a ' 6 0 ( 0 ) , a Z ° N e ( 0 ) . Z4Mg d e d u c e d r e s o n a n c e e x c i t a t i o n . ZONe l e v e l s d e d u c e d s e q u e n t i a l a - d e c a y . REPT RCNP O s a k a , 1 9 8 0 A n n , Pll9,Katori. NUCLEAR REACTIONS l Z C ( Z ° N e , l ° O ) , ( Z ° N e , Z 0 N e ) , E = 1 6 0 MeV; measured (x(l°O)(lZC)-, a(Z°Ne)(°Be)-coin; deduced reaction mechanism, a°Ne,Z4Mg d e d u c e d f o r m a t i o n mechanism as intermediate n u c l e i . REPT ISN 8 1 - 0 1 , P 4 7 , 0 s t . NUCLEAR REACTIONS mO(a,a),E > 9.2 MeV; m e a s u r e d a b s o l u t e a. a°Ne d e d u c e d resonances,J,~r, F , F a / F . B A P S A 27 6 9 7 , A C 7 , C a s k e y . NUCLEAR REACTIONS 1 6 0 ( a , a ' 7 ) , E n o t g i v e n ; m e a s u r e d ET,IT,pairproduction 7 - y i e l d . ZONe levels deduced Fa/F,noncluster structure. B A P S A 27 4 9 3 , D X a 1 2 , H i n d i . R A D I O A C T I V I T Y a°Na,24Al,ZsP,aaCl,3°K,4°Se; m e a s u r e d fl-delayed Ep,lp,Ea,la; deduced logft. 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n . ZONe l e v e l s d e d u c e d , J , r r , T , a - r e d u c e d w i d t h s . Z4Mg l e v e l s deduced J,Ir,a-reduced w i d t h s . 32S,zsSi,aOAr,4°Ca l e v e l s d e d u c e d J,~r,Fa/Fp,p-,a-reduced w i d t h s . REPT J Y F L 1 7 / 8 1 , H o n k a n e n . R A D I O A C T I V I T Y a°Na; m e a s u r e d f l - d e l a y e d a - p a r t i c l e e n e r g y s h i f t s , T , / 2 , 1 f l ; d e d u c e d log f t , vector to a x i a l v e c t o r component ratios,vector weak coupling constant. Z°Ne l e v e l s deduced isospin mixing w i t h IAS. DABBB 42 4 1 0 3 , C l i f f o r d .

A zl 0

=

=

23

NUCLEAR REACTIONS 9Be(14N,X),E n o t g i v e n ; m e a s u r e d f r a g m e n t m a s s . a3Na d e d u c e d e n t r a n c e channel e f f e c t s . A n a l y s i s o f o t h e r d a t a . B A P S A 26 l 1 3 2 , C B 1 0 , M a t e j a . NUCLEAR REACTIONS a 6 M g , a T A l ( p , a ) , E = 4 5 MeV; m e a s u r e d a(0); deduced optical model parameters. ZaNa l e v e l s d e d u c e d t r a n s i t i o n strengths. 24Mg l e v e l s d e d u c e d s p e c t r o s c o p i c amplitudes. Zero-range D W B A , c l u s t e r f o r m f a c t o r s . REPT J U L - S p e z - 1 4 6 , P 2 5 , H o y l e r .

210

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A Z4Mg

D 81HoZO

82HoZY R 80RoZS 81DaZV 81FoZU 81KaZN

810sZX:

81ViZY

82HoZU

82KaZX 82KaZZ

82WiZW:

82ZaZY:

82ZuZZ: a4A1

D 81HoZO

82HoZY R 8OKaZM

R 82FiZX

a5Mg

R 82FrZY 82WiZY:

a~A1

R 82WiZY:

24

RADIOACTIVITY a°Na,a4Al,asp,aaCl,aSK,4°Sc; m e a s u r e d fl-delayed Ep,Ip,Ea,Ia; deduced logft. 4°Sc d e d u c e d f l - s t r e n g t h function. ZONe l e v e l s d e d u e e d , J j r , T , a - r e d u c e d w i d t h s , a4Mg l e v e l s deduced Jjr,a-reduced widths, aaS,esSi,a6Ar,4°Ca l e v e l s d e d u c e d J,Tr,Fa/Fp,p-,a-reduced w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . R A D I O A C T I V I T Y a4,aeAl,~40; m e a s u r e d f17 CP c o r r e l a t i o n asymmetry, e4Mg l e v e l s d e d u c e d isospin mixing,charge dependent matrix element. DABBB 42 4 8 4 8 , H o y l e . NUCLEAR REACTIONS 24Mg,zSsi,seNi((x,a'),E=104 MeV; m e a s u r e d ~(0). a4Mg,aeSi,SSNi d e d u c e d T=0, dipole strength distribution,EWSR. DWBA a n a l y s i s . REPT K f K - 3 0 6 8 , P 4 3 , R o s t . NUCLEAR REACTIONS a°Ne(a,laC),(a,a),(a,a'),E=13.4-20.8 MeV; m e a s u r e d a(0),a(E), a4Mg deduced resonances,J,w,F. Lengendre polynomial a n a l y s i s . DABBB 42 6 7 3 , D a v i s . NUCLEAR REACTIONS a 4 M g ( n , n ) , ( n , n ' ) , E = 7 - 1 2 MeV; m e a s u r e d a ( 0 ) . a4Mg l e v e l s d e d u c e d fla. Optical,coupled-channels a n a l y s e s . REPT I N D C ( G D R ) - I 6 / G , P 1 , F o r t s c h . NUCLEAR REACTIONS IaC(160,a),E=142 MeV; m e a s u r e d a l a C ( 0 ) , a ' 6 0 ( 0 ) , a a ° N e ( 0 ) . 24Mg d e d u c e d r e s o n a n c e e x c i t a t i o n . Z°Ne l e v e l s d e d u c e d s e q u e n t i a l a-decay. REPT RCNP O s a k a , 1 9 8 0 A n n , Pllg,Katori. NUCLEAR REACTIONS 1 2 C ( a O N e , 1 6 0 ) , ( a ° N e , a ° N e ) , E = 1 6 0 MeV; measured a(~60)(laC) -, a(aONe)(SBe)-coin; d e d u c e d r e a c t i o n m e c h a n i s m . Z6Ne,a4Mg d e d u c e d f o r m a t i o n mechanism as intermediate n u c l e i . REPT ISN 8 1 - 0 1 , P 4 7 , 0 s t . NUCLEAR REACTIONS a 4 M g , a S S i , 3 Z S ( n , n ) , ( n , n ' ) , E = 9 . 7 6 , 1 4 . 8 3 MeV; m e a s u r e d a ( 0 ) . Z4Mg,aSsi,aas deduced deformation parameter systematics. Coupled-channels a n a l y s i s . REPT ISN 81-01,P50, Virdis. NUCLEAR REACTIONS a 6 M g , Z T A l ( p , a ) , E = 4 5 MeV; m e a s u r e d (7(0); d e d u c e d optical model parameters, a3Na l e v e l s d e d u c e d t r a n s i t i o n strengths, a4Mg l e v e l s d e d u c e d s p e c t r o s c o p i c amplitudes. Zero-range D W B A , c l u s t e r f o r m f a c t o r s . REPT J U L - S p e z - 1 4 6 , P 2 5 , H o y l e r . NUCLEAR REACTIONS laC(160,a),E=142 MeV; m e a s u r e d a(Ea,Oa),a(Ea,Oa,O(laC)), a4Mg d e d u c e d molecular resonance decay widths,branching r a t i o s . REPT RCNP Osaka,1981 A n n , P 1 0 9 , K a t o r i . NUCLEAR REACTIONS a 4 M g , a S S i ( p o l a r i z e d p , p ' ) , E = 6 5 MeV; m e a s u r e d a(Ep'),(y(0),analyzing p o w e r v s 0. a4Mg,zSSi l e v e l s d e d u c e d d e f o r m a t i o n parameters. CCBA a n a l y s i s . REPT RCNP Osaka,1981 Ann,P12,Kato. NUCLEAR REACTIONS laC(laC,laC'),E(cm)=15-33 MeV; m e a s u r e d lZC7(0 ). a4Mg r e s o n a n c e s d e d u c e d angle averaged spin alignment,phase angle parameters. Resonant,nonresonant theories. DABBB 4 2 4 8 4 8 , W i l l e t t . NUCLEAR REACTIONS a4Mg(e,e'),E=98-285 MeV; m e a s u r e d f o r m f a c t o r s , a4Mg d e d u c e d levels,J,Tr, T,eollective,particle-hole character. Shell model,projected Hartree-Fock,open s h e l l RPA calculations. DABBB 4 2 4 1 0 4 , Z a r e k . NUCLEAR REACTIONS IaC(IeC,'aC'),E=52-61 MeV; m e a s u r e d (~(0). a4Mg r e s o n a n c e s d e d u c e d L. B A P S A 27 6 9 8 , A D 4 , Z u r m u h l e . R A D I O A C T I V I T Y Z°Na,a4Al,asP,aaCl,a6K,4°Sc; m e a s u r e d fl-delayed Ep,Ip,Ea,Ia; deduced iogft. 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J j r , T , a - r e d u c e d w i d t h s , a4Mg l e v e l s deduced J,~r,a-reduced widths, aas,aSSi,a6Ar,4°Ca l e v e l s d e d u c e d JJr,Fa/Fp,p-,a-reduced w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . R A D I O A C T I V I T Y a4,aeAl,140; m e a s u r e d f17 CP c o r r e l a t i o n asymmetry, a4Mg l e v e l s d e d u c e d isospin mixing,charge dependent matrix element. DABBB 42 4 8 4 8 , H o y l e . NUCLEAR REACTIONS aTAl(aHe,aHe),E=73.14 MeV; m e a s u r e d cr(E(6He)); a4Mg(3He,t),E=59.57 MeV; measured cr(0,Et), a4A1 d e d u c e d l e v e l , T , m a s s e x c e s s . REPT INS T o k y o 1980 A n n , P 2 4 , K a t o .

A 25Na

=

ONLY)

=

25

NUCLEAR REACTIONS 3H(a6Mg,t),(a6Mg,d),(26Mg,a),E=40 MeV; m e a s u r e d ET,17,ty-,dT-,ay-coin , DSA. aSNa,a6,aTMg l e v e l s d e d u c e d TI/2. H i g h v e l o c i t y i o n r e c o i l i n C u , n - t y p e hyperpure Ge d e t e c t o r . B A P S A 27 4 9 3 , D X a 1 3 , F i e l d s . NUCLEAR REACTIONS 1 3 C ( l a C , X ) , E ( c m ) = 8 . 8 - 1 0 . 9 MeV; m e a s u r e d total a(fusion) v s E. aSMg deduced resonances. B A P S A 37 6 9 8 , A D 6 , F r a w l e y . NUCLEAR REACTIONS a T A l ( p , t ) , ( p , a H e ) , a l p ( p o l a r i z e d p,t),(polarized p,aHe),E=60 MeV; measured (r(0). aSMg,aSAl,agsi,agp d e d u c e d p o s s i b l e h i g h l y e x c i t e d T = 3 / 3 s t a t e s . B A P S A 27 461,AYa15,Wilkerson. NUCLEAR REACTIONS 2 7 A l ( p , t ) , ( p , a H e ) , a l p ( p o l a r i z e d p,t),(polarized p,3He),E=60 MeV; measured or(0), aSMg,aSAl,eoSi,aOp d e d u c e d p o s s i b l e h i g h l y e x c i t e d T = 3 / 2 s t a t e s . B A P S A a7 461,AYa15,Wilkerson.

211

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 2SMg

R 80BeYQ

81SpZZ 82FiZX

82GeZY

82LiZ0 82MiZQ

26A1

D 82KoZT: R 79KoZB: 82HaZM: 82MaZG 82SaZR

ZSSi

R 81AIZU

81CrZZ

D 80DeZE:

27Mg

R 82FiZX:

aTAl

R 80PuZZ: 81DiZY

82RyZZ 82SaZR 27Si

R 81CrZZ

D 80DeZE

2SAI

D 82HoZY R 79KaYU: 80YaZT: 81RoZT:

=

27

R A D I O A C T I V I T Y 27,2s,z9,3°,31,32Na; m e a s u r e d E T , 1 7 , 7 7 - c o i n . 33,34Na; m e a s u r e d E7,I7. O n - l i n e mass spectroscopic source separation. REPT IPN 1980 A n n u a l , P N 3 2 , D e t r a z . NUCLEAR REACTIONS 3H(26Mg,t),(2SMg,d),(26Mg,a),E=40 MeV; m e a s u r e d ET,IT,tT-,dT-,a7-coin, DSA. 25Na,2S,aTMg l e v e l s d e d u c e d T1/2. H i g h v e l o c i t y i o n r e c o i l i n C u , n - t y p e hyperpure Ge d e t e c t o r . B A P S A 27 4 9 3 , D X a 1 3 , F i e l d s . NUCLEAR REACTIONS a 7 A l ( ~ , a ' ) , E = 1 4 5 MeV; m e a s u r e d G(E~'),a(O). 27A1 l e v e l s d e d u c e d L, octupole excitation. REPT J U L - S p e z - 7 2 , P S , P u t t a s w a m y . NUCLEAR REACTIONS aTAl,iSTAu(p,p'X),E=200 MeV; m e a s u r e d a(Ep). 27A1 d e d u c e d G Q R , q u a s i f r e e scattering structure. Hyperpure Ge m u l t i - d e t e c t o r t e l e s c o p e . REPT J U L - S p e z - 9 9 , P 3 5 , Didelez. NUCLEAR REACTIONS 27Al(e,e'),E n o t g i v e n ; m e a s u r e d f o r m f a c t o r s . 27A1 l e v e l s d e d u c e d B(),), 6. B A P S A 27 5 3 0 , G E l l , R y a n . NUCLEAR REACTIONS 160(12C,d),(12C,p),E(cm)=17.3 MeV; m e a s u r e d p 7 - , d T - c o i n . 26,27A1 d e d u c e d multipolarity,Ti/2. B A P S A 27 6 9 7 , A C 1 2 , S a w . NUCLEAR REACTIONS 24,25,26Mg,aTAl(3He,n),E=25 MeV; m e a s u r e d a ( E n ) , G ( 0 ) . 2Ssi d e d u c e d l e v e l s . 27,26Si,aSP d e d u c e d l e v e l s , L . B A P S A 26 l 1 2 7 , B D 9 , C r a i g .

A aSNa

26

NUCLEAR REACTIONS ~4Mg(tSO,160),E n o t g i v e n ; m e a s u r e d G(0). aSMg l e v e l d e d u c e d e x c i t a t i o n mechanism. CCBA a n a l y s i s , t a r g e t , r e s i d u a l nuclei inelastic excitation. REPT IPN 1980 Annual,PN44,Bernas. NUCLEAR REACTIONS 2 ° s p b ( z S M g , 2 6 M g ' ) , E = 8 0 - 1 2 0 MeV; m e a s u r e d Coulomb excitation, reorientation. 26Mg l e v e l d e d u c e d q u a d r u p o l e moment,B(E2). B A P S A 26 l 1 2 7 , B D 1 0 , S p e a r . NUCLEAR REACTIONS 3H(2~Mg,t),(26Mg,d),(26Mg,a),E=40 MeV; m e a s u r e d ET,17,tT-,dT-,a7-coin, DSA. 25Na,2S,27Mg l e v e l s d e d u c e d T,/2. H i g h v e l o c i t y i o n r e c o i l i n C u , n - t y p e hyperpure Ge d e t e c t o r . B A P S A 27 4 9 3 , D X a 1 3 , F i e l d s . NUCLEAR REACTIONS 2aMg(polarized p,p'),E=135 MeV; m e a s u r e d a(0),A(0). 2SMg d e d u c e d l e v e l s , J,rr,high-spin state fragmentation,spin-flip excitation quenching. B A P S A 27 697,AC10, Geesaman. NUCLEAR REACTIONS 2SMg(e,e'),E=140.1,191.8 MeV; m e a s u r e d a(0),transverse form factors. aSMg d e d u c e d I A S , J , v r , c o n f i g u r a t i o n , M 6 transition strengths. B A P S A 27 6 9 7 , A C l l , L i n d g r e n . NUCLEAR REACTIONS 3 ° s i , S 4 s , 4 a C a ( p o l a r i z e d p , p ) , ( p o l a r i z e d p , p ' ) , E = 6 5 0 , 8 0 0 MeV; m e a s u r e d a(0),analyzing p o w e r v s 0. 2SMg,aOsi,34S,4aCa l e v e l d e d u c e d n e u t r o n , p r o t o n matrix element r e l a t i v e s i g n . B A P S A 27 7 3 0 , E D 9 , M i s k i m e n . R A D I O A C T I V I T Y aSmAl(fl+),34Cl(fl+),3smK(fl+); m e a s u r e d T1/2. 47r c o n t i n u o u s gas f l o w c o u n t e r , on-line separated s o u r c e s . B A P S A 37 7 1 2 , C C 1 , K o s l o w s k y . NUCLEAR REACTIONS 2 5 M g ( p , 7 ) , ( p , p ' 7 ) , E = l . 6 - 2 . 7 MeV; m e a s u r e d a ( E , E 7 ) . 26Al d e d u c e d resonances. Enriched t a r g e t s , N a I ( T l ) d e t e c t o r s . CONF R i - g a , P 2 7 1 , K o p a n e t s . NUCLEAR REACTIONS 14N,26Mg(3He,t),E n o t g i v e n ; m e a s u r e d Q-value difference. 140,26mA1 deduced Q(EC),superallowed f l - d e c a y f t . B A P S A 27 6 9 6 , A C 4 , H a r d y . NUCLEAR REACTIONS 2SMg(p,n),E=134 MeV; m e a s u r e d a(En), a6A1 d e d u c e d I A S , G a m o w - T e l l e r (T>) component strength. B A P S A 27 7 3 1 , E E 3 , M a d e y . NUCLEAR REACTIONS 160(lzC,d),(laC,p),E(cm)=17.3 MeV; m e a s u r e d p T - , d 7 - c o i n , a~,aTAl d e d u c e d multipolarity,Tt/2. B A P S A 27 6 9 7 , A C 1 2 , S a w . NUCLEAR REACTIONS 3He(a~Mg,n),E n o t g i v e n ; m e a s u r e d 7n-coin,DSA,recoil. a6Si l e v e l s deduced T1/a,neutron,proton matrix e l e m e n t r a t i o . H i g h v e l o c i t y i o n r e c o i l i n A u . BAPSA 26 l 1 2 7 , B D l l , A l e x a n d e r . NUCLEAR REACTIONS a4,as,aSMg,a7Al(SHe,n),E=25 MeV; m e a s u r e d G ( E n ) , G ( 0 ) . aaSi d e d u c e d l e v e l s , aT,ZSSi,gSP d e d u c e d l e v e l s , L . B A P S A 26 l 1 2 7 , B D 9 , C r a i g .

A 27Na

=

ONLY)

=

28

R A D I O A C T I V I T Y 27,2s,29,3°,st,S2Na; m e a s u r e d E T , I T , 7 7 - c o i n . 33,34Na; m e a s u r e d E7,I% O n - l i n e mass spectroscopic source separation. REPT IPN 1980 A n n u a l , P N 3 2 , D e t r a z . R A D I O A C T I V I T Y 24,aSAl,140; m e a s u r e d f17 CP c o r r e l a t i o n asymmetry. 24Mg l e v e l s d e d u c e d isospin mixing,charge dependent matrix element. DABBB 42 4 8 4 8 , H o y l e . NUCLEAR REACTIONS 2 7 A l , l Z s S b ( n , 7 ) , E = t h e r m a l ; m e a s u r e d E7. aSAl d e d u c e d t r a n s i t i o n s . CONF Riga,P511,Kabina. NUCLEAR REACTIONS ~TAl(a,t),(a,SHe),E=64.5 MeV; m e a s u r e d G(0). aSSi,28A1 l e v e l s d e d u c e d S. Exact finite-range DWBA a n a l y s i s . REPT INS T o k y o 1980 A n n , P 2 2 , Y a s u e . NUCLEAR REACTIONS S L i , 1 2 c , 2 e s i ( n , p ) , E = 6 0 MeV; m e a s u r e d G(0=0°); deduced effective interaction p r o p e r t i e s . 6He,12B,aeA1 d e d u c e d g i a n t m a g n e t i c d i p o l e a n a l o g s . BAPSA 26 1128, BE5,Romero.

212

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A eSA1

R 81U1ZZ: 81WiZN:

aSSi

D 81HoZO:

R 79AcZZ: 80KnZW: 80PhZZ:

80RoZS: 80YaZT: 81CrZZ: 81CsZZ: 81FrZV: 81GeZW 81NeZW 81ScZO

81SnZY

81TaZS 81TaZV: 81ViZY

82DjZZ

82DoZZ 83FaZY

82GeZX 83HaZZ

82KaZZ

82MoZU: 820eZZ: 82ScZX: 82SnZZ:

=

28

ONLY)

continued

NUCLEAR REACTIONS 58,s°,62,64Ni,aSSi(n,p),E=59-6 MeV; m e a s u r e d ~;. ZSAI d e d u c e d GDR a n a l o g . Continuum model calculations. DABBB 42 1 9 3 3 , U l l m a n n . NUCLEAR REACTIONS 56Fe(n,T),E=27.7 keV; 58Ni(n,T),E=15.5 keV; 6°Ni(n,7),E=12.5 keV; ZTAl(n, v),E=34.7 keV; measured ET,1V. 57Fe,59,6tNi,aSA1 d e d u c e d s-wave resonance FT. REPT NEANDC(E)-222U,Vol V,P3,Wisshak. R A D I O A C T I V I T Y Z°Na,Z4AI,ZsP,aaCl,a6K,4°Sc; m e a s u r e d fl-delayed Ep,lp,Ea,Ia; deduced logft. 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J , ~ , T , ~ - r e d u e e d w i d t h s , e4Mg l e v e l s deduced J,~r,a-redueed widths. 3eS,asSi,36Ar,4°Ca l e v e l s d e d u c e d Jjr,F(~/Fp,p-,a-reduced w i d t h s . REPT J Y F L 1 7 / 8 1 , H o n k a n e n . NUCLEAR REACTIONS eTAl(p,a),E=850-1500 keV; m e a s u r e d ~(O). aSSi d e d u c e d r e s o n a n c e s , J j r , F , S. REPT Z F K - 3 8 5 , P 1 3 , A c h i l l e s . NUCLEAR REACTIONS eSSi(c~,c~'p),(a,2a),E=155 MeV; m e a s u r e d c~'p(O),~a(0), eSSi d e d u c e d T=0, GQR d e c a y m e c h a n i s m . P l a n e w a v e a n a l y s i s . REPT J U L - S p e z - 7 g , P 5 , K n o p f l e . NUCLEAR REACTIONS Z 8 S i ( p o l a r i z e d 6 L i , 6 L i ) , ( p o l a r i z e d 6Li,6Li'),E=22.8 MeV; m e a s u r e d or(0), iTt1(0). 28Si level deduced fie. Coupled-channels method,collective model. REPT ISN 80-01, P55,Pham. NUCLEAR REACTIONS Z4Mg,eSSi,SSNi(a,a'),E=104 MeV; measured or(0). Z4Mg,zasi,sSNi deduced T=0, dipole s t r e n g t h distribution,EWSR. DWBA a n a l y s i s . REPT KfK-3068,P43,Rost. NUCLEAR REACTIONS 27Al(a,t),(~,aHe),E=64.5 MeV; measured ~r(0). ZSSi,aSAI levels deduced S. Exact finite-range DWBA a n a l y s i s . REPT INS T o k y o 1980 A n n , P Z 2 , Y a s u e . NUCLEAR REACTIONS e 4 , a s , a 6 M g , e 7 A l ( 3 H e , n ) , E = 2 5 MeV; m e a s u r e d a(En),a(O), a6Si d e d u c e d l e v e l s . 27,eBSi,ZgP d e d u c e d l e v e l s , L . B A P S A 26 l 1 2 7 , B D 9 , C r a i g . NUCLEAR REACTIONS e 4 M g ( a , a ) , ( a , 7 ) , E < 5140 k e V ; m e a s u r e d ET,IT,7(0),
213

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A ZSSi

R 82TaZU: 82TaZW: 82UIZZ: 82WIZV:

Zep

D 81HoZ0:

R 82FaZY :

D 8ODeZE:

29Si

R 82WiZY:

Zgp

R 81CrZZ: 81MaZF:

82DjZZ:

82WiZY:

D 8ODeZE:

30Al

R 82ChZY

30Si

R 81MuZT

82MiZQ

820eZZ 82SaZZ 82SwZZ 82TaZU: 3Op

R 79KaYV: 82NeZT:

continued

=

29

R A D I O A C T I V I T Y 27,2a,av,a°,3z,aZNa; m e a s u r e d E T , 1 7 , 7 7 - c o i n . 33,34Na; m e a s u r e d E7,17. O n - l i n e mass spectroscopic source separation. REPT IPN 1980 A n n u a l , P N 3 2 , D e t r a z . NUCLEAR REACTIONS Z 7 A l ( p , t ) , ( p , 3 H e ) , a ' P ( p o l a r i z e d p,t),(polarized p,3He),E=6O MeV; measured ~(0). ZSMg,2SAl,ZgSi,zgP d e d u c e d p o s s i b l e h i g h l y e x c i t e d T = 3 / 2 s t a t e s . B A P S A 27 461,AYalS,Wilkerson. NUCLEAR REACTIONS z4,zs,Z6Mg,ZVAl(3He,n),E=25 MeV; m e a s u r e d ff(En),cr(0). ZSsi d e d u c e d l e v e l s , zT,aSSi,agP d e d u c e d l e v e l s , L . B A P S A 26 1 1 2 7 , B D 9 , C r a i g . NUCLEAR REACTIONS ZSSi,54Fe,SeNi(aHe,3He),(aHe,d),E=89.3 MeV; 9 ° Z r , i Z 4 S n ( a H e , 3 H e ) , ( a H e , d ) , E=89.8 MeV; m e a s u r e d (x(0). Zgp,SSCo,59Cu,S'Nb,lZsSb l e v e l s d e d u c e d C2S. F i n i t e - r a n g e DWBA analysis,nonlocal potentials. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 9 , M a t s u o k a . NUCLEAR REACTIONS ZTAl,~sSi(3He,d),E=13O MeV; m e a s u r e d q(0); deduced optical model parameters. ZSSi,zgP l e v e l deduced spectroscopic strength. DWBA a n a l y s i s . REPT JUL-Spez- 146,P7,Djaloeis. NUCLEAR REACTIONS a T A l ( p , t ) , ( p , 3 H e ) , U l P ( p o l a r i z e d p,t),(polarized p,aHe),E=60 MeV; measured (r(0). 2SMg,a5A1,29Si,zgP d e d u c e d p o s s i b l e h i g h l y e x c i t e d T = 3 / 2 s t a t e s . BAPSA 27 461,AYa15,Wilkerson.

A 30Na

28

NUCLEAR REACTIONS z4,eSMg(6Li,d),E=72.7 MeV; m e a s u r e d a ( E d ) , a ( 0 ) , as,3°Si l e v e l s d e d u c e d relative strengths. REPT INS T o y k o 1981 A n n , P 1 9 , T a n a b e . NUCLEAR REACTIONS Z4Mg(14N,l°B),E=129.1 MeV; m e a s u r e d a ( E ( * ° B ) ) , a ( 0 a , 0 ( i ° B ) , E ( * ° B ) ) . ZeSi deduced resonances. REPT RCNP 0 s a k a , 1 9 8 1 A n n , P 9 1 , T a k i m o t o . NUCLEAR REACTIONS 27AI(3He,d),E=44.8 MeV; m e a s u r e d a. ZSSi d e d u c e d l e v e l s i n GQR r e g i o n . B A P S A 27 4 9 3 , D X a 1 4 , U l l m a n n . NUCLEAR REACTIONS lZC(160,ZSO),E=lg.5-21 MeV; m e a s u r e d cr(0),a(E). 28Si d e d u c e d intermediate structure resonance,L,J,lr. Phase shift,S-matrix a n a l y s e s . DABBB 42 4 4 6 9 , Wilschut. R A D I O A C T I V I T Y 2°Na,Z4Al,ZaP,3zC1,36K,4°Sc; m e a s u r e d fl-delayed Ep,Ip,Ea,Ia; d e d u c e d l o g f t . 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n . ZONe l e v e l s d e d u e e d , J , r r , T , a - r e d u c e d w i d t h s , a4Mg l e v e l s deduced J,Ir,a-reduced widths. 32S,zsSi,3BAr,4°Ca l e v e l s d e d u c e d J,Tr,Fa/Fp,p-,a-reduced w i d t h s . REPT J Y F L 1 7 / 8 1 , H o n k a n e n . NUCLEAR REACTIONS Z e S i ( p o l a r i z e d p , n ) , E = 1 3 3 . 5 MeV; m e a s u r e d cr(O),A(O). ZaSi,zeP d e d u c e d parent,analog level excitation differences. Tof,natural target,inelastic data input. DWIA a n a l y s i s . B A P S A 27 629,14,Fazely.

A ZgNa

=

ONLY)

= 30

RADIOACTIVITY 27,28,29,3°,31,32Na; measured ET,I%77-coin. 33,34Na; measured E%17. On-line m a s s spectroscopic source separation. REPT IPN 1980 Annual,PN32,Detraz. NUCLEAR REACTIONS 14C(180,np),E=15-35 MeV; measured 77-,7(particle)-coin,7-yield. 3°AI deduced t r a n s i t i o n s . BAPSA 27 497,DYaLChitwood. NUCLEAR REACTIONS 3°Si(n,n),E ~ 183.2 keV; m e a s u r e d (;(total). 3°Si deduced potential s c a t t e r i n g r a d i u s . 31Si deduced resonance,Fn. Enriched target. BAPSA 26 ll40,CEl6, Mughabghab. NUCLEAR REACTIONS 3°Si,34S,42Ca(polarized p,p),(polarized p,p'),E=650,800 MeV; m e a s u r e d cT(0),analyzing power vs 0. e6Mg,3°Si,34S,42Ca level deduced n e u t r o n , p r o t o n m a t r i x e l e m e n t r e l a t i v e sign. BAPSA 27 730,ED9,Miskimen. NUCLEAR REACTIONS 3a,34S(d,6Li),E=80 MeV; measured G(0),~(E(SLi)). 28,U°Si levels deduced Sa. F i n i t e - r a n g e DWBA a n a l y s i s . REPT JUL-Spez-146,Pll,0elert. NUCLEAR REACTIONS 3°Si(a,a'),E=120 MeV; measured (~(0). 3°Si levels deduced deformation p a r a m e t e r , n e u t r o n , p r o t o n m a t r i x e l e m e n t sign. DWBA analysis. BAPSA 27 559,HXa2,Saha. NUCLEAR REACTIONS 'aC(ISO,a),E(cm)=lO-15 MeV; measured ~(0). 3°Si deduced resonances,large L c o n t r i b u t i o n s . BAPSA 27 699,AD10,Sweet. NUCLEAR REACTIONS a4,a6Mg(6Li,d),E=72.7 MeV; measured (7(Ed),cr(e). zs,3°Si levels deduced r e l a t i v e s t r e n g t h s . REPT INS Toyko 1981 Ann,Pl9,Tanabe. NUCLEAR REACTIONS ZgSi(p,7),(p,p'7),E=2605 keV; measured (T(ET,0). 3Op resonances deduced J,6. CONF Riga,P270,Kachan. NUCLEAR REACTIONS 29Si(p,p),(p,p'),E=l.29-3.31 MeV; measured o'(0). 30p deduced resonances, Jjr,Fp,Fp',IAS. M u l t i - c h a n n e l R - m a t r i x analysis. BAPSA 27 712,CC2,Nelson.

214

SECONDARY

SOURCES

(Reports,Abstracts,etc. ONLY)

A

3tNa

D

80DeZD:

80DeZE: 83DeZS: 3tMg

D 83DeZS:

3tSi

R 81MuZT:

31S

D

82AyZZ:

31CI

D

83AyZZ:

D 80DeZE: 83DeZS:

3ZMg

D 83DeZS:

32p

R 80MAZE:

3z S

D 81HoZO:

R

8OTaZN: 81Bugv: 81FrZV: 81TaZS: 81TaZV: 81ViZY

82BaZW 83MoZU 32C1

D 81HoZO

R

8ORoZR

D

33 S

R 83JuZZ:

80DeZE:

=

32

RADIOACTIVITY z7,ae,zo,a°,al,aaNa; m e a s u r e d E T , I T , 7 7 - c o i n . 33,34Na; m e a s u r e d E7,I7. O n - l i n e m a s s s p e c t r o s c o p i c s o u r c e s e p a r a t i o n . REPT IPN 1980 A n n u a l , P N 3 3 , D e t r a z . RADIOACTIVITY 3aNa(fl-),alNa(fl-) [ f r o m lr(p,X),E=10 GeV]; m e a s u r e d Qfl. 31,3ZMg d e d u c e d m a s s e x c e s s . REPT I P N O - D R E - 8 2 - 1 4 , D e t r a z . RADIOACTIVITY 3ZNa(fl-),31Na(fl-) [ f r o m Ir(p,X),E=i0 GeV]; m e a s u r e d Qfl. 31,3aMg d e d u c e d m a s s e x c e s s . REPT I P N O - D R E - 8 3 - 1 4 , D e t r a z . NUCLEAR REACTIONS lSO,tZC,a4S(polarized d,a),E=52 MeV; m e a s u r e d itl1(8 ). l°B,azP,ION l e v e l s deduced L,J,Tr,stretched configuration. DWBA a n a l y s i s . REPT K f K - 3 0 6 8 , P a O , M a i r l e . RADIOACTIVITY a°Na,a4Al,ZoP,SZCl,aSK,4°Sc; m e a s u r e d f l - d e l a y e d E p , I p , E a , l a ; d e d u c e d l o g f t . 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , d j r , T , a - r e d u c e d w i d t h s , a4Mg l e v e l s deduced Jjr,a-reduced w i d t h s . 3aS,28Si,3OAr,4°Ca l e v e l s d e d u c e d J j r , F a / P p , p - , a - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . NUCLEAR REACTIONS ZSSi(OLi,d),E=75.8 MeV; m e a s u r e d ~(Ed),a(O). 32S l e v e l s d e d u c e d S. E x a c t f i n i t e r a n g e DWBA. REPT INS T o k y o 1980 A n n , P a S , T a n a b e . NUCLEAR REACTIONS 3ZS(e,e'),E=34-74 MeV; m e a s u r e d f o r m f a c t o r s . 3zS t r a n s i t i o n s d e d u c e d multipolarity. BAPSA 36 l 1 3 8 , B E 4 , B u r t . NUCLEAR REACTIONS 160(160,160),E(em)=25-40 MeV; lZC(160,iOO'),E(cm)=lT-47 MeV; m e a s u r e d a(E); d e d u c e d e x i t c h a n n e l s t r u c t u r e , aZS,asSi d e d u c e d r e s o n a n c e s . DABBB 42 1 0 8 7 , F r e e m a n . NUCLEAR REACTIONS tz,laC(Z°Ne,X),E=140 MeV; m e a s u r e d a ( E a ) . 3aS,zsSi d e d u c e d r e s o n a n c e s . BAPSA 36 l 1 3 3 , C B 1 3 , T a k a h a s h i . NUCLEAR REACTIONS la,13C,14N,loO,Z°Ne(leo,a),E=145 MeV; m e a s u r e d cr(Ea), aeSi,3ZS,aOAr d e d u c e d r e s o n a n c e s . BAPSA 36 7 9 0 , H X 7 , T a k a h a s h i . NUCLEAR REACTIONS a4Mg,aSSi,aZS(n,n),(n,n'),E=9.76,14.83 MeV; m e a s u r e d a(O). Z4Mg,aSSi,aaS d e d u c e d d e f o r m a t i o n p a r a m e t e r s y s t e m a t i c s . C o u p l e d - c h a n n e l s a n a l y s i s . REPT 1SN 81-01,P50, Virdis. NUCLEAR REACTIONS 3 z , a O S ( l r - j r - ) , E = 5 0 MeV; m e a s u r e d a(O). 3a,3SS d e d u c e d neutron distribution r a d i u s d i f f e r e n c e . O p t i c a l m o d e l a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 4 0 , B a r n e t t . NUCLEAR REACTIONS ~aC,leO(Z°Ne,c~),E=Sa,80,117 MeV; m e a s u r e d ~ ( E a ) . OOSi,aZS d e d u c e d possible high-spin s t a t e s . REPT INS T o k y o 1981 A n n , P 3 0 , M o r i t a . RADIOACTIVITY a°Na,Z4Al,zap,aZcI,36K,4°Sc; m e a s u r e d f l - d e l a y e d E p , l p , E a , l a ; d e d u c e d l o g f t . 4°Sc d e d u c e d ~ - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J , ~ , T , a - r e d u c e d w i d t h s . Z4Mg l e v e l s deduced Jjr,a-reduced w i d t h s . 3aS,oaSi,36Ar,4°Ca l e v e l s d e d u c e d J , ~ r , F a / F p , p - , a - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . NUCLEAR REACTIONS 3ZS(aHe,t),E=34.5 MeV; m e a s u r e d cT(0),~(Et); 3zCl d e d u c e d l e v e l s , J , ~ . REPT IPN 1980 A n n u a l , P N 8 , R o s i e r .

A 33Na

31

RADIOACTIVITY 31Na [ f r o m o n - l i n e m a s s s p e c t r o s c o p y ] ; m e a s u r e d f i T - c o i n ; d e d u c e d u p p e r limit for fl-delayed three-neutron emission probability. REPT IPN 1980 A n n u a l , P N 3 3 , Detraz. R A D I O A C T I V I T Y a?,za,zg,a°,al,aZNa; m e a s u r e d E T , I T , 7 7 - c o i n . 3a,34Na; m e a s u r e d E7,17. O n - l i n e m a s s s p e c t r o s c o p i c s o u r c e s e p a r a t i o n . REPT IPN 1980 A n n u a l , P N 3 3 , D e t r a z . R A D I O A C T I V I T Y 3ZNa(fl-),a*Na(fl-) [ f r o m Ir(p,X),E=10 GeV]; m e a s u r e d Qfl. al,aaMg d e d u c e d m a s s excess. REPT IPNO-DRE-82-14,Detraz. RADIOACTIVITY 3ZNa(fl-),SlNa(fl-) [ f r o m Ir(p,X),E=lO GeV]; m e a s u r e d Qfl. 31,3aMg d e d u c e d m a s s e x c e s s . REPT I P N O - D R E - 8 3 - 1 4 , D e t r a z . NUCLEAR REACTIONS 3 ° S i ( n , n ) , E ~ 183.3 k e V ; m e a s u r e d a ( t o t a l ) . 3°Si d e d u c e d p o t e n t i a l scattering radius. 3iSi d e d u c e d resonance,Fn. Enriched t a r g e t . BAPSA 36 1140,CE16, Mughabghab. RADIOACTIVITY 31CI [ f r o m 3ZS(p,Zn),E=33 MeV]; m e a s u r e d f l - d e l a y e d Ep,lp,T,/z. 3~S deduced l e v e l , I f l . REPT JYFL 1981 A n n , P 3 4 , A y s o t o . RADIOACTIVITY 3tCI [ f r o m 3aS(p,3n),E=33 MeV]; m e a s u r e d f l - d e l a y e d Ep,lp,Tt/a. 31S d e d u c e d l e v e l , I f l . REPT JYFL 1981 A n n , P 3 4 , A y s o t o .

A

3ZNa

=

=

33

RADIOACTIVITY z7,zs,zo,a°,al,aZNa; m e a s u r e d E T , I T , 7 7 - c o i n . 3a,a4Na; m e a s u r e d E7,I7. O n - l i n e m a s s s p e c t r o s c o p i c s o u r c e s e p a r a t i o n . REPT IPN 1980 A n n u a l , P N 3 2 , D e t r a z . NUCLEAR REACTIONS 3ZS(n,n),E=640-750 keV; m e a s u r e d y i e l d s . 33S d e d u c e d r e s o n a n c e s , L , P n , strength f u n c t i o n s . O p t i c a l m o d e l a n a l y s i s . REPT N E A N D C ( E ) - 2 3 2 U , V o l l l I , P a 6 , J u n g m a n n .

2]5

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 34Na

D 80DeZE:

34 S

R 82MiZQ:

34C1

D 82KoZT:

R 82CaZV:

D

36 S

D 82HiZW:

3SAt

82HiZW:

R

8gBaZW:

D

81HoZ0:

R 81TaZV: as K

D 80AyZZ:

81HoZ0:

3SCa

D 80AyZZ:

D 828tZT:

37C1

D 82StZT:

37AF

R 81RaZ0: 83SaZU:

37 K

R 82SaZU:

D 82KoZT:

=

36

=

37

RADIOACTIVITY 378(•-) [from 368(n,,/)3; m e a s u r e d 7-/-coin. 37C1 d e d u c e d level,J,rr, -/-branching. REPT L A - 9 3 8 1 - P R , P 8 7 , S t a r n e r . RADIOACTIVITY 37S(fl-) [ f r o m 3SS(n,,/)3; m e a s u r e d - / / - / - c o i n . 37C1 d e d u c e d level,J,rr, -/-branching. REPT L A - 9 3 8 1 - P R , P 8 7 , S t a r n e r . NUCLEAR REACTIONS 3vCl(p,n),E=120 MeV; m e a s u r e d a ( E n ) , a ( 8 ) . 3~Ar d e d u c e d G a m o w - T e l l e r strength function. Tof,CaaYcla t a r g e t . BAPSA 26 l 1 2 7 , B D 1 4 , R a p a p o r t . NUCLEAR REACTIONS l S O , 4 ° C a ( a , p ~ ) , ( a , d a ) , ( a , t a ) , ( a , 3 H e a ) , ( a , g a ) , E = 1 3 9 . 2 MeV; 160,4°Ca(p,gp), (p,pd),(p,pt),E= 101.3 MeV; 4 °Ca (p,2p),(p,pd),(p,pt),E=76.1 MeV; measured (particle)(particle)-coin,a(E,,E2,OpSa). 15,14,13N,as,ae,37K,lac,a~Ar l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a . NUCLEAR REACTIONS 1 6 0 , 4 ° C a ( a , p ~ ) , ( a , d a ) , ( a , t a ) , ( a , a H e a ) , ( a , 2 a ) , E = 1 3 9 . 2 MeV; 160,4°Ca(p,3p), (p,pd),(p,p t),E= 101.3 MeV; 4 °Ca (p,2p),(p,pd),(p,pt),E = 76.1 MeV; measured (particle)(particle)-coin,a(E,,Ea,Ol,Oa). 15,14,13N,39,3s,37K,IaC,aYAr l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a .

A as K

35

RADIOACTIVITY 36p [ f r o m 37Cl(n,2p),E=70 MeV]; m e a s u r e d E,/,l,/,T1/a,,/,/-eoin; d e d u c e d log ft, Ifl. 36p l e v e l d e d u c e d 7 r , p o s s i b l e J , c o n f i g u r a t i o n . 3SS d e d u c e d l e v e l s , , / - b r a n c h i n g , p o s s i b l e J,Tr. REPT J U L - S p e z - 1 4 6 , P 4 3 , H i l l . RADIOACTIVITY 3Sp [ f r o m 37Cl(n,2p),E=70 MeV3; m e a s u r e d E,/,I,/,Tl/2,,/,/-coin; d e d u c e d log ft, Ifl. 3Sp l e v e l d e d u c e d ~ r , p o s s i b l e J , c o n f i g u r a t i o n . ass d e d u c e d l e v e l s , , / - b r a n c h i n g , p o s s i b l e J,w. REPT J U L - S p e z - 1 4 6 , P 4 3 , H i l l . NUCLEAR REACTIONS 32,3SS(Tr-,w-),E=50 MeV; m e a s u r e d ~(0). 32,3°S d e d u c e d neutron distribution r a d i u s d i f f e r e n c e . O p t i c a l m o d e l a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 4 0 , B a r n e t t . RADIOACTIVITY 20Na,24A1,2SP,32Cl,3SK,4°Se; m e a s u r e d f l - d e l a y e d Ep,Ip,Ea,I(~; d e d u c e d l o g f t . 4OSe d e d u c e d f l - s t r e n g t h f u n c t i o n . 2°Ne l e v e l s d e d u e e d , J , T r , T , a - r e d u c e d w i d t h s . 24Ms l e v e l s deduced J,~r,a-reduced w i d t h s . 32S,assi,aSAr,4°Ca l e v e l s d e d u c e d J , ~ r , F ( x / F p , p - , ( x - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . NUCLEAR REACTIONS 12,13C,14N,mO,a°Ne(lSO,c~),E=145 MeV; m e a s u r e d a(Ea). ZSSi,3aS,36Ar d e d u c e d r e s o n a n c e s . BAPSA 26 7 9 0 , H X 7 , T a k a h a s h i . RADIOACTIVITY aSCa [ f r o m 40Ca(3He,3na),E=95 MeV]; 3SK [ f r o m 4°Ca(3He,2npa),E=95 MeV3; m e a s u r e d f l - d e l a y e d Ep,Ip; d e d u c e d d,e c o e f f i c i e n t s of i s o b a r i c m a s s m u l t i p l e t equation. 3SK d e d u c e d m a s s e x c e s s . REPT JYFL 1980 A n n , P 2 8 , A y s t o . RADIOACTIVITY 20Na,24A1,2Sp,32C1,3SK,4°Sc; m e a s u r e d f l - d e l a y e d Ep,Ip,E(x,la; d e d u c e d l o g f t . 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n . 2°Ne l e v e l s d e d u c e d , J , ~ , T , a - r e d u c e d w i d t h s . 24Ms l e v e l s d e d u c e d J , ~ r , ( x - r e d u c e d w i d t h s , a2s,2SSi,3SAr,4OCa l e v e l s d e d u c e d J , T r , F ( ~ / F p , p - , ( x - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . RADIOACTIVITY 36Ca [ f r o m 40Ca(3He,3na),E=95 MeV'l; 3SK [ f r o m 4°Ca(3He,2np(~),E=95 MeV]; m e a s u r e d f l - d e l a y e d Ep,lp; d e d u c e d d,e c o e f f i c i e n t s o f i s o b a r i c m a s s m u l t i p l e t equation. 3SK d e d u c e d m a s s e x c e s s . REPT JYFL 1980 A n n , P 2 6 , A y s t o .

A 3~S

=

NUCLEAR REACTIONS 34S(n,n),E=0.02-1450 keV; m e a s u r e d (~(total). 35S d e d u c e d s - , p - , d - w a v e resonances,parameters,doorway characteristics. R-matrix,doorway state calculations. BAPSA 27 7 1 2 , C C 3 , C a r l t o n .

A 36p

34

RADIOACTIVITY 27,28,2g,a°,al,agNa; m e a s u r e d E , / , I % , / , / - c o i n . 33,34Na; m e a s u r e d E,/,I,/. O n - l i n e m a s s s p e c t r o s c o p i c s o u r c e s e p a r a t i o n . REPT IPN 1980 A n n u a l , P N 3 2 , D e t r a z . NUCLEAR REACTIONS aOsi,34S,42Ca(polarized p , p ) , ( p o l a r i z e d p , p ' ) , E = 6 5 0 , 8 0 0 MeV; m e a s u r e d a ( 0 ) , a n a l y z i n g p o w e r v s 0. eSMg,s°si,a4s,42Ca l e v e l d e d u c e d n e u t r o n , p r o t o n matrix element r e l a t i v e s i g n . BAPSA 27 7 3 0 , E D 9 , M i s k i m e n . RADIOACTIVITY eSmAl(fl+),aaCl(fl+),asmK(fl+); m e a s u r e d T1/a. 4~r c o n t i n u o u s gas f l o w c o u n t e r , on-line s e p a r a t e d s o u r c e s . BAPSA 27 7 1 2 , C C 1 , K o s l o w s k y .

A as S

=

ONLY)

RADIOACTIVITY on-line

separated

=

38

Al(fl + ), 34 Cl(fl + ), 3 8 m K(fl + ); m e a s u r e d Tt/a. 4~r c o n t i n u o u s s o u r c e s . BAPSA 27 7 1 2 , C C 1 , K o s l o w s k y .

26m

216

gas f l o w c o u n t e r ,

SECONDARY

SOURCES

(Repor[s,Abs[racts,etc. ONLY)

A 38 K

R 82SaZU:

NUCLEAR REACTIONS (p,pd),(p,pt),E=101.3

R

8ZSaZU:

R 81BaZM:

82AjZX: 82BaZZ:

4OCa

D 81HoZN: 81HoZ0:

J

81AnZR:

R 80DeZH: 81BaZQ:

81DjZR:

81LuZZ: 82GaZS: 82ReZZ:

82ZwZY:

49Sc

D 81HoZN: 81HoZ0:

82HoZV: R 81BaZM:

81TaZT:

continued

MeV; 160,4°Ca(p,2p), 4°Ca(p,3p),(p,pd),(p,pt),E=76.1 MeV; measured (particle)(particle)-coin,a(E~,Ea,Ot,Oa). ~5,14,13N,ag,as,37K,laC,37Ar l e v e l s d e d u c e d S. DWlA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a . MeV;

=

39

NUCLEAR REACTIONS ~60,4°Ca(c~,pa),(a,da),(c~,ta),(a,3Hea),(a,Ea),E=139.E MeV; ~60,46Ca(p,Ep), (p,pd),(p,pt),E= 101.3 MeV; 4 °Ca(p,ip),(p,pd),(p,pt),E= 76.1 MeV; measured (particle)(partiele)-coin,a(E~,Ea,01,0a). ~5,14,13N,aa,3~,37K,~aC,37Ar l e v e l s d e d u c e d S. DWIA, factorization approximation. Quasifree,nonquasifree g e o m e t r y . DABBB 42 3 7 3 7 , S a m a n t a .

A 40 K

38

~60,4°Ca(a,pa),(¢x,da),(a,ta),(a,3Hea),(a,2a),E=139.3

A 39 K

=

=

40

NUCLEAR REACTIONS 4°Ca(TT+,Tr°),(Tr-,Tr°),E=164 MeV; m e a s u r e d a(O). 4°Sc,4°K d e d u c e d analogs. Distorted wave eikonal model,sum rule normalization,Goldhaber-Teller transition density. BAPSA 26 l 1 2 4 , B C 6 , B a e r . NUCLEAR REACTIONS 4°,4a,44Ca,46,48,S°Ti,54Cr,Sd,S6,SSFe,7°Zn(t,3He),E=35 MeV; m e a s u r e d c~(0). 4o 42,44K,46,48,5°Sc,54V,54,56,58Mn,TOCu d e d u c e d l e v e l s . BAPSA 27 7 3 i , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR REACTIONS 4°Ca(~r+,~°),(~r-,Tr°),E=164 MeV; m e a s u r e d a(E(~)),cr(0). 4°K,4%c d e d u c e d IAS. D i s t o r t e d wave eikonal model,Goldhaber-Teller transition density,sum rule normalization. BAPSA 27 509,EF10,Baer. R A D I O A C T I V I T Y 4°Sc [ f r o m 4°Ca(p,n)]; m e a s u r e d f l - d e l a y e d Ep,Ea,Ip,Ia,Tl/2; d e d u c e d log ft, fl-strength function; 4°Ca d e d u c e d l e v e l s , F a / F p , J , T r , T . REPT JYFL R R - 2 0 / 8 1 , H o n k a n e n . R A D I O A C T I V I T Y a°Na,a4A1,2Sp,32Cl,3SK,4°Sc; m e a s u r e d f l - d e l a y e d E p , I p , E a , I a ; d e d u c e d l o g f t . 4°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J , ~ , T , ( x - r e d u c e d w i d t h s , a4Mg l e v e l s deduced J,zr,a-reduced w i d t h s . 3aS,28Si,36Ar,4°Ca l e v e l s d e d u c e d J,~r,Fa/Fp,p-,a-reduced w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; m e a s u r e d h f s , i s o t o p e s h i f t . 41,42,43,444546,47, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 1 9 1 , A n d l . NUCLEAR REACTIONS 4°Ca(aHe,3He'),E=108.5 MeV; m e a s u r e d a(0),a(E(3He)). 4°Ca d e d u c e d g i a n t monopole strength distribution. REPT ISN 8 0 - 0 1 , P 4 4 , d e S a i n t i g n o n . NUCLEAR REACTIONS l,aH,laC,4°Ca(p,p'),E=800 MeV; m e a s u r e d a ( 0 p ' ) v s p r o t o n m o m e n t u m ; deduced quasielastic processes, laC,dOCa d e d u c e d cr(quasielastic),a(reaction). REPT L A - 8 7 6 8 - P R , P 2 4 , B a r l e t t. NUCLEAR REACTIONS 4OCa,51V,SS,6o,6aNi,68Zn,9°,ga,94,96Zr,ga,94,a6,gs,l°°Mo,la°,la4Sn,14°Ce(p,p'), E=201 MeV; m e a s u r e d a ( E p ' ) . 49Ca,SlV,SS,6°,6aNi,68Zn,9°,ga,94,96Zr,ga,9%96,gs,~°°Mo,la°,la4Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 4°Ca(a,a'p),(a,2a),E=130 MeV; m e a s u r e d cr(Ea'),a(Oa),a(Op). 4°Ca d e d u c e d giant resonance particle decay characteristics. BAPSA 26 I129,BE12,Lui. NUCLEAR REACTIONS 4°,4a,44,4eCa(p,p'),E=200 MeV; m e a s u r e d cr(0),cr(Ep'). 4°,42,44,4~Ca d e d u c e d spin-flip M1 t r a n s i t i o n enhancement. DWBA a n a l y s i s . BAPSA 27 7 3 2 , E E 9 , G a l o n s k y . NUCLEAR REACTIONS 4 ° C a ( p o l a r i z e d p,2p),12C,180(polarized p,2d),E=150 MeV; m e a s u r e d cr(E 1, E2). 4°Ca d e d u c e d s t r o n g l y b o u n d p r o t o n s h e l l e f f e c t s . ~2C,~60 d e d u c e d d e u t e r o n c l u s t e r effects. Energy-sharing,quasifree g e o m e t r i e s . DWIA a n a l y s i s . BAPSA 37 509,EF8,Rees. NUCLEAR REACTIONS 49Ca(a,2a),(a,pcx),E=120 MeV; m e a s u r e d aa(O),pa(Ù). 4°Ca d e d u c e d m o n o p o l e s t r e n g t h , E W S R . DWBA,PWBA a n a l y s e s . K i n e m a t i c a l l y c o m p l e t e e x p e r i m e n t . REPT KVI 1981 A n n , P 6 , Z w a r t s . RADIOACTIVITY a°se [ f r o m 4°Ca(p,n)]; m e a s u r e d f l - d e l a y e d Ep,Ea,lp,Ia,Tl/a; d e d u c e d log ft, fl-strength function; 4°Ca d e d u c e d l e v e l s , P a / F p , J , T r , T . REPT JYFL R R - 2 0 / 8 1 , H o n k a n e n . RADIOACTIVITY 2°Na,adAl,28P,a2Cl,a~K,~°Sc; m e a s u r e d f l - d e l a y e d E p , I p , E a , I a ; d e d u c e d l o g f t . ~°Sc d e d u c e d f l - s t r e n g t h f u n c t i o n , a°Ne l e v e l s d e d u c e d , J j r , T , a - r e d u c e d w i d t h s , aaMg l e v e l s deduced J,~r,a-reduced w i d t h s , aaS,asSi,a~Ar,4°Ca l e v e l s d e d u c e d J , ~ r , F c ~ / F p , p - , a - r e d u c e d w i d t h s . REPT JYFL 1 7 / 8 1 , H o n k a n e n . RADIOACTIVITY 4°Sc; m e a s u r e d f l - d e c a y s t r e n g t h f u n c t i o n ; d e d u c e d s t r u c t u r e . H i g h - l y i n g l e v e l f l - d e l a y e d p a r t i c l e d e c a y i n ~°Ca. REPT JYFL 1981 A n n , P 3 7 , H o n k a n e n . NUCLEAR REACTIONS 4°Ca(Tr+,Tr%,(~-,~rO),E=164 MeV; m e a s u r e d a(0). 4°Sc,4gK d e d u c e d a n a l o g s . Distorted wave eikonal model,sum rule normalization,Goldhaber-Teller transition density. BAPSA 26 l 1 2 4 , B C 6 , B a e r . NUCLEAR REACTIONS ~°Ca(aHe,t),(aHe,3He'),E=200 MeV; m e a s u r e d a(Et),o'(E(3He')),cr(0). 4°Sc d e d u c e d a n a l o g , G a m o w - T e l l e r r e s o n a n c e . High p u r i t y s t a c k e d Ge d e t e c t o r s . BAPSA ~6 11~9, BEll,Tabor.

217

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 4OSc

R

82BaZZ:

82NaZY:

J

80AnZF:

81AnZR: R

80FoZX:

81FoZW:

R 82AjZX:

42Ca

J

80AnZF:

81AnZR: R 82GaZS: 82MiZQ:

42Sc

D 80HoZ0: R 82NaZY:

42Ti

D 80HoZ0:

J

80AnZF:

81AnZR:

R 82AjZX:

44Ca

J

80AnZF:

81AnZR: R 82GaZS: 82KuZU:

41

=

42

=

43

NUCLEAR MOMENTS 41,42,43,44,45,4s,47,48Ca; measured isotope shifts,hfs; deduced hyperfine c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT K f K - 3 0 6 8 , P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; m e a s u r e d h f s , i s o t o p e s h i f t . 41,424344,45,4647, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 1 9 1 , A n d l .

A 44 K

=

NUCLEAR REACTIONS 4°,42,44Ca,4S,4S,5OTi,a4Cr,54,ss,SSFe,T°Zn(t,aHe),E=25 MeV; m e a s u r e d a(0). 40 42,44K,4S,4S,5°Se,54V,54,5°,58Mn,~°Cu d e d u c e d l e v e l s . BAPSA 27 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR MOMENTS 41,42,43,44,45,4s,47,48Ca; measured isotope shifts,hfs; deduced hyperfine c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT K f K - 3 0 6 8 , P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; m e a s u r e d h f s , i s o t o p e s h i f t . 41,4243,4445,46,47, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 l g l , A n d l . NUCLEAR REACTIONS 4°,42,44,48Ca(p,p'),E=200 MeV; m e a s u r e d a(0),a(Ep'). 4°,42,44,4SCa d e d u c e d spin-flip M1 t r a n s i t i o n enhancement. DWBA a n a l y s i s . BAPSA 27 7 3 2 , E E 9 , G a l o n s k y . NUCLEAR REACTIONS 3 ° S i , 3 4 S , 4 2 C a ( p o l a r i z e d p , p ) , ( p o l a r i z e d p , p ' ) , E = 6 5 0 , 8 0 0 MeV; m e a s u r e d a ( 0 ) , a n a l y z i n g p o w e r v s 0. aaMg,3°Si,34S,42Ca l e v e l d e d u c e d n e u t r o n , p r o t o n matrix element r e l a t i v e s i g n . BAPSA 27 7 3 0 , E D g , M i s k i m e n . RADIOACTIVITY 42Ti [ f r o m 4°Ca(3He,n),E=15 MeV]; m e a s u r e d ET,I~; d e d u c e d log f t . 42Sc deduced transitions,fl-branching. REPT JYFL 1980 A n n , P 2 8 , H o n k a n e n . NUCLEAR REACTIONS 4°,42,44,4eCa(p,n),E=120 MeV; m e a s u r e d a ( E n ) , a ( 0 ) . 40,42,44,4SSc d e d u c e d Gamow-Teller s t r e n g t h . Tof. BAPSA 27 5 1 0 , E F l l , N a r a y a n a s w a m y . RADIOACTIVITY 42Ti [ f r o m 4°Ca(aHe,n),E=15 MeV]; m e a s u r e d ET,I~/; d e d u c e d log f t . 42Sc deduced transitions,fl-branching. REPT JYFL 1980 A n n , P 2 8 , H o n k a n e n .

A 43Ca

continued

NUCLEAR MOMENTS 41,42,43,44,45,46,47,4Sea; measured isotope shifts,hfs; deduced hyperfine c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT KfK-3068, P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,48,47,4SCa; measured h f s , i s o t o p e s h i f t . 4i,4a,43,44,45,4a,47, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 1 9 1 , A n d l . NUCLEAR REACTIONS 4°Ca(a,SHe),E=36 MeV; m e a s u r e d a(0). 41Ca deduced c o r e - p a r t i c l e c o u p l i n g multiplets. Split-pole spectrometer. Coupled-channels a n a l y s i s . REPT IPN 1980 A n n u a l , PN42,Fortier. NUCLEAR REACTIONS 4°Ca(a,3He),E=36 MeV; m e a s u r e d a(E(SHe),0). 4*Ca d e d u c e d levels,L,S. DWBA,coupled-channel a n a l y s e s . E n r i c h e d t a r g e t . REPT I P N O - P h N - 8 1 - 1 1 , F o r t i e r .

A 42 K

40

NUCLEAR REACTIONS 40Ca(~r+,lro),(Tr-,~rO),E=164 MeV; m e a s u r e d a(E(Tr)),a(0). 46K,4°Sc d e d u c e d IAS. D i s t o r t e d wave eikonal model,Goldhaber-Teller transition density,sum rule normalization. BAPSA 27 5 0 9 , E F l 0 , B a e r . NUCLEAR REACTIONS 40,4a,44,48Ca(p,n),E=120 MeV; m e a s u r e d a ( E n ) , a ( 0 ) . 4°,42,44,48Sc d e d u c e d Gamow-Teller s t r e n g t h . Tof. BAPSA 27 5 1 0 , E F l l , N a r a y a n a s w a m y .

A 41Ca

=

ONLY)

=

44

NUCLEAR REACTIONS 4°,42,44Ca,46,48,5°Ti,54Cr,54,56,58Fe,7°Zn(t,3He),E=25 MeV; m e a s u r e d a(0). 4o 42,44K,4S,48,S°Sc,S4v,54,so,SSMn,7°Cu d e d u c e d l e v e l s . BAPSA 27 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR MOMENTS 41,42,43,44,45,46,47,48Ca; measured isotope shifts,hfs; deduced hyperfine c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT KFK-3068, P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; m e a s u r e d h f s , i s o t o p e s h i f t . 41,42,43,44,45,46,47, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 1 9 1 , A n d l . NUCLEAR REACTIONS 4°,42,44,48Ca(p,p'),E=200 MeV; m e a s u r e d a ( 0 ) , a ( E p ' ) . 4°,42,44,4SCa d e d u c e d spin-flip M1 t r a n s i t i o n enhancement. DWBA a n a l y s i s . BAPSA 27 7 3 2 , E E 9 , G a l o n s k y . NUCLEAR REACTIONS 44,4SCa,4S,47,48,49,5°Ti(d,t),E=5.8-10 MeV; m e a s u r e d a(0). 44,48Ca,4S,47, 4s, 49,50Ti d e d u c e d lfT/~ n e u t r o n o r b i t a l r m s r a d i u s . DWBA a n a l y s i s . DABBB 42 4 4 6 8 , K u t t .

218

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 44Sc

R

81GrZW:

82NaZY: 44Ti

D 82FrZW: R 82TaZT: 82WiZU:

J

80AnZF:

81AnZR: R 81QaZY:

45Sc

R 81ShZQ: B2AvZZ:

45Ti

R 82AvZZ:

J

80AnZF:

81AnZR:

46Sc

R 83AjZX:

4STi

R 81BeZT: 82KuZU: 82WiZU:

J

80AnZF:

81AnZR: 47Ti

R 82KuZU:

47CF

R 83HaZH:

J

80AnZF:

45

=

46

=

47

NUCLEAR MOMENTS 41,42,43,44,45,46,47,48Ca; m e a s u r e d i s o t o p e s h i f t s , h f s ; d e d u c e d h y p e r f i n e c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT K f K - 3 0 6 8 , P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; measured hfs,isotope shift. 4142,4344,4546,47, 48Ca deduced r m s charge radii. Laser spectroscopy. REPT ZfK-3191,Andl. NUCLEAR REACTIONS 44,4SCa,46,47,48,49,S°Ti(d,t),E=5.8-10 MeV; measured a(0). 44,48Ca,46,4v,48, 49,5°Ti deduced IfT/a n e u t r o n orbital r m s radius. DWBA analysis. DABBB 42 4468,Kutt. NUCLEAR REACTIONS 4°Ca(laC,ha),46Ti(3He,2n),E not given; measured "}"/-coin. 47Cr deduced levels. REPT ANL-81-79,P83,Hardie.

A 48Ca

=

NUCLEAR MOMENTS 41,4a,43,44,45,46,47,48Ca; measured isotope shifts,hfs; deduced hyperfine constants. Atomic beam induced resonance fluorescence,tunable dye lasers. REPT KfK-3068, P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; measured hfs,isotope shift. 41,42,43,444546,47, 48Ca deduced r m s charge radii. Laser spectroscopy. REPT ZfK-3191,Andl. NUCLEAR REACTIONS 4°,42,44Ca,46,48,5°Ti,54Cr,54,ss,58Fe,V°Zn(t,3He),E=25 MeV; measured a(0). 40, 42,44K,46,4s,5°Sc,54V,54,56,SSMn,V°Cu deduced levels. BAPSA 27 731,EE4,Ajzenberg-Selove. NUCLEAR REACTIONS 5°,SaCr(d,SLi),E=65 MeV; measured a(0),a(E(SLi)). 46,48Ti levels deduced r e l a t i v e S. REPT J U L - S p e z - 9 9 , P 2 7 , B e t i g e r i . NUCLEAR REACTIONS 44,48Ca,46,47,48,49,5°Ti(d,t),E=5.8-10 MeV; m e a s u r e d a(O). 44,4SCa,4S,47,4s, 4s,5°Ti d e d u c e d l f v / 2 n e u t r o n o r b i t a l r m s r a d i u s . DWBA a n a l y s i s . DABBB 42 4 4 6 8 , K u t t . NUCLEAR REACTIONS 4°,42Ca(a,X),E n o t g i v e n ; m e a s u r e d E2,I 7. 44,46Ti d e d u c e d c o n t i n u u m i s o s p i n m i x i n g . BAPSA 27 706,BD1,Wiggins,

A 47Ca

continued

NUCLEAR MOMENTS 41,42,43,44,45,46,47,48Ca; m e a s u r e d i s o t o p e s h i f t s , h f s ; d e d u c e d h y p e r f i n e c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT KfK-3068, P55,Andl. NUCLEAR MOMENTS 4°,41,42,43,44,45,46,47,48Ca; m e a s u r e d h f s , i s o t o p e s h i f t . 41,424344,45,4647, 4SCa d e d u c e d r m s c h a r g e r a d i i . L a s e r s p e c t r o s c o p y . REPT Z f K - 3 1 9 1 , A n d l . NUCLEAR REACTIONS 4 4 C a , 4 9 T i , S ° C r , S V , S S Z n , 9 e Z r , S V , a S M o ( n , d ) , ( n , n ' p ) , ( n , n p ) , E = 1 4 . 7 MeV; m e a s u r e d a; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,SlCr,Sa,69Zn,SSZr,98,99Mo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 2 3 2 U , V o l V , P a 0 , Q a i m . NUCLEAR REACTIONS 4 4 C a ( p , p ' 7 ) , E = 2 . 2 5 - 3 . 0 1 MeV; m e a s u r e d a ( 0 p ' ) , 7 ( 0 ) . 45Sc d e d u c e d resonances,J,rr,L,channel correlations. H i g h r e s o l u t i o n . BAPSA 26 1 2 2 2 , F D l l , S h r i n e r , J r . . NUCLEAR REACTIONS 4SSc(p,p'7),45Sc,51V,SSMn(p,nT),E=4.2,4.4,5 MeV; m e a s u r e d T(0),DSA. 45Sc, 45Ti,SlCr,55Fe l e v e l s d e d u c e d T 1 / 2 , J , 8 , B ( k ) , r o t a t i o n a l b a n d s . BAPSA 27 4 9 7 , D Y a 2 , A v a s t h i . NUCLEAR REACTIONS 45Sc(p,p'7),4SSc,SlV,55Mn(p,nT),E=4.3,4.4,5 MeV; m e a s u r e d "y(0),DSA. 4%c, 45Ti,SiCr,SSFe l e v e l s d e d u c e d T l / a , J , 6 , B ( k ) , r o t a t i o n a l b a n d s . BAPSA 27 4 9 7 , D Y a 2 , A v a s t h i .

A 46Ca

44

NUCLEAR REACTIONS i 8 0 ( 2 9 S i , 2 n p ) , E = 3 0 - 9 9 MeV; m e a s u r e d E7,I2. 44rn,44Se l e v e l s d e d u c e d population ratio. Evaporation model analysis,microscopic "y-decay calculation,fixed quadrupole to d i p o l e e m i s s i o n s t r e n g t h s . CONF 1 8 l s t ACS Mtg,NUCL 5 5 , G r o a n i n g . NUCLEAR REACTIONS 4°,42,44,48Ca(p,n),E=120 MeV; m e a s u r e d cr(En),a(O). 49,42,44,49Se d e d u c e d Gamow-Teller s t r e n g t h . Tof. BAPSA 27 5 1 0 , E F l l , N a r a y a n a s w a m y . R A D I O A C T I V I T Y 44Ti; m e a s u r e d T1/~. Decay r a t e , i s o t o p e c o n c e n t r a t i o n r a t e t e c h n i q u e s . BAPSA 27 7 1 2 , C C 4 , F r e k e r s . NUCLEAR REACTIONS 4°Ca(%i,d),E=75.8 MeV; m e a s u r e d a(Ed),a(0). 44Ti levels d e d u c e d Sa. Q2D spectrograph. Finite-range DWBA. REPT INS T o k y o 1981 A n n , P 2 1 , T a n a b e . NUCLEAR REACTIONS 4°,4aCa(a,X),E n o t g i v e n ; m e a s u r e d ET,I 7. 44,46Ti d e d u c e d c o n t i n u u m i s o s p i n m i x i n g . BAPSA 27 706,ED1,Wiggins.

A 45Ca

=

ONLY)

=

48

NUCLEAR MOMENTS 41,4a,43,44,45,46,47,48Ca; m e a s u r e d i s o t o p e s h i f t s , h f s ; d e d u c e d h y p e r f i n e c o n s t a n t s . A t o m i c b e a m i n d u c e d r e s o n a n c e f l u o r e s c e n c e , t u n a b l e d y e l a s e r s . REPT K f K - 3 0 6 8 , P55,Andl.

219

SECONDARY SOURCES ( R e p o r t s , A b s t r a c t s , e t c .

A 48Ca

J 81AnZR R 80PeZT

82BeZQ

82GaZS: 82ImZZ:

8eKuZU: 82PeZZ:

48Sc

R 82AjZX: 82NaZY:

48Ti

R 81BeZT: 82KuZU:

=

48

ONLY)

continued

NUCLEAR MOMENTS 40,41,42,43,44,45,46,47,48Ca; measured hfs,isotope s h i f t . 414243,44 4546,47 48Ca deduced r m s charge radii. Laser spectroscopy. REPT ZfK-3191,Andl. NUCLEAR REACTIONS 48Ca,SOTi,52Cr((x,a),(a,~'),E=104 MeV; m e a s u r e d a(0); deduced optical potential c h a r a c t e r i s t i c s . 4SCa,S°Ti,52Cr deduced n e u t r o n d i s t r i b u t i o n radii d i f f e r e n c e s . REPT KfK-3068,P35,Pesl. NUCLEAR REACTIONS 48Ca(p,p'),E=44.4 MeV; m e a s u r e d cr(e),(x(Ep'). 48Ca deduced strong I + state excitation. Microscopic DWBA analysis. High resolution magnetic spectrometer. REPT JUL-Spez-146,Pi,Berg. NUCLEAR REACTIONS 4o,42,44,4SCa(p,p'),E=200 MeV; measured a(e),cr(Ep'). 4°,42,44,48Ca deduced s p i n - f l i p MI t r a n s i t i o n e n h a n c e m e n t . DWBA a n a l y s i s . BAPSA 27 732,EEg,GaIonsky. NUCLEAR REACTIONS 48Ca,S°Ti,52Cr,54Fe(p,p'),E=65 IVreV; m e a s u r e d a(Ep'),cr(e). 48Ca,5°Ti,SaCr, 54Fe deduced r e l a t i v e 1+ s p i n - f l i p s t r e n g t h . REPT RCNP 0saka,1981 Ann,P43,1manishi. NUCLEAR REACTIONS 44,48Ca,46,47,48,4g~5°Ti(d,t),E=5.8-10 MeV; measured a(0). 44,4~Ca,46,47,48, 49,5°Ti deduced IfT/2 n e u t r o n orbital r m s r a d i u s . DWBA analysis. DABBB 4~ 4468,Kutt. NUCLEAR REACTIONS 5°Ti,52Cr((x,(x),(~x,(x'),E=104 MeV; m e a s u r e d (7(0); deduced potential m o m e n t s , m a t t e r d i s t r i b u t i o n s . 48Ca,SOTi,SaCr deduced isotonic d i f f e r e n c e s Fourier-Bessel m e t h o d , v i b r a t i o n a l model. REPT KfK-3242,Pesl. NUCLEAR REACTIONS 48,4~,44Ca,46,48,S°Ti,54Cr,54,se,SSFe,7°Zn(t,aHe),E=R5 MeV; measured (;(0). 4o 4~,~4K,46,4°,5°Se,54V,54,56,SSMn,V°Cu deduced levels. BAPSA 27 731,EE4,Ajzenberg-Selove. NUCLEAR REACTIONS 4°,4~,44,4°Ca(p,n),E=120 MeV; measured a(En),a(0). 4°,4~,44,4SSc deduced Gamow-Teller s t r e n g t h . Tof. BAPSA 27 510,EFll,Narayanaswamy. NUCLEAR REACTIONS 5°,52Cr(d,6Li),E=65 MeV; measured ~r(0),a(E(6Li)). 46,48Ti levels deduced r e l a t i v e S. REPT JUL-Spez-99,P27,Betigeri. NUCLEAR REACTIONS 44,48Ca,46,47,4s,4°,5°Ti(d,t),E=5.8-10 MeV; measured a(0). 44,4~Ca,4~,47,4°, 4°,5°Ti deduced IfT/~ n e u t r o n orbital r m s r a d i u s . DWBA analysis. DABBB 42 4468,Kutt.

A = 49 4OTi

R

82BeZT: 82KuZU:

40 V

R

79AnZP: 82ShZS:

49Cr

R 79AnZP:

NUCLEAR REACTIONS 48Ca(a,an),E=30-55 MeV; measured y(e),yy-coin,a(Ey,E). ~gTi deduced levels,T~/2,y-branching,6,configurations.REPT INDC(ARG)-9/G,Pb5,Behar. NUCLEAR REACTIONS 44,48Ca,46,4v,48,4°,5°Ti(d,t),E=5.8-10 MeV; measured ~;(0). ~4,48Ca,46,47,4s, 4°,5°Ti deduced ifT/2 n e u t r o n orbital r m s r a d i u s . DWBA a n a l y s i s . DABBB 42 4468,Kutt. NUCLEAR REACTIONS 46,48Ti(a,ny),(~,py),E=13.8,g4.2 MeV; m e a s u r e d (r(ET,0). 49V,49,StCr t r a n s i t i o n s deduced Aa,A4. Enriched targets,Ge(Li) detectors. CONF Riga,P331,Antropov. NUCLEAR REACTIONS 4 S T i ( p , p ' 7 ) , E = 2 . 2 - 3 . 1 MeV; m e a s u r e d (~(0p'),lT(~),77-coin. 4°V resonances deduced inelastic decay amplitude relati.ve magnitude,sign. Statistical t h e o r y . BAPSA 27 7 1 2 , C C 5 , S h r i n e r , J r . . NUCLEAR REACTIONS 4 B , 4 8 T i ( a , n T ) , ( a , p T ) , E = 1 3 . 8 , 2 4 . 2 MeV; m e a s u r e d a(E%O). 4°V,4°,mlCr transitions d e d u c e d A2,A 4. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . CONF R i g a , P 3 3 1 , A n t r o p o v .

A 5OSc

R 82AjZX:

5OTi

R 80PeZT:

81QaZY:

82ImZZ: 82KuZU: 82PeZZ:

5o V

R

5OCr

R 82YaZW:

82YaZW:

=

50

NUCLEAR REACTIONS 4°,42,44Ca,46,4s,5°Ti,54Cr,54,56,58Fe,7°Zn(t,aHe),E=25 MeV; m e a s u r e d a(O). 40, 42,44K,4%4s,5°Sc,54V,54,56,5SMn,7°Cu d e d u c e d l e v e l s . BAPSA 27 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR REACTIONS 4 S C a , 5 ° T i , S a C r ( ~ , a ) , ( a , ~ ' ) , E = 1 0 4 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l potential characteristics. 4°Ca,5°Ti,5~Cr d e d u e b d n e u t r o n distribution radii differences. REPT K f K - 3 0 6 8 , P 3 5 , P e s l . NUCLEAR REACTIONS 4 4 C a , 4 9 T i , 5 ° C r , 6 7 , 6 8 Z n , 9 2 Z r , 9 7 , 9 8 M o ( n , d ) , ( n , n ' p ) , ( n , n p ) , E = 1 4 . 7 MeV; m e a s u r e d a; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,51Cr,6e,S%n,gaZr,gS,ggMo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 2 2 2 U , V o I V , P 3 0 , Q a i m . NUCLEAR REACTIONS 4SCa,5°Ti,52Cr,54Fe(p,p'),E=65 MeV; m e a s u r e d a ( E p ' ) , a ( 0 ) . 48Ca,5°Ti,SaCr, 54Fe d e d u c e d r e l a t i v e l + s p i n - f l i p strength. REPT RCNP Osaka,1981 A n n , P 4 3 , I m a n i s h i . NUCLEAR REACTIONS 44,48Ca,46,47,48,49,5°TJ(d,t),E=5.8-10 MeV; m e a s u r e d a(0). 44,48Ca,46,47,48, 4g,5°Ti deduced IfT/2 n e u t r o n orbital r m s r a d i u s . DWBA analysis. DABBB 42 4468,Kutt. NUCLEAR REACTIONS 5°Ti,SaCr((x,a),(cx,a'),E=104 MeV; m e a s u r e d ~r(S); deduced p o t e n t i a l m o m e n t s , m a t t e r d i s t r i b u t i o n s . 4SCa,5°Ti,52Cr deduced isotonic d i f f e r e n c e s Fourier-Bessel m e t h o d , v i b r a t i o n a l model. REPT KfK-3242,Pesl. NUCLEAR REACTIONS 52Cr(p,t),(p,aHe),E=65 MeV; m e a s u r e d (r(Et),~(E(aHe)),~(0); deduced reaction mechanism. 5°V,5°Cr deduced analog state excitation differences. REPT RCNP Osaka, 1981 Ann,P69,Yamazaki. NUCLEAR REACTIONS S2Cr(p,t),(p,3He),E=65 MeV; m e a s u r e d a(Et),ff(E(aHe)),(;(O); deduced reaction mechanism. 5°V,S°Cr deduced analog state excitation differences. REPT RCNP Osaka, 1981 Ann,P69,Yamazaki.

220

SECONDARY

SOURCES

(Repor[s,Abst~raets,etc.

A at V

R 81BaZL: 81DjZR:

5~Cr

R 79AnZP: 8IQaZY:

82AvZZ StMn

R 82WhZZ

=

ONLY)

51

NUCLEAR REACTIONS SlV(e,e'a),E=38,150 MeV; m e a s u r e d a c t i v i t y . 51V l e v e l s d e d u c e d d i p o l e dominance for a-decay. B A P S A R6 l 1 2 9 , B E 8 , B a r b e r . NUCLEAR REACTIONS 4°Ca,SZV,Sa,~°,eaNi,SaZn,S°,~z,~4,~Zr,aZ,~4,gs,gs,~OOMo,~Zo,~Z~Sn,~OCe(p,p,), E = 2 0 1 MeV; m e a s u r e d cr(Ep'). 4°Ca,5~v,Sa,6°,~Ni,~SZn,~0,~z,~4,9~Zr,~Z,94 q~,~s,~0~Mo t a o , ~ 4 S n deduced M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N f S , D j a l a l i . NUCLEAR REACTIONS 48,4~Ti(a,n-~),(c~,pS,),E=:13.8,34.3 MeV; m e a s u r e d cr(E'~,0). 4~V,a~,StCr transitions d e d u c e d As,A4. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r s . CONF R i g a , P 3 3 1 , A n t r o p o v . NUCLEAR REACTIONS 44Ca,4aTi,5°Cr,67fiSZn,9~Zr,97,gaMo(n,d),(n,n'p),(n,np),E=14.7 MeV; measured or; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,SICr,Sa,6%n,a3Zr,~S,~gMo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 3 2 3 U , V o l V , P 3 0 , Q a i m . NUCLEAR REACTIONS 45Sc(p,p'7),45Sc,5iV,55Mn(p,nT),E=4.2,4.4,5 MeV; m e a s u r e d 3~(0),DSA. ~SSc, 45Ti,5~Cr,55Fe l e v e l s d e d u c e d T ~ / ~ , J , t ~ , B ( X ) , r o t a t i o n a l b a n d s . B A P S A 27 4 9 7 , D Y a 3 , A v a s t h i . NUCLEAR REACTIONS 5 ° C r ( p , p ' 7 ) , E = 3 . 0 5 - 4 . 3 8 MeV; m e a s u r e d a t 0 ) , 7 ( 0 ). 5~Mn d e d u c e d resonances,Jdr. B A P S A 27 4 9 7 , D Y a 3 , W h a t l e y .

A = 52 5ZCr

R 80PeZT

821mZZ 82PeZZ

5ZMn

D BODeZA R 81YaZU

5ZFe

D 80DeZA R 8IYaZU

NUCLEAR REACTIONS 48Ca,5°Ti,SZCr(c~,(x),(a,a'),E=104 MeV; m e a s u r e d or(0); d e d u c e d o p t i c a l potential characteristics. 4SCa,5°Ti,52Cr d e d u c e d n e u t r o n distribution radii differences. REPT K f K - 3 0 6 8 , P 3 5 , P e s l . NUCLEAR REACTIONS 48Ca,5°Ti,SZCr,54Fe(p,p'),E=65 MeV; m e a s u r e d ¢r(Ep'),a(8). 4~Ca,5°Ti,52Cr, 54Fe d e d u c e d relative l + spin-flip strength. REPT RCNP 0 s a k a , 1 9 8 1 A n n , P 4 3 , 1 m a n i s h i . NUCLEAR REACTIONS 5 ° T i , S Z C r ( a , a ) , ( a , c ~ ' ) , E = 1 0 4 MeV; m e a s u r e d ¢y(0); d e d u c e d potential moments,matter distributions. 4~Ca,5°Ti,SZCr d e d u c e d i s o t o n i c d i f f e r e n c e s Fourier-Bessel method,vibrational m o d e l . REPT K f K - 3 2 4 3 , P e s l . R A D I O A C T I V I T Y 5ZmFe E f r o m ZVAl(sZs,2npa),E=13OMeV]; m e a s u r e d flT'y-coin,Efl+; d e d u c e d i s o m e r J,Tr. 5ZMn l e v e l s d e d u c e d T 1 / z , 7 - b r a n c h i n g . R E P T IPN 1980 A n n u a l , P R 6 , D e l l a Negra. NUCLEAR REACTIONS 5 4 F e ( p , t ) , ( p , 3 H e ) , E = 6 5 MeV; m e a s u r e d or(0). SZMn,aZPe l e v e l s d e d u c e d enhancement f a c t o r s . D W B A , t w o - s t e p p r o c e s s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 7 9 , Y a m a z a k i . R A D I O A C T I V I T Y 52mFe E f r o m 27AI(3zS,Snpa),E=130 MeVS; m e a s u r e d fl%,'~-coin,Efl+; d e d u c e d i s o m e r J,rr. 5ZMn l e v e l s d e d u c e d T l / z , ~ / - b r a n c h i n g . REPT IPN 1980 A n n u a l , P R 6 , B e l l a Negra. NUCLEAR REACTIONS 5 4 F e ( p , t ) , ( p , a H e ) , E = 6 5 MeV; m e a s u r e d a ( 0 ) . 5ZMn,SZFe l e v e l s d e d u c e d enhancement f a c t o r s . D W B A , t w o - s t e p p r o c e s s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 7 9 , Y a m a z a k i .

A 53Cr

R 82AgZZ:

53Mn

R 79KIZS: 79K1ZZ: 81PuZZ: 83PuZX:

~3Fe

R 82FuZY:

=

53

NUCLEAR REACTIONS 5z,S~Cr(n,n),E=10-900 keV; measured a(total) vs E. 53,55Cr deduced s-, p - w a v e resonances,J,Tr,Fn,level s p a c i n g , n e u t r o n r e d u c e d w i d t h d i s t r i b u t i o n s . Tof. R-matrix a n a l y s i s . B A P S A 27 7 1 6 , C E e , A g a r w a l . NUCLEAR REACTIONS 5ZCr(p,p'7),(p,~]),E=4140-4B00 keV; measured atE). 5aMn deduced iAR,gg/ 3-fragrnentation. REPT Z F K - 3 8 5 , P l l , K l e i n w a c h t e r . NUCLEAR REACTIONS 5eCr(p,p),(p,p'),E=4597,4688 keV; m e a s u r e d n o t g i v e n . 5aMn d e d u c e d IAR, S. REPT Z F K - 3 8 5 , P 1 0 , K l e i n w a c h t e r . NUCLEAR REACTIONS 54,56,SaFe(d,SHe),E=80 MeV; m e a s u r e d cr(0),a(E(aHe)). 53,55,57Mn d e d u c e d levels,CZS,configuration. REPT J U L - S p e z - 9 9 , P 1 8 , P u t t a s w a m y . NUCLEAR REACTIONS 54,56,SaFe(d,aHe),E=80 MeV; m e a s u r e d (7(E(aHe)),a(0). 53,55,57Mn l e v e l s d e d u c e d S. DWBA a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 9 , P u t t a s w a m y . NUCLEAR REACTIONS 56Fe(aHe,SHe),E=l10,130 MeV; m e a s u r e d atE(SHe)). 5ape l e v e l s d e d u c e d relative excitation proability. REPT RCNP 0 s a k a , 1 9 8 1 A n n , P 7 4 , F u j i w a r a .

A = 54 54 V

R 82AjZX:

NUCLEAR REACTIONS 4°,42,44Ca,46,4a,5°Ti,54Cr,5%56,SeFe,7°Zn(t,SHe),E=25 Me"C; m e a s u r e d cr(0). 40 deduced levels. RAPSA 27 731,EE4,Ajzenberg-Selove. NUCLEAR REACTIONS 4°,42,44Ca,46,4s,5°Ti,54Cr,54,56,SaFeT°Zn(t,SHe),E=25 MeV; measured ~(e). 4o 42,44K,46,48,5°Sc,54V,54,so,58Mn,7°Cu deduced levels. BAPSA 27 731,EE4,Ajzenberg-Selove. NUCLEAR REACTIONS leC,54,56,SeFe,SS,e°,62Ni,64 ~6 6s,7OZn(a,~),(a,~,),E=29,40,45,50 MeV; m e a s u r e d (r(E,e). 1~C,54,56,SaFe,5a,6o62Ni,64,66,sSTOZn deduced d e f o r m a t i o n p a r a m e t e r ft. Blair phase m e t h o d . CONF Riga,P330,Pavlova. NUCLEAR REACTIONS 54Fe,84,SSZn(p,p'),E=6.9 MeV; measured ET,17,1(ce),Tl/z,interna] pair s u m coincidence. 54Fe,64fiaZn levels deduced B(E0)/B(ES),E0 decay b r a n c h i n g . REPT JYFL 1980 Ann,P31,Passoja.

42,44K,4s,48,5°Sc,S4v,54,56,58Mn,7°Cu

54Mn

R 83AjZX

54Fe

R 79PaZO

80PaZM

221

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 54Fe

R 81EIZY: 82GuZY: 82ImZZ: 82NoZZ:

R 82AgZZ:

~5Mn

R 81PuZZ: 82PuZX:

55Fe

R 8aAvZZ:

55Co

R 81MaZF:

R 82AjZX:

5BFe

R 79PaZO:

80BeYS:

81EIZY: 82CuZY: 82PaZW: 56Co

D 82LeZT: 82LeZX: R 81NaZ0:

56Ni

R 81BeZG: 81DuZU:

R 81PuZZ: 82PuZX:

57Fe

D 82EIZY:

R 81KaZM:

=

55

=

56

NUCLEAR REACTIONS 4°,42,44Ca,4a,4s,5°Ti,54Cr,54,56,58Fe,7°Zn(t,aHe),E=25 MeV; m e a s u r e d a(0). 40 42,44K,46,48,5°Sc,54V,54,5e,~SMn,~°Cu d e d u c e d l e v e l s . B A P S A 37 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR REACTIONS 1 2 C , 5 4 , 5 6 , 5 S F e , S S , s ° , e 2 N i , 6 4 , e 6 , s a , 7 ° Z n ( ~ , a ) , ( a , a ' ) , E = 2 9 , 4 0 , 4 5 , 5 0 MeV; measured a(E,O), laC,5%56,58Fe,SS,6°,62Ni,64,a6,6s,7°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS 5s,6°,aa,64Ni,64,s6,68,T°Zn(*4c,tSO),E=72 MeV; m e a s u r e d a(E(160)),cr(O). 6aFe, 6aNi d e d u c e d m a s s e x c e s s . 56,s8,6°,6aFe,6a,64,66,68Ni l e v e l s d e d u c e d S d e p e n d e n c e on neutron number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 9 , B e r n a s . NUCLEAR REACTIONS 5 4 , 5 6 F e , 6 a , 6 5 C u ( n , n ) , ( n , n ' ) , E = 1 4 MeV; m e a s u r e d or(0). 54,S~Fe,6a,SSCu d e d u c e d fla- O p t i c a l m o d e l , c o u p l e d - c h a n n e l s a n a l y s i s . DABBB 42 1 9 3 1 , E I - K a d i . NUCLEAR REACTIONS 54,56Fe,SeNi,la°Sn,a°sPb(polarized n , n ' ) , E = 1 0 MeV; m e a s u r e d A(0). 54,56Fe, ~6Ni,'~°Sn,e°sPb l e v e l d e d u c e d s p i n - o r b i t deformation parameters. BAPSA 27 542,GYa2,Guss. NUCLEAR REACTIONS 5 6 F e , 6 6 Z n ( p , p ' 7 ) , E = 5 - 9 MeV; m e a s u r e d E T , 1 7 , p T - c o i n , l ( c e ) . 56Fe,S6Zn d e d u c e d E0 t r a n s i t i o n strength. R E P T JYFL 1981 A n n , P 5 2 , P a s s o j a . R A D I O A C T I V I T Y 5aCo(fl+),56Co(fl+); m e a s u r e d f l - a s y m m e t r y ; d e d u c e d F e r m i , C a m o w - T e l l e r d e c a y mixing r a t i o . B A P S A 27 713,CC8,Lee. R A D I O A C T I V I T Y 58,56Co; m e a s u r e d lfl(O),V(0),oriented n u c l e i ; d e d u c e d F e r m i to G a m o w - T e l l e r mixing r a t i o s . DABBB 42 3 7 3 7 , L e e . NUCLEAR REACTIONS 58,6°,6aNi(polarized d,a),E=80 MeV; m e a s u r e d v e c t o r a n a l y z i n g p o w e r v s O. 56,58,66Co l e v e l s d e d u c e d J,~r. B A P S A 26 l 1 3 6 , C D 5 , N a n n . NUCLEAR REACTIONS aasi(aeSi,28Si),(aSSi,aSSi'),E=105-121 MeV; m e a s u r e d or(E). 56Ni d e d u c e d intermediate structure. B A P S A 26 l 1 3 3 , C B 1 5 , B e t t s . NUCLEAR REACTIONS ~ a N i , n 6 S n , e ° s P b ( a , a H e ) , E = 2 1 8 MeV; m e a s u r e d a(O),a(E(6He)). 56Ni,li4Sn, a ° 6 P b d e d u c e d l e v e l s . REPT IPN 1981 A n n u a I , P N 7 1 , O u h a m e l .

A 57Mn

continued

NUCLEAR REACTIONS 5 a , a 4 C r ( n , n ) , E = 1 0 - 9 0 0 keV; m e a s u r e d a ( t o t a l ) v s E. 5a,55Cr d e d u c e d s - , p-wave resonances,J,rc,Fn,level spacing,neutron reduced width distributions. Tof. R-matrix a n a l y s i s . B A P S A 27 7 1 6 , C E 6 , A g a r w a l . NUCLEAR REACTIONS 54,5s,SaFe(d,3He),E=80 MeV; m e a s u r e d o'(0),q(E(aHe)). 53,s5,SVMn d e d u c e d levels,C~S,configuration. REPT J U L - S p e z - 9 9 , P 1 8 , P u t t a s w a m y . NUCLEAR REACTIONS 54,56,5eFe(d,3He),E=80 MeV; m e a s u r e d o(E(aHe)),(7(0). 53,55,57Mn l e v e l s d e d u c e d S. DWBA a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 9 , P u t t a s w a m y . NUCLEAR REACTIONS 45Sc(p,p'7),4SSc,SlV,SSMn(p,nT),E=4.2,4.4,5 MeV; m e a s u r e d 7(0),DSA. 4SSc, 45Ti,51Cr,SSFe l e v e l s d e d u c e d T ~ / ~ , J , ( ~ , B ( X ) , r o t a t i o n a l b a n d s . B A P S A 27 4 9 7 , D Y a 2 , A v a s t h i . NUCLEAR REACTIONS aeSi,S4Fe,SeNi(3He,aHe),(aHe,d),E=89.3 MeV; 9 ° Z r , i a 4 S n ( 3 H e , a H e ) , ( 3 H e , d ) , E=89.8 MeV; m e a s u r e d (~(0). U~P,SSCo,S~Cu,mNb,lasSb l e v e l s d e d u c e d CaS. F i n i t e - r a n g e DWBA analysis,nonlocal potentials. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 9 , M a t s u o k a .

A 56Mn

54

NUCLEAR REACTIONS s 4 , 5 6 F e , a 3 , 6 5 C u ( n , n ) , ( n , n ' ) , E = 1 4 MeV; m e a s u r e d a ( 0 ) . 54,5~Fe,S3,~SCu d e d u c e d fla. O p t i c a l m o d e l , c o u p l e d - c h a n n e l s a n a l y s i s . DABBB 4~ 1 9 3 1 , E 1 - K a d i . NUCLEAR REACTIONS 5~,SSFe,5SNi,~a°Sn,~°ePb(polarized n , n ' ) , E = 1 0 MeV; m e a s u r e d A(O). 54,S6Fe, 58Ni,~°Sn,a°aPb level deduced spin-orbit deformation parameters. BAPSA 27 5 4 2 , G Y a 2 , C u s s . NUCLEAR REACTIONS 4SCa,5°Ti,Sacr,S~Fe(p,p'),E=65 MeV; m e a s u r e d ~ ( E p ' ) , ~ ( 0 ) . 4SCa,S°Ti,~aCr, 54Fe d e d u c e d r e l a t i v e 1+ s p i n - f l i p strength. REPT RCNP O s a k a , 1 9 8 1 A n n , P 4 3 , I m a n i s h i . NUCLEAR REACTIONS 45Sc(Z~C,np),E=40 MeV; m e a s u r e d 7(O),T7(t),DSA. 54Fe d e d u c e d levels,J,rr, isomer feeding strength,7-multipolarity. B A P S A 27 4 9 8 , D Y a 4 , N o e .

A 55Cr

--

ONLY)

=

57

NUCLEAR REACTIONS 54,ss,56Fe(d,3He),E=80 MeV; m e a s u r e d a(O),a(E(aHe)), sa,s5,57Mn d e d u c e d levels,C2S,configuration. REPT J U L - S p e z - 9 9 , P 1 8 , P u t t a s w a m y . NUCLEAR REACTIONS 54,56,SSFe(d,3He),E=80 MeV; m e a s u r e d a(E(UHe)),(7(0), sa,55,S7Mn l e v e l s d e d u c e d S. DWBA a n a l y s i s . REPT J U L - S p e z - 1 4 6 , P 9 , P u t t a s w a m y . R A D I O A C T I V I T Y 57mFe; m e a s u r e d 77(0,H,t); deduced electric field gradient. 57Fe l e v e l d e d u c e d Tt/a. 57Fe t r a n s i t i o n d e d u c e d 6 ( E 2 / M 1 ) , s u b s h e l l ICC r a t i o . FeTiH(X) l a t t i c e . DABBB 42 3317,E1 F i q i . NUCLEAR REACTIONS 56,58Fe(n,7),E=10-100 keV; m e a s u r e d a(E). 57,5SFe r e s o n a n c e s d e d u c e d FT. Activation technique. REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 , K a p p e l e r .

222

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 57Fe

R 81KoZP: 81WiZN:

57Co

R 79HeZS:

57Ni

R 80DjZY: 80OhZX:

R 82AjZX:

5~Fe

R 79PaZO:

89BeYS:

58Co

D 82LeZT: 82LeZX: R 81NaZ0:

5SNi

R 79PaZO:

80KnZV: 80RoZS: 81BuZU:

81DjZR:

81DjZZ:

82GuZY: 58Cu

R

82AnZV: 82RaZQ:

R 81KaZM:

59Co

R 79PiZO:

59Ni

R 81WiZN:

82HaZQ:

continued

=

58

NUCLEAR REACTIONS 4°,42,44Ca,46,de,5°Ti,SdCr,Sd,SS,SaFe,7°Zn(t,aHe),E=25 MeV; m e a s u r e d a(0). 40 4e,44K,dS,48,5°Sc,54V,54,ss,58Mn,7°Cu d e d u c e d l e v e l s . B A P S A 27 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR REACTIONS 1 Z C , S d , 5 6 , 5 8 F e , S S , S ° , 8 2 N i , 6 4 , s s , s e , 7 ° Z n ( a , ( x ) , ( a , ( ~ ' ) , E = 2 9 , 4 0 , 4 5 , 5 9 MeV; measured a ( E , 0 ) . 12C,54,56,58Fe,58,B°,62Ni,Sd,66,ss,7°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 O , P a v l o v a . NUCLEAR REACTIONS 58,6°,sa,64Ni,84,ss,ss,7°Zn(14C,160),E=72 MeV; m e a s u r e d a(E(160)),a(0). SeFe, SBNi d e d u c e d m a s s e x c e s s . 56,58,6°,6~Fe,62,sd,68,68Ni l e v e l s d e d u c e d S d e p e n d e n c e on neutron number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 9 , B e r n a s . R A D I O A C T I V I T Y 58Co(fl+),SSCo(fl+); m e a s u r e d f l - a s y m m e t r y ; d e d u c e d F e r m i , G a m o w - T e l l e r d e c a y mixing r a t i o . B A P S A 27 713,CC8,Lee. R A D I O A C T I V I T Y 5s,SSCo; m e a s u r e d Ifl(O),y(O),oriented n u c l e i ; d e d u c e d F e r m i to G a m o w - T e l l e r mixing r a t i o s . DABBB 4 2 3 7 3 7 , L e e . NUCLEAR REACTIONS 5s,s°,SZNi(polarized d,~),E=8O MeV; m e a s u r e d v e c t o r a n a l y z i n g p o w e r v s 9. 56,58,6°Co l e v e l s d e d u c e d J,Tr. B A P S A 26 l 1 3 6 , C D 5 , N a n n . NUCLEAR REACTIONS 12C,Sd,se,58Fe,SS,s°,62Ni,64,sa,sa,T°Zn(a,a),(a,a'),E=29,40,45,50 MeV; measured a ( E , 0 ) . 12C,54,56,5SFe,Sa,6°,S~Ni,~4,as,ss,7°Zn d e d u c e d deformation parameter fl. Blair phase method. CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS 5s,seNi(a,c~'),(a,a'p),((x,2a),E=155 MeV; m e a s u r e d a ( E c ~ ' ) , a ( x - , ( x p - c o i n . 5s S~Ni d e d u c e d T=0,GQR d e c a y c h a r a c t e r i s t i c . REPT J U L - S p e z - Y 2 , P 6 , K n o p f l e . NUCLEAR REACTIONS a4Mg,a~Si,SSNi(a,a'),E=104 MeV; m e a s u r e d a(0). adMg,eSSi,SeNi d e d u c e d T=0, dipole strength distribution,EWSR. DWBA a n a l y s i s . REPT K f K - 3 0 6 8 , P 4 3 , R o s t . NUCLEAR REACTIONS 5 e N i ( n , n ) , ( n , n ' ) , E = O . 9 - 4 . 5 MeV; m e a s u r e d a(0),a(total). 5SNi l e v e l deduced excitation mechanism. Optical,statistical,coupled-channels m o d e l s . REPT A N L / NDM-61,Budtz-Jorgensen. NUCLEAR REACTIONS 4°Ca,5~v,SS,6°,6aNi,~SZn,9°,9~,94,gaZr,~a,e4,~,~8,~°°Mo,~a°,~a4Sn,l~°Ce(p,p'), E = 2 0 1 MeV; m e a s u r e d a(Ep'). ~°Ca,5~V,SS,s°,SZNi,S~Zn,gO,e~,~,S°Zr,~,94,ss,~s,~°°Mo,ie°,l~dSn d e d u c e d MI r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 8 , D j a l a l i . NUCLEAR REACTIONS 5SNi(aHe,aHe),(aHe,aHe'),E=130 MeV; m e a s u r e d (7(0). 5aNi l e v e l s d e d u c e d L, fl2,fl4,giant resonance,EWSR. Optical model,DWBA analyses,complex coupling. REPT JU L - S p e z - 9 9 , P 3 , D j a l o e i s . NUCLEAR REACTIONS 54,5SFe,SSNi,l~°Sn,a°aPb(polarized n,n'),E=10 MeV; m e a s u r e d A(0). 54,5SFe, 58Ni,~°Sn,a°ePb level deduced spin-orbit deformation parameters. BAPSA 27 5 4 2 , G Y a 2 , G u s s . NUCLEAR REACTIONS N i ( p , n ) , E = 1 3 4 MeV; m e a s u r e d cr(En). 58,6°,sa,64Cu d e d u c e d levels, Gamow-Teller isospin fragmentation. B A P S A 27 7 3 1 , E E 8 , A n a n t a r a m a n . NUCLEAR REACTIONS 58Ni(p,n),E=120,160 MeV; m e a s u r e d a(O). 5~Cu d e d u c e d levels,L, Gamow-Teller strength splitting. B A P S A 27 7 3 1 , E E 6 , R a p a p o r t .

A 5eFe

57

NUCLEAR REACTIONS 56Fe(n,-~),E=5-80 keV; m e a s u r e d E%I% 57Fe r e s o n a n c e s d e d u c e d s - w a v e F% p-wave absolute -~-transition strength. REPT N E A N D C ( J ) - 7 5 / U , P T 0 , K o m a n o . NUCLEAR REACTIONS 5SFe(n,3,),E=27.7 keV; 5SNi(n,')'),E=15.5 keV; S°Ni(n,3'),E=12.5 keV; ZVAl(n, -/),E=34.7 keV; measured E3,,I% 57Fe,S9,SlNi,~SA1 d e d u c e d s-wave resonance F'y. REPT NEANDC(E)-222U,Vol V,P2,Wisshak. NUCLEAR REACTIONS F e ( p , p " ~ ) , ( p , p ) , E = 3 6 8 0 - 3 8 3 5 k e V ; m e a s u r e d a(E,0). 5~Co d e d u c e d IAR. R-matrix a n a l y s i s . REPT Z F K - 3 8 5 , P 1 2 , H e r m a n n . NUCLEAR REACTIONS 5SNi(aHe,(x),E=13O MeV; m e a s u r e d (~(0). S7Ni l e v e l s d e d u c e d C2S. E x a c t finite-range,zero-range DWBA a n a l y s e s . REPT J U L - S p e z - ' 7 2 , P 1 8 , D j a l o e i s . NUCLEAR REACTIONS 5SNi(p,d),E=30 MeV; m e a s u r e d d-~(0). STNi level d e d u c e d d e u t e r o n D - s t a t e effect on polarization. REPT INS T o k y o 1980 A n n , P 2 8 , 0 h n u m a .

A S~Mn

=

ONLY)

-

59

NUCLEAR REACTIONS 56,SSFe(n,~/),E=10-100 kcV; m e a s u r e d c~(E). 57,59Fe r e s o n a n c e s d e d u c e d P'y. Activation technique. REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 , K a p p e l e r . NUCLEAR REACTIONS 5~Fc(p,'/),E=3 MeV; m e a s u r e d a(0). 59Co d e d u c e d p r i m a r y t r a n s i t i o n s Iy. Pair spectrometers,statistical t h e o r y . CONF R i g a , P 5 9 8 , P i s m e n e t s k i j . NUCLEAR REACTIONS 5SFe(n,7),E=27.7 keV; SSNi(nc/),E=15.5 keV; 6QNi(n,7),E=12.5 keV; ~TAl(n, 7),E=34.7 keV; measured E3',I7. 57Fe,59,SlNi,2eA1 d e d u c e d s-wave resonance F 7. REPT NEANDC(E)-E22U,Vol V,PE,Wisshak. NUCLEAR REACTIONS 58Ni?°Zr(polarized d,p),E=56 MeV; m e a s u r e d a ( 0 ) , v e c t o r a n a l y z i n g p o w e r v s 0. 59Ni,9JZr l e v e l s d e d u c e d transfered nucleon quantum number dependence. DWBA a n a l y s i s . REPT RCNP O s a k a , 1 9 8 1 A n n , P 2 8 , H a t a n a k a .

223

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 59Cu

R 79KrZV: 81DjZX: 81MaZF:

R 8OBEYS:

6OCo

R 81NaZO:

6ONi

R 79PaZ0:

80LeZK:

80ToZT

81DjZR

81TsZX 82BoZS 82HaZZ

820kZX

SOCu

R 79A1YW 81TsZX: 82AnZV 820kZX

6OZn

R 820kZX

R 82MaZN:

61Ni

R 81WiZN:

61Cu

R 820kZW:

continued

=

60

NUCLEAR REACTIONS 5a,6°,62,64Ni,S4,ss,sa,~°Zn(a4C,isO),E=72 MeV; m e a s u r e d a ( E ( l s O ) ) , a ( 0 ) . S2Fe, SSNi d e d u c e d m a s s e x c e s s . 56,58,6°,82Fe,62,s4,66,SSNi l e v e l s d e d u c e d S d e p e n d e n c e on neutron number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 9 , B e r n a s . NUCLEAR REACTIONS 58,s°,S2Ni(polarized d,a),E=80 MeV; m e a s u r e d v e c t o r a n a l y z i n g p o w e r v s 0. 56,ss,S°Co l e v e l s d e d u c e d J j r . B A P S A 26 l 1 3 6 , C D 5 , N a n n . NUCLEAR REACTIONS laC,54,58,SeFe,Sa,s°,62Ni,64,ss,sa,T°Zn(a,a),(a,a'),E=29,40,45,50 MeV; measured a ( E , 0 ) , laC,54,56,5ape,SS,s°,62Ni,64,66,Bs,V°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS 8 ° N i , S ° Z r , i l S I n , i 2 ° S n , 1 4 4 S m , t 6 5 H o , 1 9 7 A u , a ° a p b ( 3 H e , 3 H e ' ) , E = 1 0 8 . 5 MeV; measured cr(E(3He)),a(0). 6°Ni d e d u c e d GQR,F. Q°Zr,USIn,le°Sn,144Sm,iSSHo,i ~Au d e d u c e d GQR, giant monopole r e s o n a n c e , P . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS 6ONi(a,cd),E=65 MeV; m e a s u r e d a(Ea),cr(0). 6°Ni d e d u c e d EWSR f r a c t i o n f o r GQR,low e n e r g y o c t u p o l e , h e x a d e c a p o l e r e s o n a n c e s . DWBA a n a l y s i s . REPT INS T o k y o 1980 Ann,P29,Tohei. NUCLEAR R E A C T I O N S 4°Ca,SiV,Se,s°,62Ni,66Zn,9°,92,94,9~Zr,92,94,96,s,i°°Mo,12°,iZ4Sn,14°Ce(p,p'), E=201 MeV; m e a s u r e d a(Ep'). 4°Ca,51V,58,6°,62Ni,SSZn,9°,92,94,SSZr,92,94,96,98,1O°Mo,12°,124Sn d e d u c e d MI r e s o n a n c e , F . R E P T IPN 1981 A n n u a l , P N O 2 , D j a I a l i . NUCLEAR REACTIONS 5 8 N i ( a , 2 p ) , ( a , n p ) , E = 3 2 MeV; m e a s u r e d E T , I T , T T - c o i n , D S A . 6°Ni,6°Cu deduced levels,T,/2,configuration. REPT ISN 8 1 - 0 1 , P 2 5 , T s a n U n g C h a n . NUCLEAR REACTIONS 6 ° N i ( T , n ) , E = 1 4 - 2 0 MeV; m e a s u r e d a ( 0 ) v s E. S°Ni d e d u c e d GDR i s o s p i n s p l i t t i n g . REPT A N L - 8 1 - 7 9 , P l 1 0 , B o w l e s . NUCLEAR REACTIONS S°Ni(2SSi,zaSi'),E=140 MeV; m e a s u r e d a(E(ZaSi)). 6°Ni,26Si l e v e l s d e d u c e d inelastic excitation mechanism. Q3D s p e c t r o m e t e r . Coupled-channels a n a l y s i s . B A P S A 27 475,BXa10,Hansen. NUCLEAR REACTIONS S S N i ( ~ S O , ~ C ) , ( ~ O , 1 4 N ) , ( l S O , l ~ O ) , E = 8 0 MeV; m e a s u r e d a(O),cr(E(l~C)), a(E(t4N)),a(E(~aO)); deduced optical model parameters. S°Zn,S°Ni,8°Cu d e d u c e d I A S , i s o b a r i c multiplet members. Exact finite-range D W B A , c l u s t e r m o d e l . REPT RCNP Osaka,1981 A n n , P 9 5 , Okuma. NUCLEAR REACTIONS SSNi(a,npT),E=24.2 MeV; m e a s u r e d E T , I T , T T - c o i n . ~°Cu d e d u c e d l e v e l s , J , rr. CONF R i g a , P 3 3 2 , A l e k s a n d r o v . NUCLEAR REACTIONS SSNi(a,2p),(a,np),E=32 MeV; m e a s u r e d ET,IT,77-coin,DSA. S°Ni,S°Cu deduced levels,Ti/a,configuration. REPT ISN 8 1 - 0 1 , P 2 5 , T s a n U n g C h a n . NUCLEAR REACTIONS N i ( p , n ) , E = I 3 4 MeV; m e a s u r e d cr(En). 5e,e°,~a,~4Cu d e d u c e d levels, Gamow-Teller isospin fragmentation. B A P S A 27 7 3 1 , E E S , A n a n t a r a m a n . NUCLEAR REACTIONS 5SNi(iSO,14C),(lSO,taN),(lSO,Z40),E=80 MeV; m e a s u r e d a(0),(z(E(*aC)), (~(E(14N)),o'(E(I40)); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 6°Zn,S°Ni,8°Cu d e d u c e d ] A S , i s o b a r i c multiplet members. Exact finite-range D W B A , c l u s t e r m o d e l . REPT RCNP O s a k a , t 9 8 1 A n n , P 9 5 , Okuma. NUCLEAR REACTIONS 5eNi(~60,~aC),(~60,~4N),(*60,~40),E=80 MeV; m e a s u r e d a(0),a(E(14C)), a(E(*4N)),a(E(~40)); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . S°Zn,6°Ni,S°Cu d e d u c e d I A S , i s o b a r i c multiplet members. Exact finite-range D W B A , c l u s t e r m o d e l . REPT RCNP Osaka,1981 A n n , P 9 5 , Okuma. A

6'Co

59

NUCLEAR REACTIONS 5SNi(p,p'v),E=2.8-4.0 MeV; m e a s u r e d a(E,ET). 59Cu d e d u c e d r e s o n a n c e s . CONF R i g a , P 2 8 3 , K r a f t . NUCLEAR REACTIONS 58Ni(3He,d),E=130 MeV; m e a s u r e d ~ ( 0 ) . 59Cu l e v e l s d e d u c e d cZs. Zero-range DWBA a n a l y s i s . REPT J U L - S p e z - 9 9 , P 2 1 , D j a l o e i s . NUCLEAR REACTIONS U8Si,54Fe,SeNi(aHe,aHe),(aHe,d),E=89.3 MeV; 9 ° Z r , ' a 4 S n ( a H e , 3 H e ) , ( 3 H e , d ) , E=89.8 MeV; m e a s u r e d a(0). a P,S5Co,~Cu,~Nb,~sSb l e v e l s d e d u c e d C~S. F i n i t e - r a n g e DWBA analysis,nonlocal potentials. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 9 , M a t s u o k a .

A OOFe

=

ONLY)

=

61

NUCLEAR REACTIONS S 2 N i ( d , 3 H e ) , E = 7 8 MeV; m e a s u r e d a ( E ( 3 H e ) ) . 6iCo d e d u c e d levels. Multi-wire,hE gas proportional counters,high resolution magnetic spectrometer. REPT JUL-Spez- 146,P10,Marinov. NUCLEAR REACTIONS SSFe(n,7),E=27.7 keV; 5aNi(n,T),E=15.5 keV; 8°Ni(n,7),E=12.5 keV; 2 7 h i ( n , 7),E=34.7 keV; measured ET,I% STFe,59,StNi,2SAl d e d u c e d s-wave resonance FT. REPT NEANDC(E)-222U,Vol V,P2,Wisshak. NUCLEAR REACTIONS 58Ni(1SO,13C),(160,13N),E=80 MeV; m e a d s u r e d cr(0),a(E(i3C)),a(E(t3N)); deduced optical model parameters. 61Cu,6*Zn d e d u c e d levels,J,Tr. E x a c t f i n i t e - r a n g e DWBA, c l u s t e r m o d e l . REPT RCNP O s a k a , 1 9 8 1 A n n , P 1 0 1 , O k u m a .

224

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 6~Zn

R

830kZW:

R 80BeYS:

81BeZE: 81BeZK:

SaNi

R 79PaZO:

80BeYS:

8OKnZV: 80ToZS:

81DjZR:

81WiZR:

62Cu

R 82AnZV:

6aZn

R 810kZW:

810kZX: 82LeZV:

R 79KoZA: 80TsZX: 81AzZZ: 81E1ZY:

R 8OBEYS:

64Cu

R 82AnZV:

S4Zn

D 82PaZY:

=

62

=

63

NUCLEAR REACTIONS Cu(n,n'v),E=14.6 MeV; m e a s u r e d a(En),ET,IT. 63,85Cu r e s o n a n c e s d e d u c e d F T / F n . CONF R i g a , P 2 8 4 , K o z y r . NUCLEAR REACTIONS S l N i ( a , n p T ) , E = 3 O MeV. 63Cu d e d u c e d yrast levels Jjr,isomer,Tl/a, -F-branching,configuration. REPT ISN 8 0 - O i , P ~ 7 , T s a n U n g C h a n . NUCLEAR REACTIONS 55Mn(12C,X),E=55 MeV; m e a s u r e d 7 - m u l t i p l i c i t y . e4,eeZn,eaCu d e d u c e d evaporation channel average 7-multiplicity. REPT ISN 8 1 - 0 1 , P 5 6 , A z g u i . NUCLEAR REACTIONS 5 4 , 5 6 F e , 6 3 , 6 5 C u ( n , n ) , ( n , n ' ) , E = 1 4 MeV; m e a s u r e d •(0). 54,56Fe,63,65Cu d e d u c e d f12. O p t i c a l m o d e l , c o u p l e d - c h a n n e l s a n a l y s i s . DABBB 42 1931,E1-Kadi.

A S4Ni

continued

NUCLEAR REACTIONS 58,6°,ea,64Ni,64,66,es,76Zn(14C,160),E=72 MeV; m e a s u r e d a(E(1sO)),G(0). 62Fe, 6SNi d e d u c e d m a s s e x c e s s . 56,ss,6°,6~Fe,eZ,e4,66,68Ni levels deduced S dependence on neutron number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 9 , B e r n a s . NUCLEAR REACTIONS e4Ni,VeGe,76Zn,62Se('4C,160),E=72 MeV; m e a s u r e d cr(E(160)),a(0). 62Fe,68Ni, 74Zn,66Ge d e d u c e d m a s s e x c e s s . DWBA a n a l y s i s . REPT IPN 1981 A n n , P N 2 8 . NUCLEAR REACTIONS 64Ni,76Zn,~eGe,S2Se(14C,~60),E n o t g i v e n ; m e a s u r e d (y(E(ie0)),a(0). 6ZFe, 66Ni,74Zn,SOGe d e d u c e d l e v e l s , J , r r , m a s s e s . DWBA a n a l y s i s . CONF H e l s i n g o r Vol2 P397, CERN 81-09. NUCLEAR REACTIONS 12C, 54 ,5 6 ,5 8 Fe, 5 8 ,6 0 ,6 2 N]• .8 4. 6 .6 6. 8 7 0 Zn(a,a),(a,c~'),E=29,40,45,50 MeV; m e a s u r e d (7(E,0). 12C,54,56,58Fe,SU,s°,62Ni,64,66,ss,TOZn d e d u c e d d e f o r m a t i o n p a r a m e t e r ft. B l a i r p h a s e m e t h o d . CONF Riga,P320,Pavlova. NUCLEAR REACTIONS 56,se,sa,S4Ni,64,ss,66,TOZn('4C,'60),E=72 MeV; m e a s u r e d (7(E(160)),(7(e). 62Fe, SSNi deduced m a s s excess. 56,58,6e,62Fe,Sa,64,66,SSNi l e v e l s deduced S d e p e n d e n c e on n e u t r o n n u m b e r . DWBA a n a l y s i s . REPT IPN 1980 Annual,PN19,Bernas. NUCLEAR REACTIONS 58,SZNi(a,a'),(a,a'p),((~,2cO,E=155 MeV; m e a s u r e d (7(Ea'),c(a-,ap-coin. 58 62Ni d e d u c e d T=0,GQR decay c h a r a c t e r i s t i c . REPT JUL-Spez-72,P6,Knopfle. NUCLEAR REACTIONS 62Ni,SaZr(d,d'),E=64.7 MeV; m e a s u r e d cr(Ed),G(0). 62Ni,g2Zr deduced EWSR s t r e n g t h d i s t r i b u t i o n , d e f o r m a t i o np a r a m e t e r f o r low e n e r g y o c t u p o l e r e s o n a n c e s . DWBA a n a l y s i s . REPT INS Tokyo 1980 Ann,P29,T0hei. NUCLEAR REACTIONS 4o Ca, 51 V, 56 , 60 , 62 N1, . 6s Zn . 90. 92 . . 94 96 Zr . 92. 94 . .e6 . 98 loo Me, 1a0 , t24 S n , 14o C e ( p , p ), , E=201 MeV; m e a s u r e d ( ; ( E p ' ) . 40Ca,51V,56,eo,saNI,. aSZn .g°. gu . .04 9 e z r . gz. 94 . .96. 98 lOeMo,iZO,iZ4Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS S 2 N i ( p , p ' 7 ) , E = 8 1 . 5 , 1 9 9 . 1 MeV; S Z N i ( a , a ' 7 ) , E = 1 5 0 . 5 MeV; m e a s u r e d (particle)7-coin; deduced isotope production p e a k s . 6aNi d e d u c e d g i a n t r e s o n a n c e d e c a y entrance c h a n n e l d e p e n d e n c e . DABBB 42 1068,Wiggins. NUCLEAR REACTIONS N i ( p , n ) , E = 1 3 4 MeV; m e a s u r e d (~(En). 56,60,62,64Cu deduced levels, Gamow-Teller isospin fragmentation. BAPSA 27 7 3 1 , E E 8 , A n a n t a r a m a n . NUCLEAR REACTIONS 56Ni(160,~60'),(leo,12C),E=80 MeV; m e a s u r e d o'(E(16O)),o'(E(lzC)),cr(8). 6aZn levels deduced spectroscopic factors. Exact finite-range DWBA,light,heavy system a-transfer o v e r l a p s . REPT RCNP O s a k a , 1 9 8 0 A n n , P l 0 3 , O k u m a . NUCLEAR REACTIONS 58Ni,nSSn(160,lZC),E=80 MeV; m e a s u r e d cr(E('2C)),cr(O). 62Zn,122Te d e d u c e d l e v e l s , p o s s i b l e J , ~ . REPT RCNP O s a k a , 1 9 8 0 A n n , P 9 3 , 0 k u m a . NUCLEAR REACTIONS 55Cr(IZC,X),E=65-140 MeV; m e a s u r e d o(fusion) v s E. 6ZZn d e d u c e d excitation channel dependence. Statistical yrast,fusion entry line models,other input d a t a . REPT RCNP Osaka,1981 A n n , P 1 1 3 , L e e .

A

S3Cu

61

NUCLEAR REACTIONS 56Ni(160,laC),(160,13N),E=80 MeV; m e a d s u r e d cr(O),cr(E(laC)),cr(E(laN)); d e d u c e d o p t i c a l m o d e l p a r a m e t e r s . 6~Cu,6~Zn d e d u c e d l e v e l s , J , r r . E x a c t f i n i t e - r a n g e DWBA, c l u s t e r m o d e l . REPT RCNP 0 s a k e , 1 9 8 1 A n n , P l 0 1 , 0 k u m a .

A SaFe

=

ONLY)

=

64

NUCLEAR REACTIONS 56,6°,6z,64Ni,64,66,ea,7°Zn('4C,160),E=72 MeV; m e a s u r e d a(E(1BO)),c~(0). 6ZFe, SSNi d e d u c e d m a s s e x c e s s . 5e,sa,e°,eZFe,ea,a4,ea,eeNi l e v e l s d e d u c e d S d e p e n d e n c e o n n e u t r o n number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N l 9 , B e r n a s . NUCLEAR REACTIONS N i ( p , n ) , E = 1 3 4 MeV; m e a s u r e d (r(En). 58,60,62,64Cu deduced levels, Gamow-Teller isospin fragmentation. BAPSA 27 7 3 1 , E E 8 , A n a n t a r a m a n . R A D I O A C T I V I T Y 64Ga; m e a s u r e d I(ee). S4Zn d e d u c e d transition,B(E2). REPT JYFL 1981 Ann,P43, Passoja.

225

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A = 64Zn

R 79PaZ0:

80PaZM:

81AzZZ 82PaZY

64Ga

D 82PaZY

R 79DaZC: 79KoZA: 81E1ZY:

OSZn

R 81AzZZ:

R 80BeYS:

OOCu

R 80TsZW:

66Zn

R 79PaZ0:

82PaZW:

R 80BeYS

81BeZE 81BeZK

82BeZZ 68Zn

R 79PaZO:

80PaZM:

81DjZR:

81QaZY:

=

66

NUCLEAR REACTIONS 5a,s°,62,S4Ni,64,66,6s,7°Zn('4C,lS0),E=72 MeV; m e a s u r e d a(E(tsO)),(r(0). 6ZFe, 6SNi d e d u c e d m a s s e x c e s s . 56,5s,6°,62Fe,62,s4,ss,68Ni l e v e l s d e d u c e d S d e p e n d e n c e on neutron number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 9 , B e r n a s . NUCLEAR REACTIONS 6 4 N i ( a , d ) , E = 5 0 MeV; m e a s u r e d ( z ( E d ) , d v - c o i n . 8 4 N i ( a , n p ) , E = 3 2 MeV; 6 4 N i ( V L i , n a ) , E = 2 2 MeV; m e a s u r e d 77(t),77-,7(particle)-coin. SOCu d e d u c e d levels,J,Tr. REPT ISN 8 0 - 0 1 , P 2 ~ , T s a n U n g C h a n . NUCLEAR REACTIONS 12C,54,5%SaFe,SS,6°,6ZNi,64,os,ss,7°Zn(a,a),(a,a'),E=29,40,45,50 MeV; measured a ( E , 0 ) , lac,Sa,ss,SSFe,Se,6°,SaNi,64,so,68,~°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS S ~ F e , 6 6 Z n ( p , p ' v ) , E = 5 - 9 MeV; m e a s u r e d Ev,IT,pv-coin,I(ce). 56Fe,6SZn d e d u c e d E0 t r a n s i t i o n strength. REPT JYFL 1981 A n n , P 5 2 , P a s s o j a .

A 68Ni

65

NUCLEAR REACTIONS SSCu(v,7),E=I.ll4 MeV; m e a s u r e d 77(0,H). SSCu l e v e l s d e d u c e d /~. CONF Riga,P539,Davydov. NUCLEAR REACTIONS C u ( n , n ' v ) , E = 1 4 . 6 MeV; m e a s u r e d a(En),ET,17. ~3,6~Cu r e s o n a n c e s d e d u c e d r7/Fn. CONE R i g a , P 2 8 4 , K o z y r . NUCLEAR REACTIONS 5 4 , S 6 F e , 6 3 , 6 5 C u ( n , n ) , ( n , n ' ) , E = 1 4 MeV; m e a s u r e d or(0), s4,SSFe,Sa,SSCu d e d u c e d flz. O p t i c a l m o d e l , c o u p l e d - c h a n n e l s a n a l y s i s . DABBB 4 2 1 9 3 1 , E I - K a d i . NUCLEAR REACTIONS 55Mn(~eC,X),E=55 MeV; m e a s u r e d v-multiplicity. 64,65Zn,O3Cu d e d u c e d evaporation channel average 7-multiplicity. REPT ISN 8 1 - 0 1 , P 5 6 , A z g u i .

A 6~Ni

continued

NUCLEAR REACTIONS l~C,54,56,SOFe,58,6°,6~Ni,64,66,6s,7°Zn(a,a),(a,a'),E=29,40,45,50 MeV; measured a ( E , 0 ) . *ZC,Sa,~6,aSFe,5a,~°,6ZNi,~4,°~,~s,7°Zn d e d u c e d deformation parameter ft. B l a i r p h a s e m e t h o d . CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS 54Fe,64,6SZn(p,p'),E=6.9 MeV; m e a s u r e d ET,IT,I(ce),T~/u,internal p a i r s u m coincidence. 5~Fe,~4,°aZn l e v e l s d e d u c e d B ( E 0 ) / B ( E 2 ) , E 0 d e c a y b r a n c h i n g . REPT JYFL 1980 Ann,P31,Passoja. NUCLEAR REACTIONS 5~Mn(~2C,X),E=55 MeV; m e a s u r e d 7-multiplicity. s4,~%n,6aCu d e d u c e d evaporation channel average 7-multiplicity. REPT ISN 8 1 - 0 1 , P 5 6 , A z g u i . NUCLEAR REACTIONS ° a Z n ( p , p ' ) , E = 5 . 9 , 6 . 9 MeV; m e a s u r e d E7,I7,7p-coin,internal pair production spectrum. 64Zn d e d u c e d t r a n s i t i o n s , B ( E 2 ) ratios,monopole transition strength. REPT J Y F L 1981 A n n , P 4 3 , P a s s o j a . R A D I O A C T I V I T Y 84Ga; m e a s u r e d I(ce). ~4Zn d e d u c e d t r a n s i t i o n , B ( E 2 ) . REPT JYFL 1981 A n n , P 4 3 , Passoja.

A = O5Cu

64

ONLY)

=

68

NUCLEAR REACTIONS 5s,6°,62,64Ni,S4,6°,ss,7°Zn(14C,IoO),E=72 MeV; m e a s u r e d a(E(160)),cr(0). 62Fe, SSNi d e d u c e d m a s s e x c e s s , ss,ss,6°,62Fe,62,64,66,SSNi l e v e l s d e d u c e d S d e p e n d e n c e o n n e u t r o n number. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N t g , B e r n a s . NUCLEAR REACTIONS 64Ni,TSGe,7°Zn,SeSe(14C,160),E=72 MeV; m e a s u r e d a(E(160)),a(O). 6eFe,6SNi, V4Zn,a°Ge d e d u c e d m a s s e x c e s s . DWBA a n a l y s i s . REPT IPN 1981 A n n , P N 2 8 . NUCLEAR REACTIONS 64Ni,V°Zn,TSGe,aeSe(14C,lsO),E n o t g i v e n ; m e a s u r e d a ( E ( i 6 0 ) ) , a ( 0 ) . 6eFe, 6SNi,74Zn,S°Ge d e d u c e d l e v e l s , J , T r , m a s s e s . DWBA a n a l y s i s . CONF H e l s i n g o r Vo12 P397, CERN 81-09. NUCLEAR REACTIONS 7OZn(14C,isO),E=72 MeV; m e a s u r e d a(0),a(E(I°O)). 6eNi d e d u c e d level,J,~T. DWBA a n a l y s i s . REPT I P N O - D R E - 8 2 - 0 8 , B e r n a s . NUCLEAR REACTIONS laC,~4,s6,SeFe,Se,6°,6aNi,64,66,6s,T°Zn(a,a),(a,a'),E=29,40,45,50 MeV; measured a(E,O), leC,54,56,SaFe,Se,6o,62Ni,64,66,6a,~°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 0 , P a v l o v a . NUCLEAR REACTIONS 54Fe,64,SSZn(p,p'),E=6.9 MeV; m e a s u r e d E-),,IT,I(ce),Tl/2,internal p a i r s u m coincidence. 54Fe,64,Sazn l e v e l s d e d u c e d B ( E 0 ) / B ( E 2 ) , E 0 d e c a y b r a n c h i n g . REPT JYFL 1980 Ann,P31,Passoja. NUCLEAR REACTIONS 4°Ca,S*v,Se,°o,62Ni,°SZn,9°,9a,94,gSZr,~2,94,9%ge,l°°Mo,l~o,la4Sn,14OCe(p,p'), E=201 MeV; m e a s u r e d a ( E p ' ) . 4°Ca,51V,58,6°,62Ni,68Zn,9°,92,94,96Zr,92,94,96,98,1°°Mo,12°,l~4Sn deduced M1 r e s o n a n e e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 4 4 C a , 4 9 T i , S O C r , O T f i S Z n , 9 ~ Z r , g Y , 9 S M o ( n , d ) , ( n , n ' p ) , ( n , n p ) , E = 1 4 . 7 MeV; measured a; d e d u c e d s y s t e m a t i c s . 4fiCa,S°Ti,alCr,6S,69Zn,S3Zr,Oe,99Mo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 0 , Q a i m .

226

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 69Cu

R 81FIZW

~SZn

R 81QaZY

R 82AjZX

~OZn

R 79PaZO

76Ge

R 80PaZL

82PaZX

70Se

R 82AhZZ

D 79MaYT:

R 82GaZV:

R 81BeZE: 81BeZK:

=

71

=

deduced

chemical

=

influence

on

72

NUCLEAR REACTIONS ~SNi(160,np),E n o t g i v e n ; m e a s u r e d ET,IT,reeoil,Doppler l e v e l s d e d u c e d T I / a , B ( E 2 ). R E P T I N D C ( A R G ) - 9 / G , P b 3 8 , G a r c i a Bermudez.

A

74Zn

70

R A D I O A C T I V I T Y 7'Ge; m e a s u r e d e l e c t r o n c a p t u r e p r o b a b i l i t y ; probability. GeS,GeS~ s o u r c e s . CONF R i g a , P 2 3 2 , M a k a r y u n a s .

A 72BF

=

NUCLEAR REACTIONS 4°,4e,44Ca,4O,4s,S°Ti,54Cr,S4,56,58Fe,7°Zn(t,3He),E=25 MeV; m e a s u r e d ~(0). 40, 4z,44K,46,48,S°Sc,54V,~4,so,SSMn,T°Cu d e d u c e d l e v e l s . B A P S A 27 7 3 1 , E E 4 , A j z e n b e r g - S e l o v e . NUCLEAR REACTIONS 1 2 C , 5 % 5 6 , 5 8 F e , S S , o o , o 2 N i f i 4 , 6 6 , 6 8 , 7 ° Z n ( a , a ) , ( a , ( x ' ) , E = 2 9 , 4 0 , 4 5 , 5 0 MeV; measured a ( E , 0 ) , l~C,54,56,58Fe,SSfio,62Ni,64,6~,~8,~°Zn d e d u c e d deformation parameter ft. Blair phase method. CONF R i g a , P 3 2 O , P a v l o v a . NUCLEAR REACTIONS 7°Ge(p,p'),E=6.9 MeV; m e a s u r e d E T , I T , I ( c e ) , i n t e r n a l p a i r s p e c t r u m . 7°Ge l e v e l s d e d u c e d B(E2),B(E0)/B(ER). A n t i - C o m p t o n suppression,sum-coincidence measurement. REPT J Y F L 1980 A n n , P 3 5 , P a s s o j a . NUCLEAR REACTIONS ~ ° G e ( p , p ' ) , E = 6 . 9 MeV; ~ 4 S e ( p , p ' ) , E = 5 . 9 MeV; m e a s u r e d c e ( t ) . V4Se,7°Ge level deduced T,/a. Magnetic lens,Si-Li electron spectrometer,slope method. REPT JYFL 1981 A n n , P 4 7 , P a s s o j a . NUCLEAR REACTIONS 7°Zn(~aC,2n),E=38.4 MeV; m e a s u r e d E')',I7,7(0). S°Kr d e d u c e d levels,J,Tr, rotational bands,configuration,yrast back bend. Two~quasiparticle plus rotor calculations. SSNi(~4N,np),E=38 MeV; m e a s u r e d 7(0),77-coin,77(0),oriented nuclei. ~°Se deduced levels,Jdr,yrast band,band crossing. Interacting boson model calculations. ~4z~44 146,148,15°Nd(~,~x'),E not given; measured Coulomb excitation. ~S°Nd deduced E2,E4 moments. Semi-classial mode]. DABBB 42 2888,Ahmed.

A

71Ge

69

NUCLEAR REACTIONS 7°Zn,*°4Ru,U°Pd,~S4Sm,~Ss,*°°Gd,~sSW,~Se,*SSpt,a°a,e°4Hg,a44pu(polarized t,a), ~SOPt,a44pu,76Ge(polarized t , p ) , E = 1 7 MeV; o z , a ° S e , ~ ° ° M o , ' a a , ~ a ~ S n ( p o l a r i z e d t,aHe),E=22-25 MeV; m e a s u r e d o ' ( 0 ) , a n a l y z i n g p o w e r v s 0,a(E~x),a(Ep),o-(~He). SSCu,~°aTc,~6°Rh,~Sapm,~,~SaEu, I85Ta,lSs,iSVlr,~°~,a°3Au,Z43Np,a°°Pt,a46pu,TaGe,S°,S~As,i°°Nb,*ei,le41n deduced mass excess. CONF Helsingor Vo]l PI07, CERN 81-09. NUCLEAR REACTIONS 44Ca,4STi,5°Cr,67,SgZn,SaZr,ST,SeMo(n,d),(n,n'p),(n,np),E=14.7 MeV; measured a; deduced systematics. 45Ca,5°Ti,5~Cr,Sa,SSZn,93Zr,SS,SSMo deduced dominant decay mode. REPT NEANDC(E)-222U,Vol V,P30,Qaim.

A

7OCu

=

ONLY)

shift.

7aBr

74

NUCLEAR REACTIONS S4Ni,VSGe,7°Zn,S2Se(14C,~60),E=7R MeV; m e a s u r e d cr(E(lsO)),a(0). 6aFe,SSNi, 74Zn,S°Ge d e d u c e d m a s s e x c e s s . DWBA a n a l y s i s . REPT IPN 1981 A n n , P N 2 8 . NUCLEAR REACTIONS S4Ni,T°Zn,~SGe,82Se(i4C,160),E n o t g i v e n ; m e a s u r e d a ( E ( l s O ) ) , a ( 0 ) . 62Fe, 6SNi,74Zn,S°Ge d e d u c e d l e v e l s , J j r , m a s s e s . DWBA a n a l y s i s . CONF H e l s i n g o r Vo12 P397, CERN 81-09.

74Ge

D 82PaZX:

R 80TaZL: 80VeZV: 74As

D 82PaZX:

74Se

D 82PaZX:

R 81SaZK:

R A D I O A C T I V I T Y 74As; m e a s u r e d ET,IT,I(ee). 74Ge t r a n s i t i o n s d e d u c e d I ( K ) / ] 7 u p p e r l i m i t , v4 76Se [ f r o m ~4,~SSe(p,n)~4,76Br d e c a y ] ; measured ET,IT,I(ce),centroid shift. ~4Se l e v e l d e d u c e d T , / 2 . 74,TSSe t r a n s i t i o n s d e d u c e d I ( K ) / I T . REPT J Y F L 1981 A n n , P 4 7 , P a s s o j a . NUCLEAR REACTIONS 74Ge(p,p'),E=22 MeV; m e a s u r e d or(0). 74Ge levels d e d u c e d flz,fl3. DWBA,CCBA a n a l y s e s . REPT IPN 1980 A n n u a l , P N l l , T a m i s i e r . NUCLEAR REACTIONS 73Ge(d,p),E=12 MeV; m e a s u r e d a(Ep). 74Ge d e d u c e d w e a k p o p u l a t i o n of 0 + level. Split-pole spectrometer. REPT IPN 1980 A n n u a l , P N 1 2 , V e r g n e s . R A D I O A C T I V I T Y ~4As; m e a s u r e d E%lT,I(ee). 74Ge t r a n s i t i o n s d e d u c e d I ( K ) / I 7 u p p e r l i m i t , v4 7SSe [ f r o m 74,V6Se(p,n)74,76Br d e c a y ] ; measured ET,IT,I(ce),centroid shift. 74Se l e v e l d e d u c e d TI/~. 74,76Se t r a n s i t i o n s d e d u c e d I ( K ) / I T . REPT J Y F L 1981 A n n , P 4 7 , P a s s o j a . R A D I O A C T I V I T Y 74As; m e a s u r e d ET,IT,I(ce). V4Ge t r a n s i t i o n s d e d u c e d I ( K ) / I 7 u p p e r l i m i t . 74 76Se [ - f r o m 74,TSSe(p,n)74,~SBr d e c a y ] ; measured ET,17,I(ce),centroid shift. 74Se l e v e l d e d u c e d T i / z . 74,76Se t r a n s i t i o n s d e d u c e d I ( K ) / I T . REPT JYFL 1981 A n n , P 4 7 , P a s s o j a . NUCLEAR REACTIONS 74,Ts,Ts,s°,S2Se(p,p'),E=65 MeV; m e a s u r e d a ( 0 ) , p r o t o n m o m e n t u m spectra; deduced two-step process. 74,76,78,8°,8RSe d e d u c e d levels,J,Tr,excitation strengths. Coupled-ehannel,DWBA a n a l y s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 3 9 , S a k a m o t o .

227

SECONDARY

SOURCES

(Reports,Abstracts,eLc.

A 74Se

R 820gZZ:

82PaZX:

74BF

D 82AnZZ:

74Kr

D 81RoZQ:

D 82BaZP: 82MeZY:

75As

D 82BaZP: 82MeZY

75Se

D 82YoZZ R 81ToZZ

82ToZY

75Kr

R 82HeZY:

D 82JoZZ R 82AuZW

76Se

D 81ToZZ 82PaZX:

R 81SaZK:

82DeZZ:

820gZZ:

76Br

D 82AnZZ:

76Kr

D 81MoZK:

81PiZY: 76Rb

D 81MoZK:

continued

=

75

R A D I O A C T I V I T Y 75mGe(fl-); m e a s u r e d EV,Iv,T1/2; d e d u c e d Ifl,log f t . 75As d e d u c e d level,J,vr. B A P S A 27 7 1 4 , C C 1 3 , B a r k a n . R A D I O A C T I V I T Y 7SmGe(fl-); m e a s u r e d EV,Iv,TI/2; d e d u c e d Ifl,log ft. 75As d e d u c e d levels. BAPSA 27 7 1 4 , C C 1 4 , M e r i c - B a r k a n . R A D I O A C T I V I T Y 75mGe(fl-); m e a s u r e d EV,Iv,T,/2; d e d u c e d Ifl,log f t . 75As d e d u c e d level,J,~r. B A P S A 27 7 1 4 , C C 1 3 , B a r k a n . R A D I O A C T I V I T Y 75mGe(fl-); m e a s u r e d EV,Iv,T1/2; d e d u c e d Ifl,log ft. 75As d e d u c e d levels. BAPSA 27 7 1 4 , C C 1 4 , M e r i c - B a r k a n . R A D I O A C T I V I T Y 7SSe(EC),tesSb(fl-),133Ba(EC),~S°Tb(fl-),ISSTm(EC); m e a s u r e d Ev,relative 17. REPT N E A N D C ( J ) - 8 3 / U , P 9 , Y o s h i z a w a . NUCLEAR REACTIONS 7 4 S e ( n , v ) , E = t h e r m a l ; m e a s u r e d EV,Iv; d e d u c e d c a p t u r e p r o d u c t i o n a f o r 75Se. 75Se d e d u c e d n e u t r o n binding energy. Bent crystal spectrometer. REPT J U L - S p e z - 9 9 , P75,Tokunaga. NUCLEAR REACTIONS 7 4 , 7 6 S e ( n , v ) , ( n , e - ) , E = s l o w ; m e a s u r e d n o t g i v e n . 75,77Se d e d u c e d l e v e l s , v-branching,J,rr. REPT J U L - S p e z - 1 4 6 , P 4 4 , T o k u n a g a . NUCLEAR R E A C T I O N S 46Ti(3aS,n2p),E=85-150 MeV; m e a s u r e d 77-,n77-coin,a(Ev). 75Kr deduced levels,J,r:,band structure,Nilsson assignments. B A P S A 27 713,CCl0,Herath-Banda.

A 76As

74

NUCLEAR REACTIONS 74,76,78,8°,82Se(polarized p , p ) , ( p o l a r i z e d p,p'),E n o t g i v e n ; m e a s u r e d a n a l y z i n g p o w e r v s O. 74,76,78,86,82Se d e d u c e d J - d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP Osaka, 1981 A n n , P 1 6 , 0 g i n o . NUCLEAR REACTIONS 7 ° G e ( p , p ' ) , E = 6 . 9 MeV; 7 4 S e ( p , p ' ) , E = 5 . 9 MeV; m e a s u r e d c e ( t ) . 74Se,V°Ge level deduced Tl/a. Magnetic lens,Si-Li electron spectrometer,slope method. REPT JYFL 1981 A n n , P 4 7 , P a s s o j a . R A D I O A C T I V I T Y *°°mpd [ f r o m 9'Zr('aC,3n)]; 76mBr [ f r o m SaCu(aSO,n2p)]; 74mBr [ f r o m 6°Ni(160, np)3; measured T1/2. B A P S A 27 2 7 , D F 1 4 , A n d r e j t s e h e f f . R A D I O A C T I V I T Y 74Kr [ f r o m SSNi(*gF,2np)3; m e a s u r e d not given; deduced levels,yrast, rotational bands. Rotational alignment model,quasiparticle excitation. In-beam V-spectroscopy,neutron multiplicity coincidence techniques. B A P S A E6 1 2 3 6 , H E 1 4 , R o t h .

A

75Ge

=

ONLY)

=

76

R A D I O A C T I V I T Y 7SAs; m e a s u r e d fl7(O). R e s o n a n t 7 - s e a t t e r i n g , f l - n e u t r i n o angular correlation equivalence d i s c u s s e d . DABBB 42 3 3 1 7 , J o n e s . NUCLEAR REACTIONS 76Ge,SZSe,12a,13OTe(p,n),E=135 MeV; m e a s u r e d a ( 0 ) , a ( E n ) . 76As?ZBr d e d u c e d L=0 G a m o w - T e l l e r strength. 128,13°Xe d e d u c e d t w o - f l p r o c e s s v i r t u a l state Gamow-Teller strength. B A P S A 27 7 3 1 , E E V , A u s t i n . R A D I O A C T I V I T Y 76Se [ f r o m d o u b l e n e u t r o n c a p t u r e on 74Se]; m e a s u r e d EV,I7; d e d u c e d n e u t r o n binding energy,transitions. Bent crystal spectrometer. REPT J U L - S p e z - 9 9 , P 7 5 , T o k u n a g a . R A D I O A C T I V I T Y 74As; m e a s u r e d Ev,Iv,I(ce). 74Ge t r a n s i t i o n s d e d u c e d I ( K ) / I 7 u p p e r l i m i t . 74, 76Se [ f r o m 74,76Se(p,n)74,VSBr d e c a y ] ; measured Ev,Iv,I(ce),centroid shift. 74Se l e v e l d e d u c e d T , / e . 74,VSSe t r a n s i t i o n s d e d u c e d I ( K ) / 1 7 . REPT J Y F L 1981 A n n , P 4 7 , P a s s o j a . NUCLEAR REACTIONS 74,vs,ve,e°,e2se(p,p'),E=65 MeV; m e a s u r e d a ( 0 ) , p r o t o n m o m e n t u m spectra; deduced two-step process. 74,76,78,8°,82Se d e d u c e d levels,J,rr,exeitation strengths. Coupled-channel,DWBA a n a l y s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 3 9 , S a k a m o t o . NUCLEAR REACTIONS 7 s , v e , s ° , e ~ S e ( p o l a r i z e d p , p ' ) , E = 1 6 MeV; m e a s u r e d a(O),A(0). 76,vs,8°,S2Se deduced deformation parameters. Coupled-channels method,rotation-vibration,asymmetric rotation m o d e l s . B A P S A 27 4 6 0 , A Y a 1 0 , D e l a r o c h e . NUCLEAR REACTIONS 7 4 , 7 6 , v s , e ° , S 2 S e ( p o l a r i z e d p , p ) , ( p o l a r i z e d p,p'),E not given; measured a n a l y z i n g p o w e r v s O. 74,78,78,SQ,SZSe d e d u c e d J - d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP O s a k a , 1981 A n n , P l S , O g i n o . R A D I O A C T I V I T Y l°°mpd [ f r o m 91Zr(leC,3n)3; 76mBr [ f r o m 63Cu('SO,n2p)]; 74mBr [ f r o m 6°Ni(*60, rip)i; measured T , / ~ . B A P S A 27 2 7 , D F 1 4 , A n d r e j t s c h e f f . R A D I O A C T I V I T Y 76,77,78Rb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell dependence. 76,77,7SRb,76,77,78KF d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . B A P S A 26 II36,CD8,Moltz. RADIOACTIVITY 76RD [ f r o m m a s s s e p a r a t o r ] ; m e a s u r e d fl+-decay. 76Kr d e d u c e d l e v e l s , J , l r , y r a s t cascade,band c r o s s i n g . B A P S A 26 1 2 3 5 , H E l l , P i e r c e y . R A D I O A C T I V I T Y 76,77,78Rb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell dependence. 76,77,78Rb,76,77,78Kr d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . B A P S A 26

l136,CD8,Moltz.

228

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 76Rb

D 81MoZN

81PiZY

RADIOACTIVITY 76,77,78Rb [ f r o m Q(EC),mass excess. High precision 81-09. RADIOACTIVITY ~SRb [ f r o m m a s s c a s c a d e , b a n d c r o s s i n g . BAPSA 26

A 77Se

D

81ZaZX

R 78MoYV

82ToZY 77Br

D 81ZaZX R 81ZuZX

~Kr

D

81MoZK

82CIZZ 77Rb

D

80DeZB

81MoZK

81MoZN

R 81F1ZW

78Se

R 81AnZU

81SaZK

82DeZZ

820gZZ:

7SKr

D 81MoZK:

7SRb

D 81MoZK:

81MoZN:

76

continued

mass separator3; measured fl-endpoint energies; deduced i n t r i n s i c Ge d e t e c t o r s . CONF H e l s i n g o r V o l l P141, CERN s e p a r a t o r ] ; m e a s u r e d fl+-decay. 7SKr deduced 1235,HEll,Piercey.

=

levels,J,~,yrast

77

RADIOACTIVITY 77Br; m e a s u r e d 77(t),77(0,H,t). 77Se level d e d u c e d T1/a,g. REPT INDC(BZL)-5/ G,P5,Zamboni. NUCLEAR REACTIONS 7s,7a,s°,SaSe(polarized d,p),E=12.5 MeV; m e a s u r e d a ( 0 ) , v e c t o r a n a l y z i n g p o w e r v s 0. 77,79,al,aase d e d u c e d levels,J,Tr,S. B r o a d - r a n g e magnetic spectrograph. DWBA a n a l y s i s . THESIS L A M o n t e s t r u q u e , N o t r e Dame University. NUCLEAR REACTIONS 74,TSSe(n,T),(n,e-),E=slow; m e a s u r e d n o t g i v e n . 75,778e d e d u c e d l e v e l s , y-branching,J,lr. REPT J U L - S p e z - 1 4 6 , P 4 4 , T o k u n a g a . RADIOACTIVITY 77Br; m e a s u r e d 7y(t),yy(O,H,t). 77Se level d e d u c e d Tl/2,g. REPT INDC(BZL)-5/ G,P5,Zamboni. NUCLEAR REACTIONS 7s,7a,so,aaSe(aHe,d),E=24 MeV; m e a s u r e d ~ ( 0 ) , g ( E d ) ; d e d u c e d Q. 77,79,st aaBr d e d u c e d l e v e l s , L , S . DABBB 42 1 0 6 9 , Z u m b r o . R A D I O A C T I V I T Y 7s,77,TSRb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell d e p e n d e n c e . 76,77,TSRb,76,77,7SKr d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . BAPSA 26 1136,CD8,Moltz. R A D I O A C T I V I T Y 77Kr [ f r o m 6acu(160,np),E=42 MeV]; m e a s u r e d I(K X-ray)/I%T1/a. 77Kr levels d e d u c e d J,rr,lCC. T h i c k Cu t a r g e t , p u l s e d b e a m . BAPSA 27 4 9 8 , D Y a 5 , C l a r k . RADIOACTIVITY 77,a°Rb,7a,21Sr,Se,sa,S4y,ae,SSZr,aS,aTNb [ f r o m o n - l i n e s e p a r a t i o n 3 ; m e a s u r e d flT-,fl(fragment)-eoin,Ey,IT; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. RADIOACTIVITY 7s,77,TSRb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell d e p e n d e n c e . 7s,77,TSRb,76,77,7SKr d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . BAPSA 28 l136,CD8,Moltz. RADIOACTIVITY 7s,77,TSRb [ f r o m m a s s s e p a r a t o r 3 ; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . H i g h p r e c i s i o n i n t r i n s i c Ge d e t e c t o r s . CONF H e l s i n g o r V o l l P14i, CERN 81-09.

A

78Ge

=

ONLY)

=

78

NUCLEAR REACTIONS 70Zn,l°4Ru,nOpd,lS4Sm,lSS,16°Gd,lsSW,19s,19Spt,Z°2,2°4Hg,e44Pu(polarized t,c~), ~ g S p t , Z 4 4 p u , V S G e ( p o l a r i z e d t , p ) , E = 1 7 MeV; s s , S O S e , l ° ° M o , l e e , 1 2 4 S n ( p o l a r i z e d t , 3 H e ) , E = 2 2 - 2 5 MeV; m e a s u r e d ~ r ( 0 ) , a n a l y z i n g p o w e r v s 0 , ~ ( E a ) , a ( E p ) , a ( a H e ) . Sgcu,l°aTc,~°gRh,lSapm,157,1SSEu, ~eSTa,195,19?Ir,a°l,s°aAu,a4aNp,a°°Pt,s4Spu,TSGe,S°,SSAs,~O°Nb,tSs,lS41n d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . NUCLEAR REACTIONS 7 7 S e ( n , a ) , E = l 1 2 - 1 2 6 5 eV; 1 4 S N d ( n , a ) , E = 4 . 3 5 - 3 0 6 eV; m e a s u r e d ~(Ea), t i m e - s p e c t r a . 78Se d e d u c e d r e s o n a n c e s , r a . 14SNd d e d u c e d r e s o n a n c e s . REPT J I N R - P 3 - 8 1 - 3 4 8 , Antonov. NUCLEAR REACTIONS ?4,TS,TS,S°,SaSe(p,p'),E=65 MeV; m e a s u r e d a ( 0 ) , p r o t o n m o m e n t u m spectra; deduced two-step process. 74,76,78,8°,82Se d e d u c e d levels,J,rr,excitation strengths. Coupled-channel,DWBA a n a l y s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 3 9 , S a k a m o t o . NUCLEAR REACTIONS 7 s , ? s , s ° , a a S e ( p o l a r i z e d p,p'),E=16 MeV; m e a s u r e d a ( 0 ) , A ( 0 ) . 7s,?s,s°,SSSe deduced deformation parameters. Coupled-channels method,rotation-vibration,asymmetric rotation m o d e l s . BAPSA 27 4 6 0 , A Y a 1 0 , D e l a r o c h e . NUCLEAR REACTIONS 74,?S,TS,So,SSSe(polarized p , p ) , ( p o l a r i z e d p , p ' ) , E n o t g i v e n ; m e a s u r e d a n a l y z i n g p o w e r v s 0. 74,TS,?a,8o,SSSe d e d u c e d J - d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP Osaka, 1981 A n n , P l 6 , 0 g i n o . R A D I O A C T I V I T Y 7S,VT,TSRb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell d e p e n d e n c e . 7s,7?,78Rb,?S,7?,TaKr d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . BAPSA 26 t136,CD8,Moltz. R A D I O A C T I V I T Y 76,77,78Rb; m e a s u r e d fl e n d p o i n t energies; deduced mass surface shell dependence. 7s,77,78RD,76,?7,78KF d e d u c e d m a s s d i f f e r e n c e . I n t r i n s i c Ge d e t e c t o r . BAPSA 26 l136,CD8,Moltz. R A D I O A C T I V I T Y 76,77,78Rb [ f r o m m a s s s e p a r a t o r 3 ; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . H i g h p r e c i s i o n i n t r i n s i c Ge d e t e c t o r s . CONF H e l s i n g o r V o l l P141, CERN 81-09.

229

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 79Ga 79Ge 79As

D 80HoZN: D 80HoZN: R 80RoZQ:

79Se

R 78MoYV:

79Br

R 81ZuZX:

79Kr

R 80SaZH:

82BeZU:

79Rb

D 80DeYZ: 81DeZD:

81JaZU:

R 8~FoZY:

82ThZY: 79Sr

D 80DeYZ 80DeZB

81DeZD

81JaZU

R 81LiZQ:

D 80HoZN: D 80HoZN: 81ZeZY: R 81BeZE:

81BeZg:

8OAs

D 81LiZP: R 81FIZW:

79

R A D I O A C T I V I T Y ~9,8°,81,82Ga,79,s°,Sl,SaGe; m e a s u r e d E - y , I T , 5 , - / - c o i n . REPT N F L - R 2 , H o f f . R A D I O A C T I V I T Y 79,s°,sl,82Ga,79,a0,at,S2Ge; m e a s u r e d ET,I%~7-coin. REPT N F L - 2 2 , H o f f . NUCLEAR REACTIONS e°,S2Se(d,3He),E=25 MeV; m e a s u r e d o'(0),G(E(aHe)); d e d u c e d Q. 7°,81As d e d u c e d l e v e l s , J j r . DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 3 4 , R o t b a r d . NUCLEAR REACTIONS vs,vs,a°,aaSe(polarized d,p),E=12.5 MeV; m e a s u r e d a(0),vector analyzing p o w e r v s 0. 77,7~,sl,83Se d e d u c e d levels,Jjr,S. Broad-range magnetic spectrograph. DWBA a n a l y s i s . THESIS L A M o n t e s t r u q u e , N o t r e Dame University. NUCLEAR REACTIONS 76,T8,s°,eeSe(aHe,d),E=24 MeV; m e a s u r e d a ( 0 ) , a ( E d ) ; d e d u c e d Q. 77,79,81, S~Br d e d u c e d l e v e l s , L , S . DABBB 4~ 1 0 6 9 , Z u m b r o . NUCLEAR REACTIONS 7 ° Z n ( ~ e C , 3 n ) , E = 3 8 . 4 MeV; m e a s u r e d E-/,Is~,~5'-coinc/(0). ~Kr deduced levels,Jjr,rotational b a n d . CONF New 0 r l e a n s ( B a n d Structure and Nuclear Dynamics) Contrib,P127. NUCLEAR REACTIONS 7 8 S e ( a , 3 n ) , E n o t g i v e n ; m e a s u r e d E T , I s ' , 7 5 ' - c o i n , 7 ( 0 ) , 7 ( t ) , D S A . 7~Kr deduced levels,M1 transition hindrance,J,~r,band characteristics,v-branching, 7-multipolarity. REPT I N D C ( A R G ) - 9 / G , P b 4 , B e h a r . R A D I O A C T I V I T Y 79Sr [ f r o m 5~Fe(3aS,n~p~),E=123 MeV3; m e a s u r e d " / 7 - , f i T - c o i n ; d e d u c e d Qfl,mass e x c e s s . ~SRb l e v e l s d e d u c e d T ~ / z , 7 - b r a n c h i n g . REPT IPN 1980 A n n u a l , P R T , D e l l a Negra. R A D I O A C T I V I T Y ~o,a~Sr,~l,a~,83,e4Y,8~,a~,a3,sa,8%r,SS,aTNb [ f r o m 5~Fe(3ZS,X),E=101 MeV; 58Ni(3ZS, X),E=175 MeV]; m e a s u r e d 7*~-,fl+~/-,5,(X-ray)-coin,Q(EC),Efl+,ET,I%E(X-ray),t(X-ray); deduced m a s s e x c e s s , l o g f t . 8~,83Sr,SS,a~Zr,7~Rb d e d u c e d levels,T1/~,7-branching, e2Sr,aUY d e d u c e d levels,~-branehing. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y 7%r,S°,s~,sz,S3y,SSZr [ f r o m ~4Fe,5°Cr(SZs,X),E=100-123 MeV]; m e a s u r e d ")'3'-, 7 ( X - r a y ) - , T f l + - c o i n , E f l + , Q ( E C ) , Q B ; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s , e3Y,~ORb deduced levels,T1/a,J,~,5'-multipolarity, a°,e~,a~,e3Sr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a c q u e t . NUCLEAR REACTIONS 78,8°,8~Kr(3He,d),E n o t g i v e n ; m e a s u r e d (7(0). 79,s~,a3Rb d e d u c e d l e v e l s , J , ~r,S. B A P S A 27 4 9 8 , D Y a 9 , F o r t u n e . NUCLEAR REACTIONS s 4 , S ~ F e ( ~ S S i , X ) , E = 8 0 - 9 9 MeV; m e a s u r e d ET,IT,7(0),~(ET),73'-coin, a(fragment) v s E; d e d u c e d e x i t c h a n n e l angular momentum e f f e c t s . VgRb,S°Sr d e d u c e d l e v e l s , e~Sr d e d u c e d l e v e l s , J , q u a s i r o t a t i o n a l b a n d s . DABBB 42 3 3 1 8 , T h e i s e n . R A D I O A C T I V I T Y 79Sr [ - f r o m 54Fe(32S,nRpa),E=123 MeVS; m e a s u r e d 7 7 - , f l ' ~ - c o i n ; d e d u c e d Qfl,mass e x c e s s . ~9Rb l e v e l s d e d u c e d T ~ / ~ , ~ - b r a n c h i n g . REPT IPN 1980 A n n u a l , P R T , D e l l a Negra. R A D I O A C T I V I T Y 77,8°Rb,Vg,SlSr,S~,e3,8~Y,8~,aSZr,~,a~Nb [ f r o m on-line separation]; measured fl~/-,fl(fragment)-coin,E%IT; deduced Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. R A D I O A C T I V I T Y 79,8~Sr,e',aa,a3,S4Y,S~,sa,83,84,SSZr,en,87Nb [ - f r o m S4Fe(3aS,X),E=I01 MeV; 58Ni(3ZS, X),E=175 MeV]; m e a s u r e d 77-,fl+T-,'7(X-ray)-coin,Q(EC),Efl+,E5",I%E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . 81,SSSr,SS,SrZr,7ORb d e d u c e d levels,Tl/~,~/-branching. S2Sr,SSY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y 79Sr,S°,8~,sa,e3Y,aaZr [ f r o m 5 4 F e , 5 ° c r ( a a s , X ) , E = I 0 0 - 1 2 3 MeV]; m e a s u r e d 5'7-, ~/(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . 83y,~gRb deduced levels,T~/a,Jjr,7-multipolarity. 8°,s~,au,e3Sr d e d u c e d l e v e l s , 5 " - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT ] P N O - T - 8 1 - 1 0 , J a c q u e t . NUCLEAI~ REACTIONS ~8Ni(~4Mg,X),E=65-110 MeV; 5aNi(~aSi,X),(29Si,X),E=80-130 MeV; SaNi(~S,X), E = 9 0 - 1 5 0 MeV; m e a s u r e d E5",I%7(t),nT-,nnT-,5"7-coin. 79Sr,aaZr d e d u c e d l e v e l s . B A P S A 26 1137,CD11,Lister.

A eOGa 8OGe

=

ONLY)

=

80

R A D I O A C T I V I T Y 79,8°,st,82Ga,Vg,s°,8~,S2Ge; m e a s u r e d E-y,17,~/-/-coin. REPT N F L - 2 2 , H o f f . R A D I O A C T I V I T Y 79,8°,81,82Ga,79,8°,e',82Ge; m e a s u r e d E s , , I ~ / , ~ 3 , - c o i n . REPT N F L - R 2 , H o f f . R A D I O A C T I V I T Y u°,sl,S2Ge [ - f r o m s p a l l a t i o n S ; m e a s u r e d E%I% REPT U n i v M a i n z , 1 9 8 0 , A n n u a l , P 1 , Zendel. NUCLEAR REACTIONS 64Ni,76Ge,T°Zn,SaSe(14C,160),E=72 MeV; m e a s u r e d (7(E(160)),a(O). 62Fe,BSNi, 74Zn,8°Ge d e d u c e d m a s s e x c e s s . DWBA a n a l y s i s . REPT IPN 1981 A n n , P N 2 8 . NUCLEAR REACTIONS 64Ni,7°Zn,76Ge,8aSe(14C,t60),E n o t g i v e n ; m e a s u r e d cr(E(l~O)),a(0). 6ZFe, 88Ni,74Zn,e°Ge d e d u c e d l e v e l s , J , T r , m a s s e s . DWBA a n a l y s i s . CONF H e l s i n g o r V o l 2 P397, CERN 81-09. R A D I O A C T I V I T Y s°,sz,83,84As; m e a s u r e d E5',Is',~/7(t). 8z,S3Se d e d u c e d l e v e l s . BAPSA 26 1137, CD13,Lien. NUCLEAR REACTIONS 7°Zn,l°4Ru,ll°Pd,t54Sm,158,iB°Gd,laBW,196,198pt,2°z,2°4Hg,~44pu(polarized t , a ) , 198Pt,z44pu,~BGe(polarized t , p ) , E = 1 7 MeV; e 2 , S ° S e , l ° ° M o , i a z , 1 2 4 S n ( p o l a r i z e d t , S H e ) , E - 2 2 25 MeV; m e a s u r e d c r ( 0 ) , a n a l y z i n g p o w e r v s 0,a(Ea),cr(Ep),(~(SHe). 6gCu,l°STc,l°~Rh,~nSpm,lST,159Eu, leSTa,195,1971r,~°l,Z°SAu,243Np,Z°°Pt,z46pu,TSGe,S°,SaAs,l°°Nb,122,i24In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 .

230

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A SOSe

R 81SaZK:

82DeZZ:

820gZZ:

SOKr

R 82AhZZ:

8ORb

D 80DeZB:

sgSF

D

81JaZU:

R 82ThZY:

SOy

D 81JaZU:

SOZr

R 80StZK:

D 80HoZN: D 80HoZN: 81ZeZY:

81As

R 80RoZQ:

SlSe

R 78MoYV:

81Br

R 79ChZM: 81ZuZX:

81Kr

R 82BuZX:

a~Rb

R 82FoZY:

81St

D 80DeZB:

81DeZD:

81JaZU:

80

continued

NUCLEAR R E A C T I O N S 74,76,78,s°,SZSe(p,p'),E=65 MeV; m e a s u r e d cr(0),proton m o m e n t u m spectra; deduced two-step process. 74,76,Ts,so,82Se d e d u c e d levels,J,rr,excitation strengths. Coupled-channel,DWBA a n a l y s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 3 9 , S a k a m o t o . NUCLEAR REACTIONS 7 6 , T s , s ° , S e S e ( p o l a r i z e d p , p ' ) , E = 1 6 MeV; m e a s u r e d (;(0),At0). 76,78,s°,SaSe deduced deformation parameters. Coupled-channels method,rotation-vibration,asymmetric rotation m o d e l s . B A P S A 27 4 6 0 , A Y a 1 0 , D e l a r o c h e . NUCLEAR REACTIONS 7 4 , 7 6 , 7 s , s ° , S e S e ( p o l a r i z e d p , p ) , ( p o l a r i z e d p,p'),E n o t g i v e n ; m e a s u r e d a n a l y z i n g p o w e r v s 0. 74,76,78,8°,82Se d e d u c e d J - d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP Osaka, 1981 A n n , P 1 6 , 0 g i n o . NUCLEAR REACTIONS 7°Zn(*2C,2n),E=38.4 MeV; m e a s u r e d E7,I7,7(0). 8°Kr d e d u c e d l e v e l s , J , r r , rotational bands,configuration,yrast back bend. Two-quasiparticle plus rotor calculations. 5 S N i ( t 4 N , n p ) , E = 3 8 MeV; m e a s u r e d 7(0),77-coin,77(0),oriented nuclei. 7°Se deduced levels,J,rr,yrast band,band crossing. Interacting boson model calculations. 142144 *46,*48,159Nd(c~,c~'),E n o t g i v e n ; m e a s u r e d C o u l o m b e x c i t a t i o n . 15°Nd d e d u c e d E2,E4 m o m e n t s . Semi-classial m o d e l . DABBB 4 2 2 8 8 8 , A h m e d . R A D I O A C T I V I T Y 77,8°Rb,79,81Sr,S2,83,S4Y,Se,SSZr,S6,STNb [ f r o m on-line separation]; measured flT-,fl(fragment)-eoin,ET,IT; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. R A D I O A C T I V I T Y 79Sr,S°,s~,sz,SaY,SSZr [ f r o m S~Fe,S°Cr(aeS,X),E=100-123 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . SaY,VSRb deduced levels,T,/e,J,~,7-multipolarity, s°,s*,se,SaSr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a e q u e t . NUCLEAR REACTIONS 5 % S S F e ( e S S i , X ) , E = 8 0 - 9 9 MeV; m e a s u r e d ET,IT,7(0),(~(ET),77-coin, (;(fragment) v s E; d e d u c e d e x i t c h a n n e l angular momentum effects. 79Rb,s°Sr deduced l e v e l s . S~Sr d e d u c e d l e v e l s , J , q u a s i r o t a t i o n a l b a n d s . DABBB 42 3 3 1 8 , T h e i s e n . R A D I O A C T I V I T Y 79Sr,S°,91,se,eaY,SaZr [ f r o m 5~Fe,S°Cr(~aS,X),E=100-123 MeVS; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . 83Y,79Rb deduced levels,T1/z,Jjr,7-multipolarity, s°,s*,se,SaSr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a c q u e t . NUCLEAR REACTIONS SSCu,~°Ca(4°Ca,4°Ca),(4°Ca,X),E=400 MeV; m e a s u r e d ( ; ( f r a g m e n t E ) , f r a g m e n t m a s s , Z . 8°Zr,*°31n d e d u c e d r e s o n a n c e structure. REPT IPN 1980 A n n u a l , P N 5 0 , S t e p h a n .

A 81Ga SIGe

=

ONLY)

=

81

RADIOACTIVITY 79,s°,sl,SaGa,79,s°,si,S2Ge; m e a s u r e d Ev,17,77-eoin. R E P T NFL-22,Hoff. RADIOACTIVITY 79,s°,si,82Ga,Vg,s°,81,S2Ge; m e a s u r e d Ev,IV,VT-eoin. R E P T NFL-22,Hoff. RADIOACTIVITY s°,m,S2Ge [ f r o m spallation]; measured E7,17. REPT Univ Mainz,1980,Annual,Pl, Zendel. NUCLEAR REACTIONS 8°,82Se(d,SHe),E=25 MeV; m e a s u r e d cr(O),c;(E(3He)); d e d u c e d Q. 79,SIAs d e d u c e d levels,J,~r. D W B A analysis. R E P T IPN 1980 Annual,PN34,Rotbard. NUCLEAR R E A C T I O N S 76,Ts,8°,SZSe(polarized d,p),E=12.5 MeV; m e a s u r e d c;(0),vector analyzing p o w e r vs e. 77,79,8i,83Se d e d u c e d levels,J,vr,S. B r o a d - r a n g e m a g n e t i c spectrograph. D W B A analysis. T H E S I S L A Montestruque,Notre Dame University. NUCLEAR REACTIONS S°Se(p,v),E=2.6 MeV; m e a s u r e d E7,17. SiBr d e d u c e d levels. Enriched targets. C O N F Riga,P273,Chirt. NUCLEAR R E A C T I O N S 76,ve,8°,S2Se(SHe,d),E=24 MeV; m e a s u r e d cr(0),•(Ed); deduced Q. ~779si, 83Br d e d u c e d levels,L,S. D A B B B 42 1069,Zumbro. NUCLEAR R E A C T I O N S 8°Kr(polarized d,p),E=ll MeV; m e a s u r e d cr(0),vector analyzing power vs 0; deduced optical m o d e l parameters. SIKr levels deduced J,~r,L,S. D W B A analysis. B A P S A 27 560,HXa3,Burks. NUCLEAR R E A C T I O N S 78,8°,82Kr(aHe,d),E not given; m e a s u r e d c;(0). 79,81,83Rb deduced levels,J, ~,S. B A P S A 27 498,DYa9,Fortune. RADIOACTIVITY 77,S°Rb,79,SISr,Se,s3,84Y,S2,SSZr,86,STNb [ f r o m on-line separation]; m e a s u r e d f17 ,fl(fragment)-coin,ET,I7; d e d u c e d Q(EC),mass excess. R E P T IPN 1980 Annual,PR6,Della Negra. RADIOACTIVITY 79,SISr,Si,S2,ss,S4Y,St,oz,s3,s4,SSZr,SS,STNb [ f r o m 54Fe(32S,X),E=I01 MeV; 5SNi(32S, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,v(X-ray)-coin,Q(EC),Efl+,ET,17,E(X-ray),I(X-ray); deduced m a s s excess,log ft. s1,SaSr,SS,STZr,79Rb d e d u c e d levels,T~/~,7-branching. S2Sr,SaY d e d u c e d levels,7-branehing. R E P T IPN0-T-81-09,Della Negra. RADIOACTIVITY 79Sr,S°,s',82,eSY,83Zr [ f r o m 54Fe,5°Cr(32S,X),E=100-123 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s excess,log ft,B-end point energies. SSY,TSRb d e d u c e d levels,Ti/z,J,zr,v-multipolarity, s°,sl,s2,SaSr d e d u c e d levels,7-branehing, fl recoil tof m a s s s p e c t r o m e t e r , H e l i u m jet transport. R E P T IPNO-T-81-10,Jacquet.

231

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

81Sr

R 82ThZY:

a'y

D 81DeZD

81JaZU

81Zr

D 81DeZD

D 80HoZN D 80HoZN

81ZeZY a~As

D 81LiZP

R 81FIZW:

8~Se

D 81LiZP: R 81SaZK:

82DeZZ:

820gZZ:

S2Br

R 82AuZW:

SZSr

D 81DeZD:

81JaZU:

82HaZL:

SZy

D 80DeZB:

81DeZD:

81JaZU:

81

continued

NUCLEAR REACTIONS s 4 , S S F e ( 2 a S i , X ) , E = S O - 9 9 MeV; m e a s u r e d ET,IT,7(0),a(ET),77-coin, a(fragment) v s E; d e d u c e d e x i t c h a n n e l angular momentum effects. 79Rb,s°Sr deduced l e v e l s , a*Sr d e d u c e d l e v e l s , J , q u a s i r o t a t i o n a l b a n d s . DABBB 42 3 3 1 8 , T h e i s e n . R A D I O A C T I V I T Y 79,elSr,81,e~,s3,e4Y,Sl,a~,ss,a4,SSZr,SS,87Nb [ f r o m S~Fe(3~S,X),E=lOl MeV; 58Ni(3~S, X),E=I75 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,ET,IT,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . 6i,83Sr,S°,SVZr,?QRb d e d u c e d levels,Ti/~,7-branching. SZSr,SSY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y 7%r,S°,al,s~,S3y,S3Zr [ f r o m S4Fe,S6Cr(SZS,X),E=lO0-123 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . SSY,~SRb deduced levels,Tl/z,J,vr,7-multipolarity. 8°,ai,aa,e3Sr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a c q u e t . RADIOACTIVITY ~9,SiSr,Si,e~,as,e4Y,S*,s~,ss,s~,aSzr,aS,a~Nb [ f r o m S4Fe(S~S,X),E=IOl MeV; 58Ni(3~S, X),E=I75 MeV]; m e a s u r e d 77-,fl+7-,v(X-ray)-coin,Q(EC),Efl+,ET,17,E(X-ray),I(X-ray); deduced m a s s excess,log ft. s~,63Sr,SS,SVZr,~SRb deduced levels,Tl/~,7-branching. 8ZSr,S3Y deduced levels,7-branching. R E P T IPNO-T-81-09,Della Negra.

A 8aGa a~Ge

=

ONLY)

=

82

RADIOACTIVITY 79,8°,81,S2Ga,79,s°,si,S2Ge; m e a s u r e d E7,17,77-coin. R E P T NFL-22,Hoff. RADIOACTIVITY 79,s°,sl,S2Ga,TS,s°,s1,S2Ge; m e a s u r e d ET,17,77-coin. R E P T NFL-22,Hoff. RADIOACTIVITY s°,sl,SaGe [from spallation]; measured E7,17. REPT Univ Mainz,1980,Annual,Pl, Zendel. RADIOACTIVITY s°,s2,s3,S4As; m e a s u r e d ET,IT,77(t ). 82,S3Se deduced levels. B A P S A 26 1137, CDl3,Lien. NUCLEAR R E A C T I O N S 7°Zn,i°4Ru,n°pd,iS4Sm,lSa,lS°Gd,ls6W,196,1gSpt,2°2,2°4Hg,244Pu(polarized t,a), 19Spt,244pu,VSGe(polarized t,p),E=17 MeV; s2,S°Se,i°°Mo,i22,124Sn(polarized t,3He),E=22-25 MeV; m e a s u r e d a(0),analyzing p o w e r vs 0,a(Ea),a(Ep),a(3He). SSCu,*°aTc,1°SRh,iS3pm,lST,159Eu, lSSTa,iSs,lSVIr,a°l,Z°3Au,aa3Np,2°°Pt,24Spu,VSGe,S°,eZAs,l°°Nb,l~z,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . R A D I O A C T I V I T Y s°,s2,s3,S4As; m e a s u r e d E % I T , 7 7 ( t ) . sa,S3Se d e d u c e d l e v e l s . B A P S A 26 1137, CD13,Lien. NUCLEAR REACTIONS 74,76,~s,o°,S2Se(p,p'),E=65 MeV; m e a s u r e d a ( 0 ) , p r o t o n m o m e n t u m spectra; deduced two-step process. 74,7°,78,8°,82Se d e d u c e d levels,Jjr,excitation strengths. Coupled-channel,DWBA a n a l y s e s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 3 9 , S a k a m o t o . NUCLEAR REACTIONS 7 s , T s , s ° , S 2 S e ( p o l a r i z e d p , p ' ) , E = 1 6 MeV; m e a s u r e d a ( 0 ) , A ( 0 ) . 76,Ts,so,S2Se deduced deformation parameters. Coupled-channels method,rotation-vibration,asymmetric rotation m o d e l s . B A P S A 27 4 6 0 , A Y a 1 0 , D e l a r o c h e . NUCLEAR REACTIONS 7 4 , T s , v s , s ° , e 2 S e ( p o l a r i z e d p , p ) , ( p o l a r i z e d p,p'),E n o t g i v e n ; m e a s u r e d a n a l y z i n g p o w e r v s 0. 74,76,78,8°,83Se d e d u c e d J - d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP Osaka, 1981 A n n , P 1 6 , 0 g i n o . NUCLEAR REACTIONS 76Ge,S2Se,i2s,13OTe(p,n),E=135 MeV; m e a s u r e d a ( 0 ) , a ( E n ) . 76As,S2Br d e d u c e d L=O G a m o w - T e l l e r strength. 126,*3°Xe d e d u c e d t w o - f l p r o c e s s v i r t u a l state Gamow-Teller strength. B A P S A 27 7 3 1 , E E T , A u s t i n . R A D I O A C T I V I T Y 79,eiSr,Sl,e2,s3,S4y,SZ,s2,63,s4,SSZr,e6,e~Nb [ f r o m 54Fe(32S,X),E=lOl MeV; SSNi(32S, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,E%IT,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . 81,83Sr,aS,87Zr,79Rb d e d u c e d levels,Tl/¢,7-branching. 82Sr,S3Y d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - O S , D e l l a Negra. R A D I O A C T I V I T Y 7QSr,a°,al,s~,S3y,S3Zr [ f r o m S4Fe,SOCr(32S,X),E=100-123 MeV3; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . 83y,79Rb deduced levels,T,/2,JJr,7-multipolarity, s°,s*,s2,S3Sr d e d u c e d l e v e l s , v - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a c q u e t . R A D I O A C T I V I T Y 83Zr(fl+p),S~Mo(fl+p),StmRu(fl+p) [ f r o m 54Fe,SaNi(S,X),(Ca,X),E=140 MeV3; measured fl-delayed Ep,Ip,pT-,p(X-ray)-coin; S2Sr,SSZr l e v e l s d e d u c e d p r o t o n b r a n c h i n g . B A P S A 27 7 1 3 , C C l l , H a g b e r g . R A D I O A C T I V I T Y 77,8°Rb,Te,SlSr,82,s3,S4Y,Q2,SSZr,eS,S~Nb [ f r o m on-line separation]; measured flT-,fl(fragment)-coin,E%IT; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. RADIOACTIVITY 79,SISr,Si,S2,s3,S4y,Sl,82,s3,s4,SSZr,SS,eVNb [ f r o m 54Fe(3~S,X),E=I01 MeV; 58Ni(32S, X),E=I75 MeV3; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,E%l%E(X-ray),l(X-ray); deduced m a s s excess,log ft. 61,S3Sr,eS,SVZr,TSRb deduced levels,Ti/2,7-branching. 82Sr,S3Y d e d u c e d levels,7-branching. R E P T IPNO-T-81-09,DeIIa Negra. RADIOACTIVITY 7gSr,e°,ei,s2,S3y,S3Zr [ f r o m S4Fe,S°Cr(3~S,X),E=I00-123 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; deduced m a s s excess,log ft,fl-end point energies. S3y,~SRb deduced levels,T~/~,Jjr,v-multipolarity, ao,e1,sz,S3Sr deduced levels,v-branching, fl recoil tof m a s s spectrometer,Helium jet transport. R E P T IPNO-T-81-10,Jacquet.

232

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 82Zr

D 80DeZB:

81DeZD:

D 81LiZP:

83Se

D 81LiZP: R 78MoYV

81HoZU 83BF

R 81ZuZX

83Rb

R 82FoZY

83Sr

D 81DeZD

81JaZU

83y

D 80DeZB

81DeZD

81JaZU

81SaZ0

83Zr

D 81DeZD

81JaZU

81SaZ0

82HaZL

R 81LiZQ

82

continued

R A D I O A C T I V I T Y 77,a°Rb,79,OlSr,SZ,83,84y,ea,SSZr,8~,aTNb [ f r o m on-line separation]; measured fl7-,fl(fragment)-coin,ET,IT; deduced Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. R A D I O A C T I V I T Y 79,a[Sr,at,ea,a3,e4Y,Ol,s~,83,s4,a5Zr,S6,STNb [ f r o m 54Fe(3~S,X),E=101 MeV; 5aNi(3ZS, X ) , E = t 7 5 MeV']; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,ET,IT,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . sl,a3Sr,aS,eTZr,79Rb d e d u c e d levels,T~/a,-~-branching. 8aSr,a3Y d e d u c e d levels,-~-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra.

A 83As

=

ONLY)

=

83

R A D I O A C T I V I T Y B°,s2,s3,S4As; m e a s u r e d E T , I T , 7 7 ( t ) . s2,S3Se d e d u c e d l e v e l s . B A P S A 26 1137, CD13,Lien. R A D I O A C T I V I T Y s°,s2,83,e4As; m e a s u r e d E T , 1 7 , ~ 7 ( t ) . s2,S3Se d e d u c e d l e v e l s . BAPSA 26 1137, CD13,Lien. NUCLEAR REACTIONS 76,78,so,S2Se(polarized d,p),E=12.5 MeV; m e a s u r e d ff(0),vecter analyzing p o w e r v s 0. 77,79,81,83Se d e d u c e d levels,Jjr,S. Broad-range magnetic spectrograph. DWBA a n a l y s i s . THESIS L A M o n t e s t r u q u e , N o t r e Dame University. NUCLEAR REACTIONS 82Se(d,p),E=8 MeV; m e a s u r e d ET,7(t). S3Se l e v e l d e d u c e d T l / 2 , i n t r u d e r character. REPT A - T L U - 8 0 1980,Annual Report,P57,Hoff. NUCLEAR REACTIONS 76,Ts,e°,S2Se(3He,d),E=24 MeV; m e a s u r e d cr(0),cr(Ed); d e d u c e d Q. 77,79sl, S3Br d e d u c e d l e v e l s , L , S . DABBB 4 2 1 0 6 9 , Z u m b r o . NUCLEAR REACTIONS 7s,s°,82Kr(3He,d),E n o t g i v e n ; m e a s u r e d a(0). 79,81,83Rb d e d u c e d l e v e l s , J , ~,S. B A P S A 27 4 9 8 , D Y a 9 , F o r t u n e . R A D I O A C T I V I T Y 79,elSr,Sl,s2,s3,S4Y,Sl,s2,s3,a4,SSZr,86,STNb [ f r o m 54Fe(32S,X),E=lOl MeV; 5SNi(32S, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,ET,IT,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . 81,83Sr,86,STZr,79Rb d e d u c e d levels,Tl/z,7-branehing. 8aSr,83Y d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e I I a Negra. R A D I O A C T I V I T Y 79Sr,S°,el,sa,83Y,S3Zr [ f r o m 54Fe,S°Cr(32S,X),E=100-123 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . S3Y,T°Rb deduced levels,Tl/2,J,Tr,-/-multipolarity. 8°,el,s~,e3Sr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a c q u e t . R A D I O A C T I V I T Y 77,S°Rb,79,SlSr,Sa,e3,S4Y,82,85Zr,SS,STNb [ f r o m on-line separation]; measured fl7-,fl(fragment)-coin,ET,IT; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. R A D I O A C T I V I T Y 79,SlSr,Sl,82,s3,S4Y,81,sa,83,s4,85Zr,86,eTNb [ f r o m 54Fe(3aS,X),E=101 MeV; 58Ni(32S, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,E%lT,E(X-ray),l(X-ray); deduced m a s s e x c e s s , l o g f t . 81,e3Sr,SS,STZr,79Rb d e d u c e d levels,T1/~,7-branching. 8aSr,SSY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y 7°Sr,a8,sl,s2,e3Y,S3Zr [ f r o m S4Fe,5°Cr(3~S,X),E=100-1~3 MeV]; m e a s u r e d 77-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s . 93Y,79Rb deduced levels,Tl/2,JJr,7-multipolarity. 8°,al,aa,83Sr d e d u c e d l e v e l s , 7 - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a e q u e t . R A D I O A C T I V I T Y e3,e¢Zr,~4,e5Nb [ f r o m 59Ni(a~Si,X),(2eSi,X)]; m e a s u r e d E % I % E ( X - r a y ) , l ( X - r a y ) , Efl+,(X-ray)7-coin,77(t),7(X-ray)(t),flT(t); deduced Q(EC),mass excess. 83,S~Y,S~,85Zr deduced l e v e l s . B A P S A 26 l 1 3 7 , C D 1 2 , S a h a . R A D I O A C T I V I T Y 7g,alSr,ai,ea,83,e4Y,al,a~,s3,e4,SSZr,aa,eTNb [ f r o m 54Fe(3aS,X),E=101 MeV; 58Ni(32S, X),E=175 MeV]; m e a s u r e d 7~/-,fl+7-,~,(X-ray)-coin,Q(EC),Efl+,ET,I%E(X-ray),I(X-ray); d e d u c e d m a s s e x c e s s , l o g f t . 8~,83Sr,SS,S~Zr,79Rb d e d u c e d levels,Ti/a,7-branching, eaSr,S3Y d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y ~gSr,e°,a~,s2,S3y,a3Zr [ f r o m 54Fe,S°Cr(3~S,X),E=100-t~3 MeV]; m e a s u r e d 7"~-, 7(X-ray)-,Tfl+-coin,Efl+,Q(EC),Qfl; d e d u c e d m a s s e x c e s s , l o g f t , f l - e n d p o i n t e n e r g i e s , e3Y,7°Rb deduced levels,Tl/~,Jjr,~-multipolarity. 8°,81,8~,83Sr d e d u c e d l e v e l s , ~ / - b r a n c h i n g , fl r e c o i l tof mass spectrometer,Helium jet transport. REPT I P N O - T - 8 1 - 1 0 , J a e q u e t . R A D I O A C T I V I T Y s3,84Zr,8~,aSNb [ f r o m 5eNi(~%i,X),(a8Si,X)]; m e a s u r e d ET,I%E(X-ray),I(X-ray), Efl+,(X-ray)7-coin,77(t),7(X-ray)(t),fl-~(t); deduced Q(EC),mass excess, s3,e¢Y,et,~SZr d e d u c e d l e v e l s . B A P S A 36 l 1 3 7 , C D 1 2 , S a h a . R A D I O A C T I V I T Y 83Zr(fl~p),97Mo(fl+p),9tmRu(fl+p) [ f r o m 5~Fe,58Ni(S,X),(Ca,X),E=140 MeV]; measured fl-delayed Ep,Ip,pT-,p(X-ray)-coin; SaSr,aeZr l e v e l s d e d u c e d p r o t o n b r a n c h i n g . B A P S A ~7 7 1 3 , C C l l , H a g b e r g . NUCLEAR REACTIONS 58Ni(34Mg,X),E=65-t10 MeV; 58Ni(38Si,X),(agSi,X),E=80-130 MeV; 58Ni(3~S,X), E = 9 0 - 1 5 0 MeV; m e a s u r e d E~,I'~,7(t),n~-,nn~'-,~/7-coin. 79Sr,93Zr d e d u c e d l e v e l s . B A P S A 26 l137,CDll,Lister.

233

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 84As

D 81HeZV 81LiZP

84y

D 80DeZB

81DeZD

81SaZ0:

84Zr

D 81DeZD:

81SaZ0:

R 82ChZX: 84Nb

D 81SaZO:

D 81ShZS:

85Rb

R 800hZW:

85y

D 82RaZY:

85ZF

D 80DeZB:

81DeZD:

81SaZ0:

BSNb

D 81SaZ0:

R 810hZZ:

86y

R 82DaZW:

86Zr

D 81DeZD:

82DeZY:

=

85

RADIOACTIVITY 85As; m e a s u r e d f l - d e l a y e d n e u t r o n s p e c t r u m . Tof. REPT J U L - S p e z - 9 9 , P 6 0 , Shaanan. NUCLEAR REACTIONS R b ( n , X ) , E = 5 - 1 5 0 0 0 eV; m e a s u r e d t r a n s m i s s i o n ; d e d u c e d r e s o n a n c e s , p a r a m e t e r s . 85Rb d e d u c e d s t r e n g t h f u n c t i o n . REPT N E A N D C ( J ) - 6 7 / U , P 2 , 0 h k u b o . RADIOACTIVITY 85my [ f r o m 76Se(12C,2np),E=48 MeV]; m e a s u r e d TI/2,V(0,H,t); d e d u c e d g, c o n f i g u r a t i o n . BAPSA 27 2 6 , D F 9 , R a g h a v a n . RADIOACTIVITY ~7,S°Rb,79,SlSr,82,83,S4Y,S2,SSZr,S6,87Nb [from on-line separation]; measured f l T - , f l ( f r a g m e n t ) - c o i n , E v , I v ; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. RADIOACTIVITY 79,8'Sr,el,82,ss,94Y,8',82,83,e4,eSZr,S~,eTNb [ f r o m 54Fe(SaS,X),E=101 MeV; 58Ni(32S, X),E=175 MeV]; m e a s u r e d V V - , f l + V - , 7 ( X - r a y ) - c o i n , Q ( E C ) , E f l + , E v , I v , E ( X - r a y ) , l ( X - r a y ) ; d e d u c e d m a s s e x c e s s , l o g f t . 81,83Sr,86,87Zr,79Rb d e d u c e d l e v e l s , T 1 / 2 , 7 - b r a n c h i n g . 82Sr,83Y d e d u c e d levels,v-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. RADIOACTIVITY 83,84Zr,e4,85Nb [ f r o m 58Ni(egSi,X),(eSSi,X)3; m e a s u r e d E T , 1 7 , E ( X - r a y ) , I ( X - r a y ) , Ep+,(X-ray)7-coin,77(t),v(X-ray)(t),flT(t); deduced Q ( E C ) , m a s s e x c e s s , ss,84Y,S4,~SZr d e d u c e d l e v e l s . BAPSA 26 l137,CD12,Saha. RADIOACTIVITY 83,84Zr,S4,85Nb [ f r o m 58Ni(zgSi,X),(~eSi,X)3; m e a s u r e d E T , I v , E ( X - r a y ) , l ( X - r a y ) , Efl+,(X-ray)v-coin,77(t),7(X-ray)(t),flT(t); deduced Q ( E C ) , m a s s e x c e s s . ~3,~4y,S4,85Zr d e d u c e d l e v e l s . BAPSA 26 l137,CD12,Saha.

A 8eRb

84

RADIOACTIVITY ~4As; m e a s u r e d f l - s t r e n g t h f u n c t i o n ; d e d u c e d d e v i a t i o n s f r o m s t a t i s t i c a l m o d e l . BAPSA 26 l 1 3 7 , C D 1 4 , H e n r y . RADIOACTIVITY s°,9~,s~,e4As; m e a s u r e d ET,17,77(t). 8~,SSSe d e d u c e d l e v e l s . BAPSA 26 1137, CD13,Lien. RADIOACTIVITY ~v,~°Rb,~9,S'Sr,S~,s~,6~Y,8~,SSZr,S6,STNb [ f r o m o n - l i n e s e p a r a t i o n 3 ; m e a s u r e d f l T - , f l ( f r a g m e n t ) - c o i n , E T , I T ; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. RADIOACTIVITY ~9,S'Sr,8~,az,s3,84y,Sl,e~,ss,e4,SSZr,e°,STNb [ - f r o m 54Fe(3~S,X),E=101 MeV; 5eNi(3~S, X),E=175 MeV]; m e a s u r e d 7 7 - , f l + 7 - , T ( X - r a y ) - e o i n , Q ( E C ) , E f l + , E T , I 7 , E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d m a s s e x c e s s , l o g f t . e~,SSSr,Se,STZr,7~Rb d e d u c e d l e v e l s , T ~ / ~ , 7 - b r a n c h i n $ . 9~Sr,SaY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e l l a Negra. RADIOACTIVITY s~,S4Zr,e4,S5Nb [ f r o m 5SNi(~Si,X),(~SSi,X)]; m e a s u r e d E 7 , l T , E ( X - r a y ) , I ( X - r a y ) , Efl+,(X-ray)7-coin,77(t),7(X-ray)(t),f17(t); deduced Q ( E C ) , m a s s e x c e s s . 83,84y,84,85Zr d e d u c e d l e v e l s . BAPSA 26 l137,CD12,Saha. RADIOACTIVITY 79,SiSr,Sl,e~,e~,S¢Y,Sl,sz,s~,s4,SSZr,aS,eTNb [ f r o m 54Fe(~2S,X),E=101 MeV; 58Ni(saS, X),E=175 MeVS; m e a s u r e d 7 7 - , f l + 7 - , T ( X - r a y ) - c o i n , Q ( E C ) , E f l + , E T , I 7 , E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d m a s s e x c e s s , l o g f t . 8~,aSSr,86,STZr,~aRb d e d u c e d l e v e l s , T t / ~ , T - b r a n c h i n g . S~Sr,eaY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e I l a Negra. RADIOACTIVITY ss,e4Zr,S4,SSNb [ f r o m 5aNi(2~Si,X),(ZgSi,X)]; m e a s u r e d E T , I T , E ( X - r a y ) , I ( X - r a y ) , Efl+,(X-ray)7-coin,77(t),7(X-ray)(t),flT(t); deduced Q(EC),mass excess, es,~Y,~%BaZr d e d u c e d l e v e l s . BAPSA 26 l137,CD12,Saha. NUCLEAR REACTIONS 5 8 N i ( 2 9 S i , n 2 p ) , E = 8 3 - 9 2 MeV; m e a s u r e d 7 ( 0 ) , 7 7 - , n 7 - c o i n , a ( E T ) . 84Zr d e d u c e d l e v e l s , J , ~ . BAPSA 27 4 9 8 , D Y a 1 0 , C h a p u r a n . RADIOACTIVITY s~,6aZr,S4,SSNb [ f r o m 5SNi(~Si,X),(2~Si,X)]; m e a s u r e d E T , I T , E ( X - r a y ) , l ( X - r a y ) , Efl+,(X-ray)T-coin,77(t),7(X-ray)(t),flT(t); deduced Q ( E C ) , m a s s e x c e s s , s~,S4Y,S~,95Zr d e d u c e d l e v e l s . BAPSA 28 l137,CD12,Saha.

A 85As

=

ONLY)

=

86

NUCLEAR REACTIONS 85Rb(n,X),E-0.1-17 keV; m e a s u r e d t r a n s m i s s i o n ; 87Rb(n,X),(n,7),E=0.2-23 keV; m e a s u r e d transmission,a(capture), e6,eSRb d e d u c e d resonance parameters. Tof s p e c t r o m e t e r . REPT N E A N D C ( J ) - 7 5 / U , P 4 , 0 h k u b o . NUCLEAR REACTIONS 85Rb(c~,3n),E=50 MeV; m e a s u r e d ET,IT,77-coin,7(0). S6y d e d u c e d levels,J, n,7-branching. REPT I N D C ( A R G ) - 9 / G , P b l , D a v i d s o n . RADIOACTIVITY 79,elSr,S',sz,ss,84Y,81,sz,ss,s4,eSZr,e6,87Nb [ f r o m 54Fe(32S,X),E=101 MeV; 58Ni(32S, X),E=175 MeV]; m e a s u r e d 7 7 - , f l + 7 - , 7 ( X - r a y ) - c o i n , Q ( E C ) , E f l + , E T , I T , E ( X - r a y ) , I ( X - r a y ) ; d e d u c e d m a s s e x c e s s , l o g f t . 81,sSSF,86,87Zr,79Rb d e d u c e d l e v e l s , T , / ¢ , 7 - b r a n e h i n g . 82Sr,eSY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e I I a Negra. RADIOACTIVITY e6,e7Nb,eTMo [ f r o m 58Ni(32S,X)]; m e a s u r e d E T , I 7 , 7 7 - , ( X - r a y ) 7 - , f l + 7 c o i n ; d e d u c e d TI/z,Q(EC). 86,87Zr,eTNb d e d u c e d l e v e l s . BAPSA 27 4 9 9 , D Y a 1 2 , D e w b e r r y .

234

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 86Zr

D 82HaZL:

a6Nb

D

BODeZB:

81DeZD:

82DeZY:

D 82RaZS D 82RaZS R 82RaZS

87Sr

R 82BuZU

87ZF

D 81DeZD

82DeZY

87Nb

D 80DeZB

81DeZD:

82DeZY: 87Mo

D 82DeZY: 82HaZL:

D 81MaZK:

SgBr

D 81MaZK:

88Rb

R 810hZZ:

88Sr

R 82VaZV:

88Zr

D 820xZZ: R 80GaZ0: 81RaZM:

8SNb

D 820xZZ:

continued

=

87

R A D I O A C T I V I T Y SVBr(fl-); m e a s u r e d EV,I V. 87Kr d e d u c e d l e v e l s . BAPSA 27 7 2 7 , E C 2 , R a m a n . R A D I O A C T I V I T Y SVBr(fl-); m e a s u r e d EV,Iv. 87Kr d e d u c e d l e v e l s . BAPSA 27 7 2 7 , E C 2 , R a m a n . NUCLEAR REACTIONS a g K r ( n , 7 ) , ( n , X ) , E n o t g i v e n ; m e a s u r e d a(capture),transmission. 87Kr deduced resonanees,Fn. B A P S A 27 7 2 7 , E C 2 , R a m a n . NUCLEAR REACTIONS 8 6 S r ( p o l a r i z e d d,p),(polarized d , d ) , E = l l MeV; m e a s u r e d ~(O),vector a n a l y z i n g p o w e r v s 0. 87St l e v e l s d e d u c e d L,Jjr,S. O p t i c a l m o d e l , D W B A a n a l y s e s . BAPSA 27 727,EC1,Burks. R A D I O A C T I V I T Y 79,SlSr,al,sz,ss,a4Y,Sl,gz,83,s4,85Zr,SS,8~Nb [ f r o m 54Fe(3aS,X),E=101 MeV; 5SNi(saS, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,T(X-ray)-coin,Q(EC),Efl+,E%IT,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . sl,SSSr,aS,87Zr,VgRb d e d u c e d levels,Tl/a,v-branching. S2Sr,BSY d e d u c e d levels,v-branching. REPT I P N 0 - T - 8 1 - 0 9 , D e l l a Negra. R A D I O A C T I V I T Y sg,S7Nb,gVMo [ f r o m 5SNi(sZS,X)]; m e a s u r e d Ev,IT,TV-,(X-ray)T-,fl+T-coin; d e d u c e d Tt/z,Q(EC). 86,87Zr,87Nb d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 2 , D e w b e r r y . R A D I O A C T I V I T Y 77,8°Rb,79,SlSr,82,a3,84Y,ga,S%r,Sg,SVNb [ f r o m on-line separation]; measured flT-,fl(fragment)-coin,Ev,Iv; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R g , D e l l a Negra. R A D I O A C T I V I T Y 79,gtSr,Si,s~,83,S4Y,al,ga,83,84,S5Zr,ag,SVNb [ f r o m 54Fe(aaS,X),E=101 MeV; 5SNi(32S, X),E=175 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,Ev,I%E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . al,83Sr,Sg,eVZr,79Rb d e d u c e d levels,Tl/2,T-branching. 82Sr,SSY d e d u c e d levels,7-branching. REPT I P N O - T - 8 1 - 0 9 , D e I l a Negra. R A D I O A C T I V I T Y sg,87Nb,87Mo [ f r o m 58Ni(3aS,X)]; m e a s u r e d Ev,17,77-,(X-ray)T-,fl+V-coin; d e d u c e d Ti/a,Q(EC). sg,SVZr,SVNb d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 2 , D e w b e r r y . R A D I O A C T I V I T Y se,SVNb,S7Mo [ f r o m 5SNi(32S,X)]; m e a s u r e d Ev,Iv,77-,(X-ray)T-,fl+7-coin; d e d u c e d T1/a,Q(EC ). ag,SVZr,eVNb d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 2 , D e w b e r r y . R A D I O A C T I V I T Y 83Zr(fl+p),87Mo(fl+p),gtmRu(fl+p) [ f r o m 5~-Fe,58Ni(S,X),(Ca,X),E=I40 MeV]; measured fl-delayed Ep,Ip,pT-,p(X-ray)-eoin; 8ZSr,SgZr l e v e l s d e d u c e d p r o t o n b r a n c h i n g . B A P S A 27 7 1 3 , C C l l , H a g b e r g .

A

88Se

86

R A D I O A C T I V I T Y aSZr(fl+p),BVMo(fl+p),91mRu(fl+p) [ f r o m 54Fe,SONi(S,X),(Ca,X),E=t40 MeVS; measured fl-delayed Ep,Ip,pv-,p(X-ray)-coin; S2Sr,86Zr l e v e l s d e d u c e d p r o t o n b r a n c h i n g . B A P S A 27 7 1 3 , C C l l , H a g b e r g . R A D I O A C T I V I T Y 77,S°Rb,79,SlSr,82,a3,a4Y,gZ,SSZr,Sg,aVNb [ f r o m on-line separation]; measured flV-,fl(fragment)-coin,E7,Iv; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT IPN 1980 A n n u a l , P R 6 , D e l l a Negra. R A D I O A C T I V I T Y 79,StSr,at,sz,s3,S4Y,St,s2,B3,84,SSZr,86,87Nb [ f r o m S4Fe(3aS,X),E=101 MeV; 58Ni(3ZS, X),E=I75 MeV]; m e a s u r e d 77-,fl+7-,7(X-ray)-coin,Q(EC),Efl+,E~f,17,E(X-ray),I(X-ray); deduced m a s s e x c e s s , l o g f t . al,aSSr,SS,SVZr,79Rb d e d u c e d levels,T~/8,v-branching, eaSt,saY d e d u c e d levels,v-branching. REPT I P N 0 - T - 8 1 - 0 9 , D e I l a Negra. R A D I O A C T I V I T Y 8s,87Nb,87Mo [ f r o m 58Ni(3aS,X)]; m e a s u r e d Ev,Iv,77-,(X-ray)7-,fl+7-coin; d e d u c e d T1/a,Q(EC). 8s,SVZr,SVNb d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 2 , D e w b e r r y .

A 87Br 87Kr

=

ONLY)

=

88

R A D I O A C T I V I T Y 8SSe; m e a s u r e d ET,Iv,vv(t). SSBr d e d u c e d levels. S h e l l m o d e l . BAPSA 26 1137, CD15,Massey. R A D I O A C T I V I T Y BaSe; m e a s u r e d Ev,Iv,vT(t). 88Br d e d u c e d l e v e l s . S h e l l m o d e l . BAPSA 26 1137, CD15,Massey. NUCLEAR REACTIONS SSRb(n,X),E=0.I-17 keV; m e a s u r e d t r a n s m i s s i o n ; 87Rb(n,X),(n,v),E=0.2-23 keV; measured transmission,a(capture), sg,SgRb d e d u c e d resonance parameters. Tof spectrometer. REPT N E A N D C ( J ) - 7 5 / U , P 4 , 0 h k u b o . NUCLEAR REACTIONS 94Mo,OaZr(d,eLi),E n o t g i v e n ; m e a s u r e d a(0),~(E(6)). 9°Zr,SaSr d e d u c e d pair vibrational excitation r a t i o . REPT KVI 1981 A n n , P 1 8 , v a n den Berg. R A D I O A C T I V I T Y 88Nb [ f r o m 9°Zr(p,3n)J; m e a s u r e d f l - , T - d e c a y . 88Nb d e d u c e d isomers,T1/2,decay characteristics. 88Zr d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a l l , 0 x o r n . NUCLEAR REACTIONS 9 0 Z r , l l g S n , a ° s P b ( a , 6 H e ) , E = 3 1 8 MeV; m e a s u r e d atE(SHe)). 88Zr,tlgSn,a°gpb deduced levels,broad structures. REPT IPN 1980 A n n u a l , P N 1 4 , G a l e s . NUCLEAR REACTIONS Se(160,X),(IZC,X),E n o t g i v e n ; m e a s u r e d 7(O,H,t). 9°,9a,94Mo,88Zr d e d u c e d isomer state quadrupole moment. Recoil i m p l a n t a t i o n i n Zr. BAPSA 26 l 1 4 6 , D D 2 , R a g h a v a n . R A D I O A C T I V I T Y SgNb [ f r o m 9°Zr(p,3n)q; m e a s u r e d f l - , 7 - d e e a y . 8SNb d e d u c e d i s o m e r s , T l / z , d e c a y characteristics. 88Zr d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a l l ; O x o r n .

235

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

89Rb

R 82StZY:

89y

R 80ArZT: 80StZM:

82YaZU 89Zr

R 80DuZS 80DuZT

R 82NiZY

9OZr

R 80LeZJ 80LeZK

80MaZB 80MoZE: 81DjZR:

81FuZX:

81TaZO:

82AoZY:

82CoZZ:

82SjZZ: 82TaZX:

82VaZV: 99Mo

R 81RaZM:

R 82DrZY:

91Zr

R 79AvZX: 82HaZQ:

=

90

NUCLEAR REACTIONS 89y(n,n),E=2.6-30 keV; m e a s u r e d a(O). 90y d e d u c e d p - w a v e r e s o n a n c e s , J , spin channel contribution. REPT J I N R - E 3 - 8 2 - 3 3 6 , N i k o l e n k o . NUCLEAR REACTIONS 9°Zr(13C,13C'),E=109 MeV; m e a s u r e d a(E(13C)). 9°Zr d e d u c e d low e n e r g y o c t u p o l e r e s o n a n c e e x c i t a t i o n . REPT ISN 8 0 - 0 1 , P 4 5 , L e b r u n . NUCLEAR REACTIONS 6 ° N i , 9 ° Z r , l ' S I n , ~ 2 ° S n , 1 4 4 S m , 1 6 5 H o , ' 9 7 A u , 2 ° S p b ( 3 H e , 3 H e ' ) , E = 1 0 8 . 5 MeV; m e a s u r e d a ( E ( 3 H e ) ) , a ( 0 ) . 6°Ni d e d u c e d GQR,F. 9°Zr,nSln,12°Sn,144Sm,lSSHo,197Au d e d u c e d GQR, g i a n t m o n o p o l e r e s o n a n c e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS 9OZr(~+,Tr+'),E=226 MeV; m e a s u r e d a ( E ( ~ r ) ) , a ( 0 ) . 9°Zr d e d u c e d T = I , quadrupole,monopole r e s o n a n c e s . REPT ISN 8 0 - 0 1 , P 4 8 , M a r t y . NUCLEAR REACTIONS 9°Zr,12°Sn,2°sPb((x,(~'),E=100,172 MeV; m e a s u r e d a ( E a ' ) . 9°Zr,12°Sn,2°ePb d e d u c e d G Q R , g i a n t m o n o p o l e r e s o n a n c e s , F . REPT J U L - S p e z - 7 2 , P S , M o r s c h . NUCLEAR REACTIONS 4°Ca,51V,58,6°,62Ni,68Zn,SO,92,94,9°Zr,92,g4,96,se,lO°Mo,12°,124Sn,'4°Ce(p,p'), E=201 MeV; m e a s u r e d a ( E p ' ) . 4°Ca,5~V,Se,66,62Ni,SeZn,g°,92,o4,O6Zr,92,94,96,98,~°°Mo,~2°,~24Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 9 ° Z r ( p , p ' ) , E = 6 5 MeV; m e a s u r e d a ( 0 ) . 9°Zr d e d u c e d particle-hole m u l t i p l e t e x c i t a t i o n . DWBA a n a l y s i s , m i c r o s c o p i c f o r m f a c t o r s . REPT RCNP 0 s a k a , 1 9 8 0 A n n , P43,Fujiwara. NUCLEAR REACTIONS 9°Zr(a,a'7),E=100 MeV; m e a s u r e d a-y(O). 9°Zr d e d u c e d low e n e r g y o c t u p o l e decay characteristics. NaI(T1) s c i n t i l l a t i o n spectrometers. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 5 , Tanaka. NUCLEAR REACTIONS 92Zr,13aBa(polarized p,t),E=28.5 MeV; m e a s u r e d a ( 0 ) , v e c t o r a n a l y z i n g p o w e r v s 0; d e d u c e d r e a c t i o n m e c h a n i s m . 9°Zr l e v e l d e d u c e d L=0 t r a n s f e r competing mechanisms. First-,second-order D W B A , m u l t i - s t e p p r o c e s s e s . REPT INS T o k y o 1981 A n n , P 2 3 , Aoki. NUCLEAR REACTIONS 9o,92Zr(a,a),(a,a'),E=104 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l parameters. 96,92Zr deduced T=0,quadrupole,hexadeeapole transition rates. Coupled-channels method,extended optical potential,semi-microscopic folding model, anharmonic v i b r a t o r . REPT K f K - 3 1 0 5 , C o r c a l c i u c . NUCLEAR REACTIONS 9°Zr,208pb(160,~O'),E=400 MeV; m e a s u r e d a(0). 9°Zr,~°spb d e d u c e d g i a n t r e s o n a n c e s . BAPSA 27 7 3 2 , E E l t , S j o r e e n . NUCLEAR REACTIONS 9°Zr(a,a'),E=99.3 MeV; m e a s u r e d a(Ea'),aT-coin,aT(O). 9°Zr d e d u c e d low energy octupole resonance,decay m e c h a n i s m , B ( E 1 ) / B ( E 3 ) . REPT RCNP Osaka,1981 A n n , P 5 2 , Tanaka. NUCLEAR REACTIONS 9aMo,~Zr(d,SLi),E n o t g i v e n ; m e a s u r e d a ( 0 ) , a ( E ( a ) ) . 9°Zr,SeSr d e d u c e d pair vibrational excitation r a t i o . REPT KVI 1981 A n n , P 1 8 , v a n d e n Berg. NUCLEAR REACTIONS Se(t60,X),(lZC,X),E n o t g i v e n ; m e a s u r e d 7(0,H,t). 9°,9u,a~Mo,SeZr d e d u c e d i s o m e r s t a t e q u a d r u p o l e m o m e n t . Recoil i m p l a n t a t i o n i n Zr. BAPSA 26 l 1 4 6 , D D 2 , R a g h a v a n .

A 91y

89

NUCLEAR REACTIONS 6SKr(cx,p),E n o t g i v e n ; m e a s u r e d a(0). SSRb l e v e l s d e d u c e d J,~r. DWBA analysis,particle-vibrator m o d e l . BAPSA 27 5 6 1 , H X a 1 2 , S t e p h a n s . NUCLEAR REACTIONS 89Y(~+,Tr+')(~r-,~r-'),E=163 MeV; m e a s u r e d a(E(rr)),cr(0). SSy d e d u c e d g i a n t r e s o n a n c e , F . DWIA c a l c u l a t i o n s . REPT ISN 8 0 - 0 1 , P 4 6 , A r v i e u x . NUCLEAR REACTIONS 9 ° Z r , ~ 4 4 S m ( p o l a r i z e d d,3He),E=52 MeV; m e a s u r e d a ( E ( 3 H e ) ) , a ( 0 ) , i T l t ( 0 ) ; deduced spin-orbit s p l i t t i n g , aSY,i~3pm d e d u c e d h o l e - s t a t e d o m i n a n c e . Z e r o - r a n g e DWBA. REPT K f K - 3 0 6 8 , P 2 7 , S t u i r b r i n k . NUCLEAR REACTIONS eSy(n,n),(n,n'),E=ll MeV; m e a s u r e d a(0). eSy levels d e d u c e d d e f o r m a t i o n parameters. O p t i c a l m o d e l , D W B A a n a l y s e s . BAPSA 27 6 2 8 , H 5 , Y a n Y i - M i n g . NUCLEAR REACTIONS 9°Zr,OeMo(3He,(x),E=97.3 MeV; m e a s u r e d cr(E(x). 89Zr,S~Mo d e d u c e d l f y / z fragmentation,T(<),T(>) components. REPT IPN 1980 A n n u a l , P N 1 2 , D u h a m e l . NUCLEAR REACTIONS 9°Zr,9~Mo(3He,a),E=100 MeV; m e a s u r e d a(Ecx). 89Zr,9*Mo d e d u c e d IAS, inner-shell pickup structure. REPT ISN 8 0 - 0 1 , P 4 9 , D u h a m e l .

A 99y

=

ONLY)

=

91

NUCLEAR REACTIONS SlZr(p,np),E=16 MeV; m e a s u r e d p n - c o i n ; d e d u c e d p r e n e u t r o n , p r e p r o t o n emission mechanism. 91y d e d u c e d IAS. BAPSA 27 713,CC12,Drake. NUCLEAR REACTIONS 91Zr(n,n'7),E=fast; m e a s u r e d ET,T(0); d e d u c e d A 2. 91Zr l e v e l s d e d u c e d J, ~,~. CONF R i g a , P 5 6 8 , A v c h u k h o v . NUCLEAR REACTIONS 58Ni,9°Zr(polarized d,p),E=56 MeV; m e a s u r e d (;(0),vector a n a l y z i n g p o w e r v s 0. 59Ni,SlZr l e v e l s d e d u c e d t r a n s f e r e d nucleon quantum number d e p e n d e n c e . DWBA a n a l y s i s . REPT RCNP Osaka,1981 A n n , P 2 8 , H a t a n a k a .

236

SECONDARY

SOURCES

(Reports,Abs[rac[s,etc.

A 91Zr

R 82RaZR:

91Nb

R 81FuZW: 81MaZF:

91Mo

R 80DuZS: 80DuZT:

9~Ru

D 83HaZL:

D 80JuZY

9aSF

D 80JuZY

9ZZr

R 80ToZS

81DjZR

82CoZZ:

92Mo

R 79IvZX

81DjZR

81RaZM 82ToZV

9aTe

D 81DiZS

R BtQaZY:

93Nb

R 31BhZY:

93Mo

R 32ToZV:

93Tc

R 81AyZZ:

continued

=

93

R A D I O A C T I V I T Y 9a,94,9s,98,1°°Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n I'y,'yT(O),"yT-coin,I(ce),fl-delayed n e u t r o n s . SaSr deduced n e u t r o n

p r o d u c t s 3 ; m e a s u r e d ET, emission probability. 94 ICC,B(E2). gSSr [ f r o m gSRb

9a,°6,gaSr l e v e l s d e d u c e d 6,J,Tr,7-branching. 9~,9aSr d e d u c e d decay3; measured f l - / - c o i n , l ( c e ) , ' ) , 7 ( 0 ) , E T , I 7. 98y d e d u c e d levels,6(M1/ES),6(E1/MS), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. R A D I O A C T I V I T Y 92,g4,g6,gs,l°°Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s 3 ; m e a s u r e d E 7, I%~7(0),75,-eoin,I(ce),fl-delayed neutrons. 9SSr d e d u c e d n e u t r o n emission probability. 94 ga,ss,SeSr l e v e l s d e d u c e d 6,JJr,~,-branching. 96,99Sr d e d u c e d ICC,B(E2). 96Sr E f r o m 9~Rb decay]; measured fl-/-coin,I(ce),77(0),E*/,I~/, gay deduced levels,6(M1/E2),6(E1/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. NUCLEAR REACTIONS 6aNiflZZr(d,d'),E=64.7 MeV; m e a s u r e d (7(Ed),a(0). 6ZNi,SaZr d e d u c e d EWSR strength distribution,deformation parameter f o r l o w e n e r g y o c t u p o l e r e s o n a n c e s . DWBA a n a l y s i s . REPT INS T o k y o 1980 A n n , P 3 9 , T o h e i . NUCLEAR REACTIONS 40Ca,51v,5S,6°,SaNi,SSZn,e°,ga,94,OSZr,9Z,94,9s,99,1°°Mo,lao,~U4Sn,14OCe(p,p'), E=201 MeV; m e a s u r e d (~(Ep'). 4OCa,51v,5S,e°,SaNi,aSZn,SO,Oa,o%SSZr,9a,94,os,gs,l°°Mo,ia°,~4Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 9°,92Zr(a,a),(a,a'),E=104 MeV; m e a s u r e d at0); deduced optical model parameters. 9°,9ZZr deduced T=0,quadrupole,hexadecapole transition rates. Coupled-channels method,extended optical potential,semi-microscopic folding model, anharmonic vibrator. REPT K f K - 3 1 0 5 , C o r e a l c i u c . NUCLEAR REACTIONS 9a,ss,gSMo,ng,ia4Sn(a,~),(a,a'),E=29.3,49,45,50 MeV~ m e a s u r e d or(E,0), s2, 96,SSMo,its,ta4Sn d e d u c e d d e f o r m a t i o n parameter ft. B l a i r p h a s e m e t h o d . CONF R i g a , P 3 2 1 , Ivanov. NUCLEAR REACTIONS 4°Ca,51V,aS,so,saNi,SSZn,9O,Se,94,SSZr,92,94,gs,gs,lOOMo,12°,124Sn,140Ce(p,p,), E = 2 0 1 MeV; m e a s u r e d ~ ( E p ' ) . 40Ca,Slv,Sg,6°,62Ni,69zn,gO,sZ,s4,gSzr,g~,94,ss,98,tOOMo,lZ°,t24Sn d e d u c e d M1 r e s o n a n e e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS Se(IS0,x),(~aC,X),E n o t g i v e n ; m e a s u r e d 7(0,H,t). 9°,9~,94Mo,gaZr d e d u c e d isomer state quadrupole moment. Recoil i m p l a n t a t i o n i n Zr. BAPSA 26 1 1 4 6 , D D 2 , R a g h a v a n . NUCLEAR REACTIONS g 2 , g 4 M o ( a , a ' ) , E = 6 4 . 4 MeV; m e a s u r e d cr(Ea'),(~(0). 9a,gSMo d e d u c e d l o w e n e r g y o c t u p o l e r e s o n a n c e s , E W S R . QSD m a g n e t i c spectrograph. DWBA a n a l y s i s . REPT INS T o k y o 1981 A n n , P 2 4 , T o h e i . R A D I O A C T I V I T Y 9~Tc [ f r o m 9aMo(3He,2np)]; m e a s u r e d 7 7 - c o i n ; d e d u c e d y r a s t l e v e l s , J . S h e l l m o d e l . REPT D O E / E R / 4 0 0 1 4 - 3 , P 3 9 , D i a n a .

A

93iF

91

NUCLEAR REACTIONS 8ZSe(13C,4n),E=40 MeV; m e a s u r e d -~(0,H,t). 91ZF d e d u c e d i s o m e r g. BAPSA 27 7 2 7 , E C 3 , R a g h a v a n . NUCLEAR REACTIONS g°Zr(aHe,d),E=89.3 MeV; m e a s u r e d c~(Ed),a(0), atNb l e v e l s d e d u c e d CaS. DWBA a n a l y s i s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 6 5 , F u j i w a r a . NUCLEAR REACTIONS ZSsi,54Fe,5SNi(aHe,aHe),(SHe,d),E=89.3 MeV; 9 ° Z r , l Z 4 S n ( a H e , a H e ) , ( a H e , d ) , E=89.8 MeV; m e a s u r e d or(0), agP,55Co,59Cu,giNb,XZ5Sb l e v e l s d e d u c e d CaS. F i n i t e - r a n g e DWBA analysis,nonlocal potentials. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 9 , M a t s u o k a . NUCLEAR REACTIONS gOZr,gZMo(SHe,a),E=97.3 MeV; m e a s u r e d c~(Ea). S%r,glMo d e d u c e d l f T / z fragmentation,T(<),T(>) components. REPT IPN 1989 A n n u a l , P N 1 2 , D u h a m e l . NUCLEAR REACTIONS 9°Zr,gaMo(aHe,(~),E=100 MeV; m e a s u r e d c~(Ea). SSZr,9~Mo d e d u c e d IAS, inner-shell pickup structure. REPT ISN 8 0 - 0 1 , P 4 9 , D u h a m e l . R A D I O A C T I V I T Y SSZr(fl+p),aTMo(fl+p),g~mRu(fl+p) [ f r o m 54Fe,5SNi(S,X),(Ca,X),E=140 MeV3; measured fl-delayed Ep,Ip,pT-,p(X-ray)-coin; SaSr,S~Zr l e v e l s d e d u c e d p r o t o n b r a n c h i n g . B A P S A 27 7 1 3 , C C l l , H a g b e r g .

A 9ZRb

=

ONLY)

=

93

NUCLEAR REACTIONS 4 4 C a , 4 9 T i , S ° C r , S T , S S Z n , S 2 Z r , 9 7 , 9 8 M o ( n , d ) , ( n , n , p ) , ( n , n p ) , E = 1 4 . 7 MeV; measured cr; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,51Cr,6S,Sazn,Sazr,98,SaMo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 0 , Q a i m . NUCLEAR REACTIONS 9 3 N b ( d , d ' ) , E = 1 7 . 5 MeV; m e a s u r e d a ( E d ' ) . 93Nb d e d u c e d go/a-proton fragmentation. Particle-core c o u p l i n g m o d e l . REPT D O E / E R / 4 0 0 1 4 - 3 , P 2 8 , B h a n g . NUCLEAR REACTIONS 9 a , 9 4 M o ( a , a ' ) , E = 6 4 . 4 MeV; m e a s u r e d cr(Ea'),cT(0), us,geMs d e d u c e d l o w e n e r g y o c t u p o l e r e s o n a n c e s , E W S R . Q2D m a g n e t i c spectrograph. DWBA a n a l y s i s . REPT INS T o k y o 1981 A n n , P 2 4 , T o h e i . NUCLEAR REACTIONS 9aMo(p,'),),E=2-2.68 MeV; m e a s u r e d cr(E~). 9aTc level d e d u c e d t e n t a t i v e J, ~r. CONF H e l s i n g o r V o l l P 2 4 7 , CERN 8 1 - 0 9 .

237

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

93Tc

R 82ViZZ:

93Ru

D 80AyZY: 81AyZZ:

D

79WaZU:

80JuZY:

82DaZY: 820kZV: 94Sr

D 8OJuZY:

82DaZY: 94Zr

R

81DjZR:

94Nb

R

79DoZW 79WiZG

94Mo

R 79LeZL 81DjZR

81RaZM: 94Tc

R 82BeZS:

94Ru

D 81NoZY:

R 79LeZL: 82LiZM:

D 82DaZY: 82YeZZ:

95Sr

D 82DaZY:

continued

=

94

R A D I O A C T I V I T Y 94,96Rb,143,144Cs [ f r o m on-line separation]; measured ET,I?; d e d u c e d fl-delayed neutron emission probability. CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products), P311,Warner. R A D I O A C T I V I T Y 92,94,96,98,1°°Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E?, 17,77(0),77-coin,I(ce),fl-delayed neutrons. 98Sr d e d u c e d n e u t r o n emission probability, g4 9z,9~,gSSr l e v e l s d e d u c e d 6,J,~r,7-branching. 96,98Sr d e d u c e d ICC,B(E2). 96Sr [ f r o m 96Rb decay]; measured flT-coin,I(ce),77(O),E?,I?. 96y d e d u c e d levels,6(M1/E2),(5(E1/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. RADIOACTIVITY 94,95,96,97Rb; m e a s u r e d Efl,Ifl; deduced Q]?. 94,95,99,97Sr [ f r o m 94,95,96,97Rb decay]; measured Eft,I]?; d e d u c e d Qfl. B A P S A 27 4 9 9 , D Y a 1 4 , D a u t e t . RADIOACTIVITY 94Rb(]?-),(n); measured ]?-delayed neutron emission probability. REPT NEAN D C ( J ) - 8 3 / U , P 4 4 , 0 k a n o . R A D I O A C T I V I T Y 92,94,96,99,i°9Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d ET, IT,77(0),77-coin,I(ce),]?-delayed neutrons. 96Sr d e d u c e d n e u t r o n emission probability. 94 9z,96,98Sr l e v e l s d e d u c e d 6,J,lr,7-branching. 96,9aSr d e d u c e d ICC,B(E2). 96Sr [ f r o m 96Rb decay]; measured f17-coin,I(ce),77(0),ET,I7. 96y d e d u c e d levels,6(M1/E2),6(E1/M2), configuration. THESIS C J u n g , J u s t u s Liebig-Universitat. R A D I O A C T I V I T Y 94,95,96,97Rb; m e a s u r e d Eft,I]?; d e d u c e d Qfl. 94,95,98,97Sr [ f r o m 94,95,96,97Rb decay]; measured Eft,I]?; d e d u c e d Q]?. B A P S A 27 4 9 9 , D Y a 1 4 , D a u t e t . NUCLEAR REACTIONS 4°Ca,51v,Sa,6°,S2Ni,6eZn,9°,ga,94,96Zr,92,94,96,ga,i°OMo,Z2°,la4Sn,Z4°Ce(p,p'), E=Z01 MeV; m e a s u r e d a ( E p ' ) . 4°Ca,51V,Se,ao,62Ni,6eZn,g°io2,94,96Zr,O2,94,98,ge,z°°Mo,126,124Sn deduced M1 r e s o n a n c e , F . REPT IPN 1981 Annual,PN62,DjalalJ. NUCLEAR REACTIONS 9 4 Z r ( p , n T ) , E = 3 . 3 MeV; m e a s u r e d E7,I 7. 94Nb d e d u c e d transitions. Enriched t a r g e t s , G e ( L i ) d e t e c t o r . CONF R i g a , P 5 7 8 , D o m b r a d i . NUCLEAR REACTIONS 9 3 N b ( n , n ) , ( n , 7 ) , ( n , X ) , E < 7 keV; measured o'(total),a(elastic), a(capture),transmission. 94Nb d e d u c e d s-,p-wave strength functions,< F 7 >. REPT NEANDC(E)-202U,Vol III,P14,Winter. NUCLEAR REACTIONS 99Zr,92Mo(a,2n7),E=27 MeV; m e a s u r e d 7(0,H,t). 94Mo,94Ru l e v e l s d e d u c e d g, configurations. CONF R i g a , P 2 4 3 , L e b e d e v . NUCLEAR REACTIONS 4°Ca,51v,Se,6°,aaNi,68Zn,gO,92,94,96Zr,92,94,96,gs,l°°Mo,12o,t24Sn,14°Ce(p,p'), E=201 MeV; m e a s u r e d a ( E p ' ) . 40Ca,SZv,Sa,so,6~Ni,68Zn,9°,92,94,96Zr,92,94,gs,es,lO°Mo,12°,124Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS Se(160,X),(lZC,X),E n o t g i v e n ; m e a s u r e d 7(0,H,t). 9°,92,94Mo,aSZr d e d u c e d isomer state quadrupole moment. Recoil i m p l a n t a t i o n i n Zr. BAPSA 26 l 1 4 6 , D D 2 , R a g h a v a n . NUCLEAR REACTIONS 99Nb(a,3n),E=30-55 MeV; m e a s u r e d E T , I T , T T - c o i n , - / ( 8 ) , a ( E - / , E ) . 94Tc deduced levels,isomer T1/2,7-branching,configurations. S h e l l m o d e l . REPT I N D C ( A R G ) - 9 / G , Pbll,Behar. R A D I O A C T I V I T Y 95mpd [ f r o m 5SNi(4°Ca,n2p),E=133-173 M e V ] ; m e a s u r e d ] ? - d e l a y e d Ep,Ip, fl-delayed pT(t); deduced log f t . 9 5 R h , 9 4 R u l e v e l s d e d u c e d 7-branching. 146Dy [ f r o m 9°Zr(SSNi,2p)3; ' S ° E r [ f r o m 94Mo(SSNi,2p),geMo(6ONi,2p)]; m e a s u r e d a(E7),77-coin,77(t),DSA, ] ? - d e l a y e d p 7 ( t ) . ~4~Dy,~S°Er d e d u c e d levels,J,~r. 15OTm,~44Tb,~46Ho,~4SEr; m e a s u r e d ]?-decay. CONF H e l s i n g o r V o l l P253, CERN 8 1 - 0 9 . NUCLEAR REACTIONS 99Zr,9~Mo(a,2n7),E=27 MeV; m e a s u r e d 7(0,H,t). 99Mo,a4Ru l e v e l s d e d u c e d g, configurations. CONF R i g a , P 2 4 3 , L e b e d e v . NUCLEAR REACTIONS ~°Ni(4°Ca,2n2p),(4OCa,2pa),E=140 MeV; m e a s u r e d E7,IT,a(ET). 9~Pd,~4Ru d e d u c e d l e v e l s , J , ~ r . B A P S A 27 7 2 7 , E C 4 , L i s t e r .

A 95Rb

93

NUCLEAR REACTIONS 9~Mo(p,7),E=2.36-2.58 MeV; m e a s u r e d y i e l d v s E. 93Tc d e d u c e d p r o t o n b i n d i n g e n e r g y . T h i c k t a r g e t . REPT J Y F L 1981 A n n , P 4 1 , V i e r i n e n . R A D I O A C T I V I T Y 93mRu [ f r o m 99Mo(3He,Rn),E=24 MeV]; m e a s u r e d ]?-delayed Ep,Ip. REPT JYFL 1980 Ann,P42,Aysto. R A D I O A C T I V I T Y 93mRu [ f r o m 99Mo(3He,2n),E=24 MeV]; m e a s u r e d f l - d e l a y e d Ep,Ip; d e d u c e d Q(EC), absolute fl-branching,log f t . CONF H e l s i n g o r V o l l P 2 4 7 , CERN 8 1 - 0 9 .

A 94Rb

=

ONLY)

=

95

RADIOACTIVITY 94,95,96,97Rb; measured Efl,lfl; d e d u c e d Q~. 94,95,96,97Sr [ f r o m 94 9596,97Rb decay]; measured Efl,lfl; d e d u c e d Qfl. B A P S A 27 4 9 9 , D Y a 1 4 , D a u t e t . R A D I O A C T I V I T Y °SRb; m e a s u r e d f l - d e l a y e d E n , I n , n T - c o i n . Tof,SHe gas s c i n t i l l a t o r . BAPSA 27 498,DYa8,Yeh. R A D I O A C T I V I T Y z4,95,96,9~Rb; m e a s u r e d Efl,Ifl; d e d u c e d Qfl. 94,95,96,97Sr [ - f r o m 94 95 96,97Rb decay]; measured Efl,Ifl; d e d u c e d Qfl. B A P S A 27 4 9 9 , D Y a 1 4 , D a u t e t .

238

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 95Rh

D 81NoZY:

ospd

D 81NoZY:

D 79PeZL

79WaZU

80JuZY

82DaZY 96Sr

D 79PeZL

80JuZY

82DaZY

96y

D 80JuZY

96ZF

R 81DjZR

9eNb

R 79DoZV

96Mo

R 79IvZX

81DjZR

82VaZW:

9STc

R 81MaZQ:

9spd

R 82LiZM:

95

continued

RADIOACTIVITY 95mpd [ f r o m 5 8 N i ( 4 ° C a , n 2 p ) , E = 1 3 3 - 1 7 3 MeV]; m e a s u r e d fl-delayed Ep,Ip, fl-delayed p-/(t); d e d u c e d log f t . 9 5 R h , 9 4 R u l e v e l s d e d u c e d -/-branching. t46Dy [ f r o m 9 ° Z r ( S e N i , 2 p ) ] ; lS°Er [ f r o m 94Mo(SSNi,Zp),SZMo(S°Ni,2p)]; m e a s u r e d a(E-/),-/7-coin,-/7(t),DSA, fl-delayed p-/(t). 146Dy,15°Er d e d u c e d l e v e l s , J , r r . 15°Tm,144Tb,146Ho,148Er; m e a s u r e d fl-decay. CONF H e l s i n g o r V o l l P253, CERN 8 1 - 0 9 . R A D I O A C T I V I T Y 95mpd [ f r o m S S N i ( 4 ° C a , n 2 p ) , E = 1 3 3 - 1 7 3 MeV]; m e a s u r e d fl-delayed Ep,Ip, fl-delayed p-/(t); d e d u c e d log f t . 9 5 R h , 9 4 R u l e v e l s d e d u c e d -/-branching. ~SDy [from 9 ° Z r ( S S N i , 2 p ) ] ; tS°Er [ f r o m 94Mo(SSNi,Ep),SZMo(S°Ni,2p)]; m e a s u r e d cr(ET),-/-/-coin,-/-/(t),DSA, fl-delayed p-/(t). ~4~Dy,iS°Er d e d u c e d l e v e l s , J , r r . ~°Tm,144Tb,~4eHo,~48Er; m e a s u r e d fl-deeay. CONF H e l s i n g o r V o l l P253, CERN 8 1 - 0 9 .

A

96Rb

=

ONLY)

=

96

R A D I O A C T I V I T Y 96,97,S8,99,100Rb [ f r o m a35U(n,F),E=thermal]; measured fl-delayed neutron s p e c t r a , f l - / - c o i n ; d e d u c e d TI/2. 9s,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96 9SRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 96,SeSr,SSY,sem,SgNb,l°aMo,l°aTc Efrom aaSU(n,F),E=thermal]; measured fiT-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. R A D I O A C T I V I T Y 94,SSRb,143,144Cs [ f r o m on-line separation]; measured E-/,1-/; d e d u c e d fl-delayed neutron emission probability. CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products), P311,Warner. R A D I O A C T I V I T Y 92,94,96,g8,1°°Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E-/, I-/,-/-/(0),-/-/-coin,I(ce),fl-delayed neutrons. 9SSr d e d u c e d n e u t r o n emission probability. 94 92,96,98Sr l e v e l s d e d u c e d 6,J,rr,y-branching. 96,SSSr d e d u c e d ICC,B(E2). 9SSr [ f r o m 9SRb decay]; measured fl-/-coin,I(ce),-/-/(0),ET,I-/. 96y d e d u c e d levels,~(M1/E2),~(E1/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. R A D I O A C T I V I T Y 94,ss,ss,97Rb; m e a s u r e d Efl,Ifl; d e d u c e d Qfl. 94,95,96,S7Sp [ f r o m 94,ss,as,97Rb decay]; measured Efl,Ifl; d e d u c e d Qfl. B A P S A 37 4 9 9 , D Y a 1 4 , D a u t e t . R A D I O A C T I V I T Y 96,97,ss,99,16ORb [ f r o m 235U(n,F),E=thermal]; measured fl-delayed neutron s p e e t r a , f l - / - c o i n ; d e d u c e d Tt/z. 9s,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96 9aRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 9°,SSSr,SSY,99m,99Nb,l°ZMo,ZSaTc [from a35U(n,F),E=thermal]; measured fl-/-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. R A D I O A C T I V I T Y 9a,94,ss,ss,lo°Rb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E-/, IT,-/7(0),-/-y-coin,I(ce),fl-delayed neutrons. 98St d e d u c e d n e u t r o n emission probability. 94 9z,96,SSSr l e v e l s d e d u c e d &,J,Tr,-/-branching. 96,SSSr d e d u c e d ICC,B(E2). ° 6 S t [ f r o m 9SRb decay]; measured fl-/-coin,I(ce),-/-/(0),ET,I-/. 96y d e d u c e d levels,6(M1/E2),6(El/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. R A D I O A C T I V I T Y 94,95,96,9~Rb; m e a s u r e d Efl,Ifl; d e d u c e d Qfl. 94,95,gs,97Sr [ f r o m 94,95,96,97Rb decay]; measured Efl,Ifl; d e d u c e d Qfl. B A P S A 27 4 9 9 , D Y a 1 4 , D a u t e t . R A D I O A C T I V I T Y 9a,94,96,ss,lOORb [ f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E-/, I%-/-/(0),-/-/-coin,I(ce),fl-delayed neutrons. 98Sr d e d u c e d n e u t r o n emission probability. 94, 9a,96,98Sr l e v e l s d e d u c e d 6 , J , ~ r , - / - b r a n c h i n g . 96,98Sr d e d u c e d ICC,B(E2). 96St [ f r o m 96Rb decay]; measured fl'/-coin,I(ce),-/-/(0),E-/,I-/. 96y d e d u c e d levels,6(M1/E2),~(El/M3), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. NUCLEAR REACTIONS 4°Ca,51v,5S,S°,SaNi,SSZn,g°,sa,8%SSZr,Sa,94,ss,se,199Mo,i2°,la4Sn,J4°Ce(p,p'), E=201 MeV; m e a s u r e d cr(Ep'). 4°Ca,SiV,SS,s°,aZNi,eSZn,99,sa,94,96Zr,Sa,94,9°,sa,iO6Mo,iZ6,1Z4Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 9 6 Z r ( p , n T ) , E = 3 . 3 MeV; m e a s u r e d E-/,t-/. 96Nb d e d u c e d transitions. Enriched t a r g e t s , G e ( L i ) d e t e c t o r s . CONF R i g a , P 5 7 9 , D o m b r a d i . NUCLEAR REACTIONS 9a,ss,SaMo,na,la4Sn(a,cx),(cx,a'),E=29.3,40,45,50 MeV; m e a s u r e d or(E,0). 9z, 96,9aMo,HS,ia4Sn d e d u c e d d e f o r m a t i o n parameter ft. B l a i r p h a s e m e t h o d . CONF R i g a , P 3 2 1 , Ivanov. NUCLEAR REACTIONS 46Ca,Slv,SS,69,SaNi,SaZn,96,sa,94,96Zr,Sa,94,96,ss,iO°Mo,*a°,la4Sn,H6Ce(p,p'), E = 3 0 1 MeV; m e a s u r e d c~(Ep'). 4 ° C a , S l V , 5 8 , 6 ° , S a N i , S a Z n , 9 ° , s a , 9 4 , S S Z r , S a , 9 4 , 9 6 , s a , l ° ° M o , i a ° , l a 4 S n deduced M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS l°4,t°z,i°°Ru(d,6Li),E n o t g i v e n ; m e a s u r e d or(0). 96,98,1°°Mo levels d e d u c e d relative strengths. DWBA,coupled-channels a n a l y s e s . REPT KVI 1981 A n n , P I T , v a n d e n Berg. NUCLEAR REACTIONS 93Nb(a,n),E=14,18 MeV; m e a s u r e d E % I - / , c r ( E T ) , - / ( 0 ) , I C C , 7 - / - , n - / - c o i n , l i n e a r p o l a r i z a t i o n . 96To d e d u c e d l e v e l s , J , w . DABBB 4E 1 0 6 8 , M a c h . NUCLEAR REACTIONS 6 9 N i ( 4 ° C a , 2 n 2 p ) , ( 4 ° C a , 2 p c 0 , E = 1 4 0 MeV; m e a s u r e d ET,I%cr(ET). 96pd,94Ru deduced l e v e l s , J , T r . B A P S A E7 7 E 7 , E C 4 , L i s t e r .

239

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 97Rb

D 79PeZL:

82DaZY: 97Sr

D 82DaZY:

97Zr

R 82AlZV:

97Ru

R 79HeZQ:

97Rh

R 82MaZQ:

D 79PeZL:

80JuZY:

98Sr

D 79PeZL:

80JuZY:

99y

D 79PeZL:

81BaZT: g8Zr

D 80KaZP: 81BaZT:

99Mo

B 79IvZX:

81DjZR:

81QaZY

82VaZW

98Ru

R

81WhZY

97

RADIOACTIVITY 96,97,98,99,169Rb [ - f r o m 2 3 5 U ( n , F ) , E = t h e r m a l S ; m e a s u r e d f l - d e l a y e d n e u t r o n s p e c t r a , f i T - c o i n ; d e d u c e d Tt/2. 96,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96, 98Rb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n s e p a r a t i o n e n e r g y . 96,SSr,SY,99m,99Nb,lO2Mo,lO2Tc [-from 23SU(n,F),E=thermalS; measured fiT-coin; deduced Qfi,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s e . F i s s i o n Products),P288,Peuser. RADIOACTIVITY 94,95,96,97Rb; m e a s u r e d Efi,Ifl; d e d u c e d Qfl. 94,96,96,97Sr [ - f r o m 94,95,96,97Rb decay']; measured Efl,Ifi; d e d u c e d Qfl. BAPSA 27 4 9 9 , D Y a 1 4 , D a u t e t . RADIOACTIVITY 94,95,96,9~Rb; m e a s u r e d Efl,Ifi; d e d u c e d Qfl. 94,95,96,97Sr [ - f r o m 9 4 , 9 5 , 9 6 , 9 7 R b decay]; measured Efl,Ifi; d e d u c e d Qfl. BAPSA 27 4 9 9 , D Y a 1 4 , D a u t e t . NUCLEAR REACTIONS 9 % r ( n , 7 ) , E = 0 . 3 0 1 - 2 9 . 8 3 keV; m e a s u r e d a ( c a p t u r e ) v s E. 97Zr d e d u c e d r e s o n a n c e s , L , J , F n , F T . REPT N E A N D C ( E ) - 2 3 2 U , V o l I I I , P 1 2 , A l l e n . NUCLEAR REACTIONS 9 5 M o ( a , 2 n ) , E = c y c l o t r o n ; m e a s u r e d a T - c o i n . 9~Ru l e v e l d e d u c e d T1/2, configuration. REPT Z F K - 3 8 5 , P 3 0 , H e i s e r . NUCLEAR REACTIONS S S R u ( a , 2 n p ) , E n o t g i v e n ; m e a s u r e d E T , I T , T T - c o i n , 7 ( 0 ) . 97Rh d e d u c e d levels,v-branching. REPT I N D C ( A R G ) - 9 / G , P b l 6 , M a c c h i a v e l l i .

A

99Rb

=

ONLY)

=

98

RADIOACTIVITY 96,97,98,99,100Rb [ f r o m 2 3 S U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d f i - d e l a y e d n e u t r o n s p e c t r a , f i T - c o i n ; d e d u c e d T1/2. 9e,99Rb d e d u c e d f i - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96 98Rb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n s e p a r a t i o n e n e r g y . 9s,aSr,9SY,om,99Nb,'°~Mo,t°2Tc [from 2SSU(n,F),E=thermal]; measured fiT-coin; deduced Qfi,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),PR88,Peuser. RADIOACTIVITY 92,94,9678,i°°Rb [ - f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E7, I7,77(0),77-coin,I(ce),fl-delayed n e u t r o n s . 9SSr d e d u c e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 94 9z,96,SSr levels deduced 6,J,vr,T-branching. 96,98Sr d e d u c e d ICC,B(E2). 96Sr [ - f r o m 96Rb decayJ; measured flT-coin,I(ce),TT(0),E7,I7. 96y d e d u c e d levels,6(M1/E2),6(E1/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. RADIOACTIVITY 9s,v,e,99,1°°Rb [from 235U(n,F),E=thermalS; measured fl-delayed neutron s p e c t r a , f i T - c o i n ; d e d u c e d T1/a. 98,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 98 99Rb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n s e p a r a t i o n e n e r g y . 99,98Sr,aY,99m,99Nb,192Mo,19aTc [from 235U(n,F),E=thermal]; measured fi7-coin; deduced Qfi,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. RADIOACTIVITY 92,94,99,99,109Rb [ - f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s 3 ; m e a s u r e d ET, I7,77(0),77-coin,I(ce),fl-delayed n e u t r o n s . 9SSr d e d u c e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 94 92,96,99Sr l e v e l s d e d u c e d ¢ ~ , J , T r , T - b r a n c h i n g . 9s,SSr d e d u c e d ICC,B(E2). 96Sr [ - f r o m 96Rb decay3; measured flT-coin,I(ce),TT(O),ET,I7. 96y d e d u c e d levels,c~(Ml/E2),O(E1/M2), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. RADIOACTIVITY 9s,97,99,99,tORb [from 235U(n,F),E=thermal]; measured fi-delayed neutron s p e c t r a , f i T - c o i n ; d e d u c e d TI/2. 96,99Rb d e d u c e d f i - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96 98Rb d e d u c e d Q f i , m a s s e x c e s s , t w o - n e u t r o n s e p a r a t i o n e n e r g y . 99,98Sr,aY,99m,99Nb,19aMo,'O2Tc [-from 235U(n,F),E=thermalS; measured f/T-coin; deduced Qfi,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. RADIOACTIVITY 99y; m e a s u r e d fiT(t). 9azr d e d u c e d levels,T1/2,B(E2). REPT J U L - S p e z - 9 9 , P 6 2 , Battistuzzi. RADIOACTIVITY 99Zr [ - f r o m f i s s i o n p r o d u c t s e p a r a t o r 3 ; m e a s u r e d 77(0). 99Zr levels d e d u c e d J,Tr. Ge(Li) d e t e c t o r s . REPT J U L - S p e z - 7 2 , P 6 2 , K a w a d e . RADIOACTIVITY 99y; m e a s u r e d fiT(t). 98Zr d e d u c e d levels,Tl/2,B(E2). REPT J U L - S p e z - 9 9 , P 6 2 , Battistuzzi. NUCLEAR REACTIONS 92 , 96 ,98 Mo, 116 , 124 S n ( a , a ) , ( a , a ' ) , E = 2 9 . 3 , 4 0 , 4 5 , 5 0 MeV; m e a s u r e d a(E,e). 92 96,99Mo,H6,124Sn d e d u c e d d e f o r m a t i o n parameter fi. B l a i r p h a s e m e t h o d . CONF Riga,P321, Ivanov. ( P , P ,) NUCLEAR REACTIONS 49Ca . 51 v. 59 . 69 SZNi . . 6SZn . .99 92 . 94. 96Zr . 92 . 94. 86. 96 .iOOMo . l. e 6 .1 2 4 S. n 149Ce . ., E=201 MeV; m e a s u r e d a ( E p ' ) . 4°Ca . s i.v . 59. 60 sa N .1,SeZn . 90. 92 . . 94 96Zr . 92. 94 . .96. 98 199Mo,IaO,124Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 44 Ca, 49 Ti, 90 Cr, 67 , 68 Z n , 82 Z r , 97 , 98 M o ( n , d ) , ( n , n ' p ) , ( n , n p ) , E = 1 4 . 7 MeV; m e a s u r e d e;; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,SiCr,SS,SZn,93Zr,a,99Mo deduced dominant decay m o d e . REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 0 , Q a i m . NUCLEAR REACTIONS l°4,m2,t°Ru(d,SLi),E n o t g i v e n ; m e a s u r e d a(0). 9s,a,iOaMo l e v e l s d e d u c e d r e l a t i v e s t r e n g t h s . D W B A , c o u p l e d - c h a n n e l s a n a l y s e s . REPT KVI 1981 A n n , P 1 7 , v a n d e n Berg. NUCLEAR REACTIONS 9s,l°°Mo(SHe,xn),E=13 MeV; m e a s u r e d 7(0),TT-coin. 9e?°lRu d e d u c e d levels, v-branching. BAPSA 26 l 1 4 6 , D D 3 , W h i s n a n t .

240

SECONDARY

SOURCES

(Reports,Abs[rac[s,etc.

A 99Rb

D 79PeZL :

82DaZR: 99Sr

D 82DaZR: 82PeZX:

99y

D 82MoZX:

82PeZX: 99Nb

D '79PeZL:

81SiZW: 82BaZV: 99Mo

D 81SiZW: R 81QaZY:

99Tc

D 79GeZQ:

99RU

J

99Rh

R 81KaZU:

82EIZX:

81PaZU:

D 79PeZL:

80JuZY:

~OOZr

D

lOONb

R 81F1ZW:

lOOMs

R 81DjZR:

80WoZO:

8:3VaZW: IOORh

R 82BeZR:

99

R A D I O A C T I V I T Y 96,97,98,99,199Rb [ f r o m a35U(n,F),E=thermal]; measured fl-delayed neutron spectra,fl?-coin; d e d u c e d Tl/a. 9s,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 96 9eRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 96,98Sr,SSy,99m,99Nb,i°2Mo,l°aTc [-from aUSU(n,F),E=thermal]; measured fl-/-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. R A D I O A C T I V I T Y 99Rb(fl-),99Sr(fl-); m e a s u r e d Efl,Ifl; d e d u c e d f l - e n d p o i n t e n e r g i e s , m a s s e x c e s s . B A P S A 27 7 2 7 , E C 5 , D a u t e t . R A D I O A C T I V I T Y 99Rb(fl-),99Sr(fl-); m e a s u r e d Efl,Ifl; d e d u c e d f l - e n d p o i n t e n e r g i e s , m a s s e x c e s s . B A P S A 27 7 2 7 , E C 5 , D a u t e t . R A D I O A C T I V I T Y 99St [ - f r o m m a s s s e p a r a t o r ] ; m e a s u r e d ?3,-coin,T1/a. 99y d e d u c e d levels. BAPSA 27 4 9 9 , D Y a t 3 , P e t r y . R A D I O A C T I V I T Y 99y [ f r o m fission product on-line mass separation]; measured ?-y-coin; deduced isomer,T1/2,1evels,J,Tr,?-branching,possible rotational b a n d . REPT J U L - S p e z - 1 4 6 , P46,Monnand. R A D I O A C T I V I T Y 99Sr [ - f r o m m a s s s e p a r a t o r ] ; m e a s u r e d 3~?-coin,Tl/a. 99y d e d u c e d levels. BAPSA 27 4 9 9 , D Y a 1 3 , P e t r y . R A D I O A C T I V I T Y 96,97,98,99,1°°Rb [ - f r o m 2 3 S U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d fl-delayed neutron s p e c t r a , f l - y - c o i n ; d e d u c e d Tl/2. 9a,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 98 98Rb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 96,SSSF,98y,99m,99Nb,I°2Mo,l°ZTc [-from aaSU(n,F),E=thermal]; measured fiT-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),P288,Peuser. R A D I O A C T I V I T Y 99Nb; m e a s u r e d fl-y-coin,fl?(t). 99Mo level d e d u c e d T l / 2 , t r a n s i t i o n p r o b a b i l i t y , configuration. REPT J U L - S p e z - 9 9 , P 6 4 , S i s t e m i c h . R A D I O A C T I V I T Y 99Nb [ - f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d fl?(t). 99Nb level d e d u c e d Tt/z, B(E2). REPT J U L - S p e z - 1 4 6 , P 4 7 , B a t t i s t u z z i . R A D I O A C T I V I T Y 99Nb; m e a s u r e d fl?-coin,fl?(t). 99Mo level d e d u c e d T 1 / a , t r a n s i t i o n p r o b a b i l i t y , configuration. REPT J U L - S p e z - 9 9 , P 6 4 , S i s t e m i c h . NUCLEAR REACTIONS 4 4 C a , 4 9 T i , 5 ° C r , S ? , 6 8 Z n , S e Z r , 9 7 , 9 8 M o ( n , d ) , ( n , n ' p ) , ( n , n p ) , E = 1 4 . 7 MeV; measured G; d e d u c e d s y s t e m a t i c s . 45Ca,5°Ti,51Cr,aa,69Zn,93Zr,98,99Mo d e d u c e d d o m i n a n t decay m o d e . REPT N E A N D C ( E ) - 2 2 2 U , V o l V , P 3 0 , Q a i m . R A D I O A C T I V I T Y 99mTc; m e a s u r e d E~,I(ce). 99Tc t r a n s i t i o n s deduced subshell intensity r a t i o s . CONF R i g a , P 5 6 5 , G e r a s i m o v . NUCLEAR MOMENTS tHCd,99Ru; m e a s u r e d h y p e r f i n e m a g n e t i c f i e l d v s T. T i m e d i f f e r e n t i a l perturbed angular correlation method,chalcogenide S p i n e l s . DABBB 42 4 1 O 3 , E l f a z a n i . NUCLEAR REACTIONS 96,SSMo(SLi,3n),E=28 MeV; m e a s u r e d a ( E ? ) , ? ( 0 ) j / ~ - c o i n . 99,10tRh d e d u c e d transitions. B A P S A 26 7 9 E , H X 1 8 , K a j r y s . NUCLEAR REACTIONS 9 a , S a M o ( a , n ) , E = l O - 1 8 MeV; m e a s u r e d a ( E ? ) , ? ( 0 ) , 3 ~ ? - , n ~ / - c o i n . 99,~°lRh deduced transitions. B A P S A 26 7 9 1 , H X 1 5 , P a r a d i s .

A lOORb

=

ONLY)

=

100

R A D I O A C T I V I T Y 9s,g?,sa,go,l°°Rb [ - f r o m 2 3 5 U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d fl-delayed neutron spectra,fl?-coin; d e d u c e d Tl/a. 98,99Rb d e d u c e d f l - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 9s, 9SRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y , ss,SaSr,SaY,99m,OSNb,l°2Mo,l°2Tc [-from 235U(n,F),E=thermal]; measured fl?-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products),PE88,Peuser. R A D I O A C T I V I T Y 92,94,96,ss,l°°Rb [ - f r o m o n - l i n e s e p a r a t i o n , s p a l l a t i o n p r o d u c t s ] ; m e a s u r e d E% I?,-y~(0),?7-coin,I(ce),fl-delayed neutrons. 9aSr d e d u c e d n e u t r o n emission probability. 94 9a,gs,SeSr l e v e l s d e d u c e d 6,J,Tr,?-branching. 96,9SSr d e d u c e d ICC,B(E2). 9SSr [ - f r o m SaRb decay]; measured flT-coin,I(ce),~/?(O),E?,I?. 96y d e d u c e d levels,6(Ml/Ea),O(El/Ma), configuration. THESIS G J u n g , J u s t u s Liebig-Universitat. RADIOACTIVITY l°°Zr [from fission product separator]; measured ??(0,H). l°°Zr level deduced g. REPT JUL-Spez-72,P63,Wolf. NUCLEAR REACTIONS ~°Zn,t°4Ru,i1°Pd,lS4Sm,t5s,16eGd,~sSW,19s,laSpt,aoa,aO4Hg,a44pu(polarized t,a), 19SPt,a44Pu,76Ge(polarized t , p ) , E = 1 7 MeV; a2,e°Se,1°°Mo,12a,lZ4Sn(polarized t,3He),E=22-25 MeV; m e a s u r e d c r ( 0 ) , a n a l y z i n g p o w e r v s 0,~(Ec0,G(Ep),cr(3He). 69Cu,lO3Tc,lO9Rh,15Spm,157,t59Eu, 185Ta,195,197Ir,291,2°3Au,243Np,2°°Pt,a46pu,TaGe,e9,SaAs,l°9Nb,t2z,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . NUCLEAR REACTIONS 4OCa,Slv,Sa,S°,a2Ni,SaZn,9°,sa,94,SSZr,92,94,sa,se,lOOMo l a o , l ~ 4 S n , 1 4 9 C e ( p , p , ) , E = 2 0 1 MeV; m e a s u r e d a ( E p ' ) . 4°Ca,Slv,SS,a°,S2Ni,SSZn,99,sa,94,SaZr,SZ,s4,ss,98,190Mo,129,124Sn deduced M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS l°4,i°2,m°Ru(d,SLi),E n o t g i v e n ; m e a s u r e d a(0). 96,98,1°°M0 l e v e l s d e d u c e d relative strengths. DWBA,coupled-channels a n a l y s e s . REPT KVI 1981 A n n , P 1 7 , v a n d e n Berg. NUCLEAR REACTIONS 99Ru(a,2np),SSMo(SLi,4n),E n o t g i v e n ; m e a s u r e d E ( X - r a y ) , I ( X - r a y ) . l ° ° R h deduced levels,J,Tr,T1/a,3'-branching. REPT I N D C ( A R G ) - 9 / G , P b 2 0 , B e h a r .

241

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

199Rh

R

199pd

D 82AnZZ:

82MaZP:

R 81WhZY:

iOIRh

R 81KaZU: 81PaZU:

D 81HiZX:

81HiZY: 82ShZY: 192Zr

D 81HiZX:

81HiZY: 82ShZY: lOZMo

D 79DeYW:

79PeZL:

102To

D 79DeYW:

79PeZL:

lOZRu

R

192pd

D 81CoZR:

81HaZH:

R 80LuZT: leZAg

D 81CoZR:

R 79AvZY:

lozCd

D 81BeZB: 81BeZD:

continued

=

101

NUCLEAR REACTIONS 9e,l°gMo(3He,xn),E=13 MeV; m e a s u r e d -y(0),-yT-coin. 9e,191Ru d e d u c e d levels, -y-branching. B A P S A 26 l 1 4 6 , D D 3 , W h i s n a n t . NUCLEAR REACTIONS 96,98Mo(6Li,3n),E=28 MeV; m e a s u r e d a(E-y),-y(0),-y-y-coin. 99,191Rh d e d u c e d transitions. B A P S A 26 7 9 2 , H X 1 8 , K a j r y s . NUCLEAR REACTIONS 9 e , g S M o ( a , n ) , E = 1 0 - 1 8 MeV; m e a s u r e d a ( E - y ) , - y ( B ) , - y T - , n 3 ' - c o i n . 99,1°1Rh deduced transitions. B A P S A 26 7 9 1 , H X 1 5 , P a r a d i s .

A iO2y

100

NUCLEAR R E A C T I O N S 99Ru(a,2np)?°°Ru(a,3np),E not g i v e n ; measured E ( X - r a y ) , I ( X - r a y ) . ~°°Rh levels deduced I%ICC,7-multipolarity,isomer J,vr. REPT I N D C ( A R G ) - 9 / G , P b l T , M a c c h i a v e l l i . R A D I O A C T I V I T Y ~9°mpd [ f r o m 9~Zr(lZC,3n)]; 7~mBr [ f r o m ~3Cu(iSO,n2p)]; 74mBr [ f r o m SONi(~SO, np)]; measured T l / z . B A P S A 27 2 7 , D F 1 4 , A n d r e j t s c h e f f .

A 1OIRu

=

ONLY)

=

102

R A D I O A C T I V I T Y 10Zy [ f r o m 235U(n,F)]; m e a s u r e d E T , I - y , 7 - y - , ( X - r a y ) - y - c o i n , T l / 2 . l°aZr d e d u c e d levels,-y-branehing,yrast band. Gas-filled recoil separator. CONF H e l s i n g o r Vo12 P 4 4 3 , CERN 8 1 - 0 9 . R A D I O A C T I V I T Y 10Zy; m e a s u r e d E T , I - / , - / 7 - , - y ( X - r a y ) - c o i n , T l / 2 . l°2Zr d e d u c e d levels,J,Tr,B(E4)/ B(E2),deformation. B A P S A 26 I146,DD4,Hi11. R A D I O A C T I V I T Y lO2y [ f r o m fission product separation]; measured ET,IT,Tl/a,7-/-, -y(X-ray)-coin. l ° a Z r d e d u c e d l e v e l s , J , T r . REPT J U L - S p e z - 1 4 6 , P 4 8 , S h i z u m a . R A D I O A C T I V I T Y lOZy [ f r o m Z35U(n,F)]; m e a s u r e d E % I - y , - y T - , ( X - r a y ) 7 - c o i n , T l / 2 . l°ZZr d e d u c e d levels,7-branching,yrast band. Gas-filled recoil separator. CONF H e l s i n g o r Vo12 P 4 4 3 , CERN 8 1 - 0 9 . R A D I O A C T I V I T Y 10Zy; m e a s u r e d E T , l T , 7 7 - , 7 ( X - r a y ) - e o i n , T l / z . l°2Zr d e d u c e d levels,J,Tr,B(E4)/ B(E2),deformation. B A P S A 26 l 1 4 6 , D D 4 , H i I 1 . R A D I O A C T I V I T Y 10ay [ f r o m fission product separat~onq; measured ET,IT,T,/a,-y-y-, 7(X-ray)-eoin. l ° a Z r d e d u c e d l e v e l s , J , r r . REPT J U L - S p e z - 1 4 6 , P 4 8 , S h i z u m a . R A D I O A C T I V I T Y l°2Mo [ f r o m a 3 S U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d E % I % E ( X - r a y ) , I ( X - r a y ) , 7 7 - c o i n , Eft; deduced Ifl,log ft. l°ZTc deduced levels,-ybra nchi ng,J,Tr. CONF Grenoble(Nucl.Spectrosc.Fission Products),P297,De Gelder. R A D I O A C T I V I T Y 9s,97,ge,gs,l°ORb [ f r o m a3SU(n,F),E=thermal]; measured B-delayed neutron s p e c t r a , B - y - c o i n ; d e d u c e d Tl/z. 99,99Rb d e d u c e d B - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 99 9SRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 9s,gSSr,98y,99m,99Nb,19aMo,lOaTc [from a3SU(n,F),E=thermal]; measured B-y-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e e t r o s c . F i s s i o n Products),P288,Peuser. R A D I O A C T I V I T Y l°aMo [ f r o m ~ 3 S U ( n , F ) , E = t h e r m a l ] ; m e a s u r e d E T , I % E ( X - r a y ) , I ( X - r a y ) , - / - y - c o i n , Eft; deduced Ifl,log ft. 19ZTe deduced 1 e v e 1 s , - y - b r a n c h i n g, J , ~r. C O N F Grenoble(Nucl.Spectrosc.Fission Products),P297,De Gelder. R A D I O A C T I V I T Y 99,97,gs,99,19°Rb I - f r o m a 3 5 U ( n , F ) , E = t h e r m a 1 3 ; m e a s u r e d B-delayed neutron s p e c t r a , f i T - c o i n ; d e d u c e d T~/a. 98,99Rb d e d u c e d B - d e l a y e d n e u t r o n e m i s s i o n p r o b a b i l i t y . 9s 9SRb d e d u c e d Q f l , m a s s e x c e s s , t w o - n e u t r o n separation e n e r g y . 9e,98Sr,geY,99m,99Nb,19ZMo,19aTc [from Z35U(n,F),E=thermal]; measured B'y-coin; deduced Qfl,mass excess,two-neutron separation e n e r g y . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Produets),P288,Peuser. NUCLEAR REACTIONS l ° O M o ( V L i , x n p ) , ( T L i , x n d ) , ( T L i , x n t ) , E = 4 8 MeV; m e a s u r e d (particle)-y-, V - y - c o i n . 194,1°eRu d e d u c e d l e v e l s . B A P S A 26 l 1 4 6 , D D 5 , H a e n n i . R A D I O A C T I V I T Y l°amAg,l°emIn [ f r o m Mo(14N,xnyp),E=90 MeV]; m e a s u r e d -y-y(0),I(ce). 19epd,l°sCd deduced levels,J,rr,E0 transition strength,B(E0)/B(E2). Interacting boson approximation calculations. CONF H e l s i n g o r Vo12 P 4 6 0 , CERN 8 1 - 0 9 . NUCLEAR REACTIONS l°2,~94pd(isO,lsO'),E=44 MeV; m e a s u r e d d o u b l e C o u l o m b e x e i t a t i o n , E - y , I % l°z,194pd t r a n s i t i o n s d e d u c e d B(E2). REPT JYFL 1980 A n n , P 4 4 , L u o n t a m a . R A D I O A C T I V I T Y 19emAg,iOSmIn [ f r o m Mo(14N,xnyp),E=90 MeV]; m e a s u r e d -y-y(0),I(ce). leZpd,i°sCd deduced levels,J,Tr,E0 transition strength,B(E0)/B(E2). Interacting boson approximation calculations. CONF H e l s i n g o r V o l 2 P 4 6 0 , CERN 8 1 - 0 9 . NUCLEAR REACTIONS l°z,l°4Pd(p,n),E < 7.E MeV; m e a s u r e d i s o m e r i c a r a t i o v s (E). l°e,l°4Ag l e v e l s d e d u c e d J. CONF R i g a , P 2 8 9 , A v c h u k h o v . RADIOACTIVITY l°z,l°3In [from 92Mo(14N,X),E=86 M e V ] ; m e a s u r e d E-y,IT,Tl/z. l ° 3 I n l e v e l d e d u c e d J,Tr. l°aCd d e d u c e d t r a n s i t i o n s . REPT L Y C E N - 8 1 0 1 , P 3 3 , B e r a u d . R A D I O A C T I V I T Y l°3,1°2In [ f r o m 9°,92Mo(14N,X),E=80,86 MeV]; m e a s u r e d T1/z,-y-y-eoin,-y(O),E-y,I-y. 19aCd d e d u c e d levels,J,Tr,band structure,-y branching. CONF H e l s i n g o r V o l 2 P692, CERN 81-09.

242

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A ~oaCd

R 81TrZZ:

82JaZY: ~O~in

D 81BeZB: 81BeZD:

81WoZV:

D 8ESiZX:

~OSMo

D 8ESiZX:

lO3Tc

R 81FIZW:

lOaRu

R 80BeYX:

80GuZV:

81BeZQ lOaRh

D 79VaZE

~63in

D 81BeZB 81BeZD

81CeZX 81WoZV 8EWoZW R 80StZK

D 81TiZZ

lO4Tc

D 8tTiZZ

~O4Ru

R 81HaZH

lo4pd

D 80LuZT: R 80LuZT: 82NaZU:

lO4Ag

D BOLuZT:

continued

=

103

R A D I O A C T I V I T Y l°3Nb [ - f r o m f i s s i o n ] ; m e a s u r e d ET,IT,TT-,T(X-ray)-coin. l°3Mo d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 5 , S i s t e m i c h . R A D I O A C T I V I T Y t°3Nb [ f r o m fission]; measured ET,IT,T?-,'y(X-ray)-coin. l°SMo d e d u c e d l e v e l s . B A P S A 27 4 9 9 , D Y a 1 5 , S i s t e m i e h . NUCLEAR REACTIONS ?°Zn,l°4Ru,n°Pd,lS¢Sm,iSS,16°Gd,lS6W,196,19°Pt,2°a,aO4Hg,a4¢Pu(polarized t,a), 198Pt,244Pu,?6Ge(polarized t , p ) , E = 1 7 MeV; 8 2 , e ° S e , l ° ° M o , i a a , l a 4 S n ( p o l a r i z e d t,3He),E=23-25 MeV; m e a s u r e d a(0),analyzing p o w e r v s 0 , a ( E a ) , a ( E p ) , ( r ( a H e ) . 69Cu,lOSTc,l°gRh,153pm,iS?,I59Eu, 185Ta,195,t97Ir,a°l,a°3Au,a43Np,2°°Pt,246pu,78Ge,S°,eaAs,l°6Nb,taa,ia4In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 6 1 - 0 9 . NUCLEAR REACTIONS l ° 2 R u ( d , p ) , E = 4 5 MeV; ~°4Ru(p,d),E=E9 MeV; m e a s u r e d ff(Ep),cr(Ed),cr(0). l°3Ru levels deduced L. DWBA a n a l y s i s . High resolution magnetic spectrometer. REPT JUL-Spez-7E,P39,Berg. NUCLEAR REACTIONS l e a R u ( n , 7 ) , E = t h e r m a l ; measured ET,Iv,3'V(O),TT-coin. l°3Ru deduced neutron binding energy,rotational band alignment characteristics. E n r i c h e d t a r g e t . REPT JUL-Spez-TE,P70,G uven. NUCLEAR REACTIONS maRu(d,p),E=45 MeV; t°4Ru(p,d),E=29 MeV; l°3Ru levels d e d u c e d ECaS. DWBA analysis. High resolution magnetic spectrometer. REPT J U L - S p e z - 9 9 , P 3 8 , B e r g . R A D I O A C T I V I T Y l°3mRh [ f r o m ~93pd d e c a y , i o n e x c h a n g e ] ; m e a s u r e d ET,IT,TI/a; d e d u c e d ICC,K X-ray emission r a t e s . REPT NEANDC(E)-EOEU,Vol I I I , P E S , V a n i n b r o u k x . RADIOACTIVITY l°a,l°3In [from a a M o ( t 4 N , X ) , E = 8 6 MeV]; m e a s u r e d ET,IT,T1/e. 1°Sin l e v e l d e d u c e d J,rr. l°aCd d e d u c e d t r a n s i t i o n s . REPT L Y C E N - 8 1 0 1 , P 3 3 , B e r a u d . R A D I O A C T I V I T Y 1°3,1°2In [ f r o m 9°,92Mo(14N,X),E=80,86 MeV]; m e a s u r e d T 1 / a , T T - c o i n , T ( 0 ) , E ? , I T. toeCd d e d u c e d levels,J,Tr,band structure,T-branching. CONF H e l s i n g o r V o l e P69E, CERN 61-09. R A D I O A C T I V I T Y 1°3,1°51n [ f r o m on-line mass separator]; measured flT-coin,fl-endpoint e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . CONF H e l s i n g o r V o l l P134, CERN 6 1 - 0 9 . R A D I O A C T I V I T Y l°a,~°3,~°SIn [ f r o m Mo,OaMo(14N,X)]; m e a s u r e d flT-eoin,Efl,Ifl,fl e n d - p o i n t e n e r g i e s . ~93,1°5In d e d u c e d m a s s e s . B A P S A 36 l 1 4 6 , D D 6 , W o u t e r s . R A D I O A C T I V I T Y mam4,1°SIn [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT JYFL 1961 A n n , P 5 5 , W o u t e r s . NUCLEAR REACTIONS SaCu,4°Ca(¢°Ca,4°Ca),(4OCa,X),E=400 MeV; m e a s u r e d o r ( f r a g m e n t E ) , f r a g m e n t mass,Z. 8°Zr,t°aIn deduced resonance structure. REPT IPN 1980 A n n u a l , P N 5 0 , S t e p h a n .

A 1O4Mo

102

NUCLEAR REACTIONS 9aMo(laC,Sn),E=50 MeV; m e a s u r e d E%ITj/7(t),7(0). lazed d e d u c e d l e v e l s , J , rr,isomer T~/~,?-multipolarity,?-branching,eonfiguration. CONF H e l s i n g o r Vol~ P 4 5 9 , CERN 81-09. NUCLEAR REACTIONS 94Mo(a3Na,Enp),E=85 MeV; ~aMo(laC,En),E=48 MeV; m e a s u r e d T ? - c o i n . n4Te, ~°aCd d e d u c e d h i g h - s p i n s t a t e s . P H C A A 38 4 1 , F A a , J a n z e n . R A D I O A C T I V I T Y ~°a,iOaln [ f r o m 9aMo(t4N,X),E=86 M e V ] ; m e a s u r e d E%IT,Tt/a. t°aln level d e d u c e d J,?r. t°aCd d e d u c e d t r a n s i t i o n s . REPT L Y C E N - 8 1 0 1 , P 3 3 , B e r a u d . R A D I O A C T I V I T Y ~63,~°~In [ f r o m 99,gaMo(14N,X),E=60,86 MeV]; r r f e a s u r e d T l / a , T T - c o i n , T ( 0 ) , E T , I T. ~°aCd d e d u c e d levels,JJr,band structure,T-branching. CONF H e l s i n g o r V o l e P692, CERN 81-09. R A D I O A C T I V I T Y t°a,~°3,~°Sln [ f r o m Mo,9~Mo(~4N,X)]; m e a s u r e d flT-eoin,Efl,Ifl,fl e n d - p o i n t e n e r g i e s , i°3,~°SIn d e d u c e d m a s s e s . B A P S A 26 1 1 4 6 , D D 6 , W o u t e r s .

A

IOSNb

=

ONLY)

=

104

R A D I O A C T I V I T Y l°4Mo [ f r o m i s o t o p e s e p a r a t o r ] ; m e a s u r e d ET,IT,7~/(t); d e d u c e d tog ft. IO4Te deduced levels,7-branching,JJr,configuration. REPT U n i v M a i n z , 1 9 8 0 , A n n u a l , P 3 4 , T i t t e l . R A D I O A C T I V I T Y l°4Mo [ f r o m i s o t o p e s e p a r a t o r ] ; m e a s u r e d ET,I%TT(t); d e d u c e d log f t . l°4Tc deduced levels,7-branching,J,rr,configuration. REPT U n i v M a i n z , 1 9 8 0 , A n n u a l , P 3 4 , T i t t e l . NUCLEAR REACTIONS 1 ° ° M o ( T L i , x n p ) , ( ? L i , x n d ) , ( ? L i , x n t ) , E = 4 8 MeV; m e a s u r e d (particle)7-, 77-coin. l°4,1°aRu deduced l e v e l s . B A P S A 26 l 1 4 6 , D D 5 , H a e n n i . R A D I O A C T I V I T Y 104mAg; m e a s u r e d I ( e e ) , 7 - s p e c t r a . ~°4pd l e v e l d e d u c e d d e c a y c h a r a c t e r i s t i c s . REPT J Y F L 1980 A n n , P 4 4 , L u o n t a m a . NUCLEAR REACTIONS l°2,i°4pd(loO,lsO'),E=44 MeV; m e a s u r e d d o u b l e C o u l o m b e x c i t a t i o n , E - / , I - / . l°2,1°4pd t r a n s i t i o n s deduced B(ES). REPT JYFL 1980 A n n , P 4 4 , L u o n t a m a . NUCLEAR REACTIONS l°4,1°6,1°8,II°Pd(polarized p , p ) , ( p o l a r i z e d p,p'),E=22 MeV; m e a s u r e d or(0), A(0). lo4 lo6 l o s , u o p d d e d u c e d flz,fla. DWBA a n a l y s i s . REPT U T T A C - 4 5 , P 3 8 , N a g a n o . R A D I O A C T I V I T Y l°4mAg; m e a s u r e d I ( c e ) , 7 - s p e e t r a . l°4pd l e v e l d e d u c e d d e c a y c h a r a c t e r i s t i c s . REPT J Y F L 1980 A n n , P 4 4 , L u o n t a m a .

243

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A lO4Ag

R 79AvZY:

lO4in

D 82WoZW:

=

R 82CaZT:

~OSRh

R 82CaZT:

~O~Ag

R 79KeZW:

79LeZK:

*OSln

D 81CeZX: 81WoZV: 82WoZW:

D 82BoZZ:

*oapd

D 82BoZZ:

R 82NaZU: 'OSAg loSCd

D 79BaXZ: 79BaYA: D 81RoZ0:

81RoZP:

R 81AnZS: lO6in

D 81RoZ0:

81RoZP:

R 82AyZY: 1OSSn

D 80AuZU:

R 82SaZX:

i°7I n

D 82AnZY:

R

*OTSn

81AuZW:

D 80AuZV:

=

106

R A D I O A C T I V I T Y l°6Rh [ f r o m l°SRu decay3; m e a s u r e d (ce)fl-coin,I(ce). l°6Pd t r a n s i t i o n d e d u c e d B ( E 0 ) / B ( E 2 ) l i m i t s . REPT KVI 1981 A n n , P 5 4 , B o u w m a n . R A D I O A C T I V I T Y l°SRh [ f r o m l°SRu decay3; m e a s u r e d (ce)fl-coin,I(ce). l°sPd t r a n s i t i o n d e d u c e d B ( E 0 ) / B ( E 2 ) l i m i t s . REPT KVI 1981 A n n , P 5 4 , B o u w m a n . NUCLEAR REACTIONS l°4,166,1°8,n°Pd(polarized p , p ) , ( p o ] a r i z e d p,p'),E=22 MeV; m e a s u r e d a(O), A(0). 1°4,1°6,*°8,11°Pd d e d u c e d f12,f13. DWBA a n a l y s i s . REPT U T T A C - 4 5 , P 3 8 , N a g a n o . R A D I O A C T I V I T Y l°SAg; m e a s u r e d A u g e r s p e c t r a . CONF R i g a , P 2 5 6 , B a b e n k o v . R A D I O A C T I V I T Y 1°SAg; m e a s u r e d A u g e r s p e c t r a . CONF R i g a , P 2 5 5 , B a b e n k o v . R A D I O A C T I V I T Y l°8,1°6In; m e a s u r e d ET,IT,I(ce),77(t),7(ce)(t). i°8,*°sCd d e d u c e d levels, 7-branching. Vibrator plus particle,interacting b o s o n m o d e l s . REPT IPN 1981 A n n u a l , P N 3 5 , Roussiere. R A D I O A C T I V I T Y 1°6,'°6In [ f r o m Sn(p,xn2p),E=20O MeV; Sn(SHe,xnyp),E=270 MeVS; m e a s u r e d ET, IT,77(t),7(ce)(t),I(ee); deduced log f t , i s o m e r J. 1°8,1°6Cd d e d u c e d levels,0 + state decay characteristics. Interacting b o s o n m o d e l . REPT I P N O - T - 8 1 - 0 5 , R o u s s i e r e . NUCLEAR REACTIONS SSNb(lsO,2np),E n o t g i v e n , m~Cd l e v e l s d e d u c e d i s o m e r T1/a. Generalized centroid shift method. B A P S A 26 l 1 4 6 , D D 7 , A n d r e j t s c h e f f . R A D I O A C T I V I T Y *°a,l°SIn; m e a s u r e d ET,IT,I(ce),77(t),7(ee)(t). 1°8,'°6Cd d e d u c e d levels, 7-branching. V i b r a t o r p l u s p a r t i c l e , i n t e r a c t i n g b o s o n models. REPT IPN 1981 A n n u a l , P N 3 5 , Roussiere. R A D I O A C T I V I T Y l°8,mSIn [ f r o m Sn(p,xn2p),E=2O0 MeV; Sn(SHe,xnyp),E=270 MeVS; m e a s u r e d ET, IT,77(t),7(ce)(t),l(ee); deduced log f t , i s o m e r J. *°8,'°sCd d e d u c e d l e v e l s , 0 +" s t a t e d e c a y characteristics. Interacting b o s o n m o d e l . REPT I P N O - T - 8 1 - 0 5 , R o u s s i e r e . NUCLEAR REACTIONS l ° s C d ( p , n T ) , E = l o w ; m e a s u r e d a ( E T ) , 7 7 - c o i n , l°SIn d e d u c e d t r a n s i t i o n . REPT A N L - 8 1 - 7 9 , P 8 5 , A y s t o . R A D I O A C T I V I T Y l°6,1°eSn [ f r o m 54Fe(SSNi,X)]; m e a s u r e d 7 7 - , ( X - r a y ) 7 - c o i n ; deduced levels, 7-branching,J,Tr,neutron hl~/2 orbital excitation. REPT IPN 1980 A n n u a l , P N 2 1 , A u g e r .

A JoTpd

105

NUCLEAR REACTIONS *°°Mo(TLi,2n),(TLi,np),E n o t g i v e n ; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) , 7 7 ( 0 ) , o r i e n t e d n u c l e i . * ° S R h , i ° 5 R u d e d u c e d l e v e l s . B A P S A 27 7 2 7 , E C 6 , C a s t a i n . NUCLEAR REACTIONS l°°Mo(TLi,2n),(TLi,np),E n o t g i v e n ; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) , 7 7 ( 0 ) , o r i e n t e d n u c l e i , l ° S R h , * ° S R u d e d u c e d l e v e l s . B A P S A 27 7 2 7 , E C 6 , C a s t a i n . NUCLEAR REACTIONS l°SRh,nSSn(a,2n),E=27 MeV; m e a s u r e d E T , I T , l i n e a r p o l a r i z a t i o n , 7 ( 0 ). t65Ag d e d u c e d levels,J,rr,7-multipolarity,7-branchings,$. 12iTe d e d u c e d levels,ICC,Jjr, 7-multipolarity,6. REPT Z F K - 3 8 5 , P 3 2 , K e l l e r . NUCLEAR REACTIONS l°SRh,ilS, llSln((x,~nT),E=27 MeV; m e a s u r e d 7(0,H,t). l°SAg,nS,li7Sb l e v e l s d e d u c e d g. CONF R i g a , P 2 4 4 , L e b e d e v . R A D I O A C T I V I T Y I°3,I°51n [ f r o m on-line mass separator]; measured flT-coin,fl-endpoint energies; deduced Q ( E C ) , m a s s e x c e s s . CONF H e l s i n g o r V o ] l P 1 3 4 , CERN 8 1 - 0 9 . R A D I O A C T I V I T Y t°a,i°3,~°51n [ f r o m Mo,9~Mo(14N,X)]; m e a s u r e d flT-coin,Efl,Ifl,fl e n d - p o i n t e n e r g i e s . *°~,'°SIn d e d u c e d m a s s e s . B A P S A 26 1 1 4 6 , D D 6 , W o u t e r s . R A D I O A C T I V I T Y I°3,1°4,1°51n [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT JYFL 1981 A n n , P 5 5 , W o u t e r s .

A lOSRh

continued

NUCLEAR REACTIONS l°a,l°4pd(p,n),E < 7.2 MeV; m e a s u r e d i s o m e r i c ~ r a t i o v s (E). l°e,164Ag l e v e l s d e d u c e d J. CONF R i g a , P 2 8 9 , A v c h u k h o v . RADIOACTIVITY i°3,i°4,i°5In [ f r o m o n - l i n e m a s s separation3; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Q ( E C ) , m a s s e x c e s s . REPT J Y F L 1981 A n n , P 5 5 , W o u t e r s .

A = ~O5Ru

104

ONLY)

=

107

NUCLEAR REACTIONS l ° s , l ° s p d , n a , n O S n ( 3 H e , ~ ) , E = 7 0 MeV; m e a s u r e d # ( E a ) , 7 7 - c o i n , 7 ( e ). l°vPd deduced broad level,F,J,Tr,v-branehing. REPT KVI 1981 A n n , P l 5 , S a k a i . RADIOACTIVITY l°8m,l°gmSn,l°Tmln [from 94,95Mo(160)xnyp)]; measured Ti/2; d e d u c e d muIti-quasiparticle configurations. Centroid shift method. B A P S A 27 2 7 , D F 1 3 , Andrejtscheff. NUCLEAR REACTIONS l ° S c d ( 3 H e , 2 n ) , ( 3 H e , n p ) , E = 2 0 MeV; m e a s u r e d 77-coin,7(e). l°TSn,1°71n deduced levels,JJr,T-branching. REPT IPN 1981 A n n u a l , P N 5 1 , A u g e r . R A D I O A C T I V I T Y I°7Sn [ f r o m 1°sCd(3He,xn),E=35 MeV]; m e a s u r e d 7 7 - c o i n ; d e d u c e d t r a n s i t i o n s . REPT IPN 1980 A n n u a l , P N 1 4 , A u g e r .

244

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A lOTSn

R 81AuZW:

R

~OSAg

R 80BoZS

8ENaZU

81BoZP

82MiZ0 8EMiZX toOCd

D 81CoZR

81RoZ0

81RoZP

10Sin

D

80RoZP

81CoZR

81RoZO

81RoZP

lO8Sn

D 80AuZU 8EAnZY

R 81FIZW

189Ag

D 79DAZE

logCd

D 79DAZE

1O9In

R 82A1ZZ

iOOSn

D 81JoZX

82AnZY

R

81JoZX

continued

=

;°?Sn,~°?In

108

NUCLEAR REACTIONS l ° 4 , 1 ° 6 , 1 8 s , n ° P d ( p o l a r i z e d p , p ) , ( p o l a r i z e d p,p'),E=E2 MeV; m e a s u r e d ~(0), A(0). l°4,1°6,1°8,H°Pd d e d u c e d fiE,fla. DWBA a n a l y s i s . REPT U T T A C - 4 5 , P 3 8 , N a g a n o . NUCLEAR REACTIONS m ? A g ( n , y ) , E = t h e r m a l , r e s o n a n c e ; l°SAg(n,y),E=thermal; measured E%17, ??-coin. l°SAg d e d u c e d l e v e l s . REPT J U L - S p e z - 7 E , P T 1 , B o g d a n o v i c . NUCLEAR REACTIONS i 8 7 , 1 ° 9 A g ( n , y ) , E = t h e r m a l ; m e a s u r e d ?-spectra. 1°SAg d e d u c e d n e u t r o n binding energy,levels,J,rr,configuration. Phonon model, n°Ag deduced neutron binding energy. Pair spectrometer. REPT J U L - S p e z - 9 9 , P ? 6 , B o g d a n o v i c . NUCLEAR REACTIONS m?,mSAg(n,X),E < 7 keV; m e a s u r e d t r a n s m i s s i o n . ~°8,1mAg d e d u c e d s - w a v e strength functions,average l e v e l s p a c i n g s . REPT N E A N D C ( J ) - 8 3 / U , P 1 8 , M i z u m o t o . NUCLEAR REACTIONS l ° T A g ( n , y ) , E = t h e r m a l , r e s o n a n c e ; m e a s u r e d E T , I % 7 7 - c o i n , I ( c e ) , T ~ / a . ~°SAg deduced levels,J,rr,eonfigurations. REPT J U L - S p e z - 1 4 6 , P 4 9 , M i t s u n a r i . R A D I O A C T I V I T Y t0amAg,mSmIn [ f r o m Mo(~4N,xnyp),E=90 MeV]; m e a s u r e d yV(0),I(ce). ~°aPd,maCd deduced levels,J,w,E0 transition strength,B(E0)/B(E2). Interacting boson approximation calculations. CONF H e l s i n g o r V o l e P 4 6 0 , CERN 8 1 - 0 9 . RADIOACTIVITY t°s,i°6In; measured E%I%I(ce),7?(t),?(ce)(t). 188,1°6Cd d e d u c e d levels, ?-branching. Vibrator plus particle,interacting b o s o n m o d e l s . REPT IPN 1981 A n n u a l , P N 3 5 , Roussiere. R A D I O A C T I V I T Y '°6,~°6In [ f r o m Sn(p,xnEp),E=aO0 MeV; Sn(aHe,xnyp),E=E70 MeV]; m e a s u r e d E% I?,7?(t),7(ce)(t),I(ce); deduced log f t , i s o m e r J. ~°8,~°6Cd d e d u c e d levels,0 + state decay characteristics. Interacting b o s o n m o d e l . REPT I P N O - T - 8 1 - 0 5 , R o u s s i e r e . R A D I O A C T I V I T Y ~°8ln [ f r o m Sn(aHe,xn3p),E=g83 MeV]; m e a s u r e d 7y(t),7(ce)(t). REPT IPN 1980 Annual,PN35,Roussiere. R A D I O A C T I V I T Y t°emAg,~oSmln [ f r o m Mo(~4N,xnyp),E=90 MeV]; m e a s u r e d y?(0),I(ce), maPd,mSCd deduced levels,J,w,E0 transition strength,B(E0)/B(EE). Interacting boson approximation calculations. CONF H e l s i n g o r V o l e P 4 6 0 , CERN 8 1 - 0 9 . R A D I O A C T I V I T Y ~°a,t°SIn; m e a s u r e d Ey,I%I(ce),7y(t),y(ce)(t). ~°s,~°6Cd d e d u c e d levels, ?-branching. Vibrator plus particle,interacting b o s o n m o d e l s . REPT IPN 1981 A n n u a l , P N 3 5 , Roussiere. R A D I O A C T I V I T Y t8a,t°~In [ f r o m Sn(p,xnEp),E=E00 MeV; Sn(3He,xnyp),E=ET0 MeV]; m e a s u r e d E% I?,yT(t),?(ce)(t),l(ce); deduced log f t , i s o m e r J. 1°8,~°6Cd d e d u c e d levels,0 + state decay characteristics. Interacting b o s o n m o d e l . REPT I P N O - T - 8 1 - 0 5 , R o u s s i e r e . R A D I O A C T I V I T Y ~8~,~°eSn [ f r o m 54Fe(5aNi,X)]; m e a s u r e d 7 7 - , ( X - r a y ) 7 - c o i n ; deduced levels, y-branehing,J,rr,neutron h~l/a orbital excitation. REPT IPN 1980 A n n u a l , P N i l , A u g e r . R A D I O A C T I V I T Y ~°Sm,~°amSn,~°TrnIn [ f r o m 94,SSMo(~60,xnyp)]; measured Tl/a; deduced multi-quasiparticle configurations. Centroid shift method. B A P S A 27 2 7 , D F 1 3 , Andrejtscheff.

A lO~Rh

107

NUCLEAR REACTIONS ~ ° 6 C d ( a H e , g n ) , ( a H e , n p ) , E = E 0 MeV; m e a s u r e d 77-coin,7(0). deduced levels,J,rr,y-branching. REPT IPN 1981 A n n u a l , P N 5 1 , A u g e r .

A

~o~pd

=

ONLY)

=

109

NUCLEAR REACTIONS 7°Zn,l°4Ru,ll°Pd,i54Sm,15s,16°Gd,186W,196,1SSPt,2°2,EO4Hg,244pu(polarized t , a ) , 19Spt,a44pu,76Ge(polarized t , p ) , E = 1 7 MeV; s E , 8 ° S e , l ° ° M o , i a a , l ~ 4 S n ( p o l a r i z e d t,SHe),E=22-25 MeV; m e a s u r e d a(0),analyzing p o w e r v s 0 , a ( E a ) , a ( E p ) , a ( S H e ) . 89Cu,l°STc,1°SRh,153pm,15?,l~SEu, ~SSTa,195,197Ir,e°l,2°aAu,243Np,2°°Pt,246pu,78Ge,8°,SaAs,i°°Nb,t22,12¢ln d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . R A D I O A C T I V I T Y l°sCd; m e a s u r e d I(ce). 1°SAg t r a n s i t i o n s deduced subshell intensity ratios. P r i s m fl s p e c t r o m e t e r , C d , C d T e , C d S e s o u r c e s . CONF R i g a , P g 3 3 , D a v i d o n i s . R A D I O A C T I V I T Y l°9Cd; m e a s u r e d I(ce). ~°°Ag t r a n s i t i o n s deduced subshell intensity ratios. P r i s m fl s p e c t r o m e t e r , C d , C d T e , C d S e s o u r c e s . CONF R i g a , P E 3 3 , D a v i d o n i s . NUCLEAR REACTIONS l°?,l°SAg,~21,12asb(sHe,n),E=E5.4 MeV; m e a s u r e d a ( E n ) . I°9,1111n d e d u c e d l e v e l s , L . B A P S A 27 5 1 ? , E X a 3 , A l f o r d . R A D I O A C T I V I T Y l°sSb [ f r o m 9aMo(Z°Ne,X)]; m e a s u r e d E % I % ( X - r a y ) ? - , 7 ? - , f l ? - c o i n , f l + e n d p o i n t energy,T1/2; deduced Q(EC),log f t . l ° 9 S n d e d u c e d levels,J,Tr,y-branching. CONF H e l s i n g o r V o l e P 4 6 9 , CERN 8 1 - 0 9 . RADIOACTIVITY l°Sm,l°amSn,l°?mIn I-from 94,SSMo(lSO,xnyp)]; measured T1/2; d e d u c e d multi-quasiparticle configurations. Centroid shift method. B A P S A 27 ET,DF13, Andrejtscheff. NUCLEAR REACTIONS m6Cd(a,n),E=lE.5-18 MeV; m e a s u r e d E ? , I ? , n y - , y y - c o i n , y ( O ) . l°9Sn d e d u c e d levels,J,w,?-branching,y-multipolarity. Enriched target. Legendre polynomial analysis. CONF H e l s i n g o r V o l e P 4 6 9 , CERN 8 1 - 0 9 .

245

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

ioSSb

D 81JoZX:

R 81HaZO:

83NaZU:

llOAg

D 83SuZZ: R 81BoZP:

82MiZ0: txoCd

R 81HyZY:

li6in

R 80GeZY:

D 79TrZN:

l~ICd

D 79TrZN: J

'Uln

82ElZX:

D 79TrZN: R 83AIZZ:

1,1Sn

R 80PeZR:

81DuZV: 82HyZZ:

83MaZK:

=

=

D 79BaYK:

n2Sn

R 79DeYT: 81JoZY:

83LiZX:

i10

111

RADIOACTIVITY " l A g , U l l n ; m e a s u r e d E(ce),I(ce). l u C d d e d u c e d I C C , 8 , M l - , E 2 - p e n e t r a t i o n parameters. CONF R i g a , P 7 4 , T r o i t s k a y a . RADIOACTIVITY U l A g , l ' l l n ; m e a s u r e d E(ce),I(ce). u l C d d e d u c e d I C C , ( ~ , M l - , E E - p e n e t r a t i o n parameters. CONF R i g a , P 7 4 , T r o i t s k a y a . NUCLEAR MOMENTS lnCd,OORu; m e a s u r e d h y p e r f i n e m a g n e t i c f i e l d vs T. T i m e d i f f e r e n t i a l perturbed angular correlation method,chalcogenide S p i n e l s . DABBB 42 4 1 0 3 , E l f a z a n i . RADIOACTIVITY ' l ' A g , l U l n ; m e a s u r e d E(ce),I(ce). l n C d d e d u c e d I C C , ( ~ , M l - , E E - p e n e t r a t i o n parameters. CONF R i g a , P 7 4 , T r o i t s k a y a . NUCLEAR REACTIONS 'o7,1°gAg,lal,12aSb(3He,n),E=25.4 MeV; m e a s u r e d o'(En), l ° 9 , n ' I n d e d u c e d l e v e l s , L . BAPSA 37 5 1 7 , E X a 3 , A l f o r d . NUCLEAR REACTIONS n 2 , U 6 S n ( p o l a r i z e d d,t),E=40 MeV; m e a s u r e d a ( 0 ) , a n a l y z i n g p o w e r v s 0. nl,USSn deduced valence-,inner-hole s t a t e s , J . V e c t o r p o l a r i z e d b e a m . REPT IPN 1980 Annual,PN16,Perrin. NUCLEAR REACTIONS n 2 S n ( p o l a r i z e d d,t),E=40 MeV; m e a s u r e d a n a l y z i n g p o w e r v s 0. UlSn deduced levels,J,n,configuration. DWBA a n a l y s i s . REPT ISN 8 1 - 0 1 , P 4 4 , D u h a m e l . NUCLEAR REACTIONS n2,u6,1a°,la4Sn(p,d),E=50-65 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l parameters, ln,lis,uo,iUasn deduced levels,L,Jjr. Zero-range DWBA,local a p p r o x i m a t i o n . REPT RCNP Osaka,1981 A n n , P 5 9 , H y a k u t a k e . NUCLEAR REACTIONS 112,116,12°,124Sn(p,d),E=50,65 MeV; m e a s u r e d a(Ed),cr(0), l u , l l s , n o , 1 2 3 S n d e d u c e d L=l,4 s p e c t r o s c o p i c s t r e n g t h f u n c t i o n s , h o l e s t a t e f r a g m e n t a t i o n . High r e s o l u t i o n spectrograph. REPT RCNP 0 s a k a , 1 9 8 1 A n n , P 6 1 , M a t o b a .

A liaAg

continued

NUCLEAR REACTIONS l°6,1o8,u°Pd(208Pb,2OSpb'),E=878 MeV; m e a s u r e d ET,17,Coulomb e x c i t a t i o n . u ° P d d e d u c e d levels,B(E2). I n t e r a c t i n g b o s o n , b o s o n e x p a n s i o n m o d e l s . REPT A - T L U - 8 0 1980, Annual Repot t,P43,Hasselgren. NUCLEAR REACTIONS l ° 4 , 1 ° ° , l ° 8 , n ° P d ( p o l a r i z e d p , p ) , ( p o l a r i z e d p,p'),E=33 MeV; m e a s u r e d a(0), A(0). l°4,1°6,1°s,n°Pd d e d u c e d f12,f13. DWBA a n a l y s i s . REPT U T T A C - 4 5 , P 3 8 , N a g a n o . RADIOACTIVITY ll°Ag [ f r o m l°gAg(n,-?)]; m e a s u r e d E T , I - / , I ( c e ) , 7 7 - c o i n ; d e d u c e d l e v e l s , J , ~ , 7-multipolarity,7-branching. REPT J U L - S p e z - 1 4 6 , P 5 0 , S u s h s o v . NUCLEAR REACTIONS l ° 7 , ] ° g A g ( n , - f ) , E = t h e r m a l ; m e a s u r e d 7 - s p e c t r a . ~°6Ag d e d u c e d n e u t r o n binding energy,levels,J,~r,configuration. Phonon model, n°Ag deduced neutron binding energy. Pair spectrometer. REPT J U L - S p e z - 9 9 , P 7 6 , B o g d a n o v i c . NUCLEAR REACTIONS l°7,m9Ag(n,X),E < 7' keV; m e a s u r e d t r a n s m i s s i o n , l°s,n°Ag deduced s - w a v e strength functions,average l e v e l s p a c i n g s . REPT N E A N D C ( J ) - 8 3 / U , P 1 6 , M i z u m o t o . NUCLEAR REACTIONS '96,19Spt,n~Cd(p,t),E=54.6 MeV; m e a s u r e d a ( 0 ) , t r i t o n m o m e n t u m spectra. n°Cd deduced 8+ level population. Zero-range DWBA. REPT RCNP O s a k a , 1 9 8 0 A n n , P 8 3 , Hyakutake. NUCLEAR REACTIONS l°°Mo(~4N,4n),E n o t g i v e n ; m e a s u r e d E - f , I T , 7 7 - c o i n , - / ( 0 ) , 7 - p o l a r i z a t i o n , I(ce). n ° I n d e d u c e d l e v e l s . REPT ISN 8 0 - 0 1 , P 3 9 , G e n e v e y .

A lllAg

109

RADIOACTIVITY '°gSb [ - f r o m 9aMo(aONe,X)]; m e a s u r e d E3,,I~/,(X-ray)7-,77-,flT-coin,fl + e n d p o i n t e n e r g y , T 1 / 2 ; d e d u c e d Q(EC),log f t . ~°aSn d e d u c e d l e v e l s , J j r , ~ / - b r a n e h i n g . CONF H e l s i n g o r Vol2 P469, CERN 8 1 - 0 9 .

A n0pd

=

ONLY)

112

RADIOACTIVITY ll2Ag [ f r o m li°Pd(a,d)]; m e a s u r e d -/7(e); deduced A2,A4. CONF Riga,P75, Babenko. NUCLEAR REACTIONS ua,114Sn(n,n'~/),E=fast; measured ~/(0). ua,U4Sn t r a n s i t i o n s deduced 6. CONF Riga,P531,Demidov. NUCLEAR REACTIONS i12,114,116,11e,la°Sn(160,160'),E=48 MeV; m e a s u r e d E%IT,double Coulomb c x c i t a t i o n , 7 7 - c o i n . 112,1~4,u6,118,12OSn levels deduced B(E2),B(E3). REPT A-TLU-80 1980, A n n u a l Repor t,P49,Jonsson. NUCLEAR REACTIONS 9°,92,94Zr,lla,li6,124Sn(p,n),E=79.2 MeV; m e a s u r e d a(0). i'a,li°,la4Sn deduced n e u t r o n to p r o t o n r m s r a d i u s ratio. DWBA a n a l y s i s . BAPSA 27 26,DF7,Lind.

246

SECONDARY

SOURCES

(Reports,Abstracts,etc

A Hapd

D

81MeZY

HaAg

D

81MeZY

D 31MeZY

ll4Sn

R '79DeYT 30IsZX

BIDuZU 91JoZY

li4Te

R B2JaZY

D :91MeZY

nSAg

D BIMeZY

H51n

D 79MaYS R 8OLeZK

115Sn

R 80PeZR

80PeZS 81DeZC 32HyZZ

32MaZK

usSb

R 79LeZK R 82PiZY

R 79IvZX

80GaZO 80IsZX

levels

deduced

na,llSAg

levels

deduced

114

=

I15

RADIOACTIVITY u3,::4,115Pd [ f r o m a5aCf(SF)]; m e a s u r e d E7,I3'. li3,USAg l e v e l s d e d u c e d 7-branching. CONF 181st ACS Mtg,NUCL 5 7 , M e i k r a n t z . RADIOACTIVITY u a , l ' 4 , 1 ' s P d [ f r o m aSZcf(SF)]; m e a s u r e d E7,!% 113,U5Ag l e v e l s d e d u c e d 7-branching. CONF 181st ACS Mtg,NUCL 5 7 , M e i k r a n t z . RADIOACTIVITY ltSmIn; m e a s u r e d I T - d e c a y p r o b a b i l i t y ; d e d u c e d c h e m i c a l i n f l u e n c e on probability. I n , I n F 3 , I n C 1 a s o u r c e s . CONF R i g a , P 3 3 4 , M a k a r y u n a s . NUCLEAR REACTIONS 6°Ni,gOZr,llSIn,ta°Sn,144Srn,16SHo,197Au,2°spb(aHe,3He'),E=lOS.5 MeV; m e a s u r e d (7(E(3He)),a(0). 6°Ni d e d u c e d CQR,F. 9°Zr,llSln,l~°Sn,'t4SmJdSHo,197Au d e d u c e d GQR, g i a n t m o n o p o l e r e s o n a n c e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS n ~ , U % n ( p o l a r i z e d d,t),E=40 MeV; m e a s u r e d c r ( 0 ) , a n a l y z i n g p o w e r v s 0. ul,llSSn deduced valence-,inner-hole s t a t e s , & V e c t o r p o l a r i z e d b e a m . REPT IPN 1980 Annual,PN16,Perrin. NUCLEAR REACTIONS U % n ( p o l a r i z e d d,t),E=40 MeV; m e a s u r e d a ( 0 ) , v e c t o r a n a l y z i n g p o w e r vs 0. llSSn l e v e l s d e d u c e d L,J,Tr. DWBA a n a l y s i s . REPT ISN 8 0 - 0 1 , P 5 0 , P e r r i n . NUCLEAR REACTIONS e°aPb,n%n(3He,a),E=283 MeV; m e a s u r e d (~(Ea). USSn d e d u c e d l e v e l s , J j r , configuration. REPT IPN 1981 A n n u a l , P N 6 8 , D e v a u x . NUCLEAR REACTIONS lla,n6,1a°,ta4Sn(p,d),E=50-65 MeV; m e a s u r e d or(0); d e d u c e d o p t i c a l m o d e l parameters, n~,us,ng,~23Sn d e d u c e d l e v e l s , L , J , r r . Z e r o - r a n g e DWBA,locaI a p p r o x i m a t i o n . REPT RCNP Osaka,1981 A n n , P 5 9 , H y a k u t a k e . NUCLEAR REACTIONS n2,116)2°,le4Sn(p,d),E=50,65 MeV; m e a s u r e d o'(Ed),cr(0), ul,ns,119,123Sn d e d u c e d L=l,4 s p e c t r o s c o p i c s t r e n g t h f u n c t i o n s , h o l e s t a t e f r a g m e n t a t i o n . High r e s o l u t i o n spectrograph. REPT RCNP 0 s a k a , 1 9 8 1 A n n , P 6 1 , M a t o b a . NUCLEAR REACTIONS l°3Rh,U3,USIn(a,RnT),E=27 MeV; m e a s u r e d 3'(0,H,t). '°SAg,U5,uTSb l e v e l s d e d u c e d g. CONF R i g a , P 2 4 4 , L e b e d e v . NUCLEAR REACTIONS l°dCd(~eC,3np),E=63 MeV; m e a s u r e d not given, hal deduced levels, c o l l e c t i v e b a n d p r o p e r t i e s . BAPSA 27 7 2 8 , E C 7 , P i e l , J r . .

A

11SSn

=

lta,USAg

RADIOACTIVITY u a , l l 4 , u s P d [ f r o m aSZcf(SF)]; m e a s u r e d E7,I7. na,tlSAg l e v e l s d e d u c e d 7-branching. CONF 181st ACS Mtg,NUCL 5 7 , M e i k r a n t z . NUCLEAR REACTIONS u a , n ~ S n ( n , n ' 7 ) , E = f a s t ; m e a s u r e d 7(0). u a , n 4 s n t r a n s i t i o n s d e d u c e d 6. CONF R i g a , P 5 3 1 , D e m i d o v . NUCLEAR REACTIONS U 6 S n ( p , t ) , E = a g . 5 MeV; n S S n ( p , t ) , E = 3 0 . 4 MeV; l a ° S n ( p , t ) , E = a g . 1 MeV; measured (~(0). u ~ , u ~ , l ' S S n d e d u c e d 0 + s t a t e c h a r a c t e r . DWBA a n a l y s i s , d i r e c t , t w o - s t e p p r o c e s s . REPT INS T o k y o 1980 A n n , P 3 6 , I s h i z a k i . NUCLEAR REACTIONS SSNi,ndSn,a°sPb(a,dHe),E=218 MeV; m e a s u r e d cr(0),cr(E(~He)). 5~NiJl*Sn, a°dPb d e d u c e d l e v e l s . REPT IPN 1981 A n n u a l , P N T 1 , D u h a m e l . NUCLEAR REACTIONS u a , u ¢ , u ~ , H s , t a ° S n ( l a O , t 6 0 ' ) , E = 4 8 MeV; m e a s u r e d E T , I T , d o u b l e C o u l o m b exeitation,77-coin. Ha,u4,n6,11a,la°Sn l e v e l s d e d u c e d B(Ea),B(E3). REPT A - T L U - S O 1980, Annual Report,P49,Jonsson. NUCLEAR REACTIONS ~4Mo(aaNa,inp),E=85 MeV; 92Mo(laC,3n),E=48 MeV; m e a s u r e d 7 7 - c o i n . n4Te, t°aCd d e d u c e d h i g h - s p i n s t a t e s . PHCAA 38 41,FAa,Janzen.

A i15pd

113

RADIOACTIVITY i13,114,115pd [from aSacf(SF)]; m e a s u r e d E%! 7. 7-branching. CONF 181st ACS Mtg,NUCL 5 7 , M e i k r a n t z . RADIOACTIVITY ll3,114,11spd [ f r o m a S a c f ( S F ) ] ; m e a s u r e d E7,I7. 7-branching. CONF 181st ACS Mtg,NUCL 5 7 , M e i k r a n t z .

A ll4pd

=

ONLY)

=

116

NUCLEAR REACTIONS az,96,aSMo,nd,la4Sn(a,a),(a,a'),E=39.3,40,45,50 MeV; measured ~(E,0). 92, 96,9aMo,tls,la4Sn deduced d e f o r m a t i o n p a r a m e t e r ft. Blair phase method. CONF Riga,P321, Ivanov. NUCLEAR REACTIONS 9°Zr,ltaSn,a°apb(a,dHe),E=218 MeV; m e a s u r e d cr(E(eHe)). 8SZr,116Sn,a°dPb deduced levels,broad s t r u c t u r e s . REPT IPN 1980 Annual,PNl4,Gales. NUCLEAR REACTIONS UdSn(p,t),E=29.5 MeV; tlaSn(p,t),E=30.4 MeV; la°Sn(p,t),E-29.1 MeV; m e a s u r e d ~(0). ii4,ue,ltSSn deduced 0 + state c h a r a c t e r . DWBA a n a l y s i s , d i r e c t , t w o - s t e p process. REPT INS Tokyo 1980 Ann,P36,1shizaki.

247

SECONDARY

SOURCES

(Repor[s,Abstracts,etc.

A llSSn

R 81JoZY:

82LiZX:

D 81ZaZY:

l~7in

D 81ZaZY:

H7Sn

D 80MuZT: R 82NiZX:

ll7sb

R 79LeZK:

ll7Te

R 79HaYF: 79KaYX:

D 81KaZP: R 80IsZX:

81JoZY:

81MaZH: uaSb

D 81KaZP: R 82YaZZ:

na I

R 82WaZR:

R 80CrZY: 81DiZU: 810kZY:

82HyZZ:

82MaZK

82NiZX 820kZY

=

117

=

118

RADIOACTIVITY n s S b [ f r o m 121Sb(p,4n)nSTe d e c a y ] ; m e a s u r e d I(ce),I7,77(0). USSn d e d u c e d levels,Jjr,(E0/E2),relative m o n o p o l e s t r e n g t h . N a t u r a l t a r g e t . REPT l N S - 4 3 4 , K a w a k a m i . NUCLEAR REACTIONS l i e S n ( p , t ) , E = 2 9 . 5 MeV; n S S n ( p , t ) , E = 3 0 . 4 MeV; 12OSn(p,t),E=29.1 MeV; measured a ( 0 ) . ll4,11a,llSSn d e d u c e d 0 + s t a t e c h a r a c t e r . DWBA a n a l y s i s , d i r e c t , t w o - s t e p p r o c e s s . REPT INS T o k y o 1980 A n n , P 3 6 , 1 s h i z a k i . NUCLEAR REACTIONS n2,H4,ue,ua,12°Sn(~eo,lSo'),E=48 MeV; m e a s u r e d E % I T , d o u b l e C o u l o m b excitation,-/~/-coin, nz,l'4,n6,na,12°Sn levels deduced B(E2),B(E3). REPT A - T L U - 8 0 1980, Annual Repot t,P49,Jonsson. NUCLEAR REACTIONS llaSn(~r+,~r+'),(rr-,rr-'),E=130 MeV; m e a s u r e d a(0). 'laSh d e d u c e d T=0,GQR, o c t u p o l e r e s o n a n c e , a ( T r - ) / a ( T r + ) . DWBA a n a l y s i s . REPT D O E / E R / 4 0 0 1 4 - 3 , P 5 1 , M a s t e r s o n . RADIOACTIVITY 'loSb [ f r o m 121Sb(p,4n)naTe d e c a y ] ; m e a s u r e d I(ce),I%77(0). n S S n d e d u c e d levels,J,rr,(E0/E2),relative monopole strength. N a t u r a l t a r g e t . REPT I N S - 4 3 4 , K a w a k a m i . NUCLEAR REACTIONS u 4 C d ( 7 L i , 3 n ) , E = 3 2 MeV; l l o p d ( ' l B , 3 n ) , E = 4 3 MeV; m e a s u r e d 7(0),~7(t), 7(TLi)(t),7(nB)(t). nnSb deduced levels,Jjr,band structure. BAPSA 27 5 1 7 , E X a l , Y a n g . NUCLEAR REACTIONS n 4 S n ( 7 L i , 3 n ) , E = 3 4 MeV; n z C d ( l ° B , 4 n ) , E = 5 0 MeV; m e a s u r e d (r(ET),7(0), 77(t). "8I deduced levels,band structure,E2 crossovers,configurations. BAPSA 27 728,EC8, Watson,III.

A 119Sn

continued

RADIOACTIVITY nTCd; m e a s u r e d 77(0,H). 117In l e v e l d e d u c e d g. REPT I N D C ( B Z L ) - 5 / G , P 4 , Zamboni. RADIOACTIVITY uTCd; m e a s u r e d 77(0,H). 117In l e v e l d e d u c e d g. REPT I N D C ( B Z L ) - 5 / G , P 4 , Zamboni. RADIOACTIVITY UTSn [ f r o m u s C d ( a , 3 n ) ] ; m e a s u r e d I(ce),Auger s p e c t r a . REPT INS T o k y o 1980 Ann,P34,Muramatsu. NUCLEAR REACTIONS n s , u s , 1 2 ° , 1 2 a , 1 2 4 S n ( n , n ) , E = l - 2 0 0 keV; m e a s u r e d a(E). n~,Ug,lZl,12a,12SSn deduced s-,p-wave strength functions,radius p a r a m e t e r s . REPT J I N R - P 3 - 8 2 - 4 3 6 , N i k o l e n k o . NUCLEAR REACTIONS ~°3Rh,na,l~SIn(a,2nT),E=27 MeV; m e a s u r e d ~/(0,H,t). lasAg,n5,nTSb l e v e l s d e d u c e d g. CONF R i g a , P ~ 4 4 , L e b e d e v . NUCLEAR REACTIONS n s , u 7 , U g s n ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d ( ~ ( t ) . n7,ua,t21Te d e d u c e d levels, isomer T~/~,-/-multipolarity,rotational b a n d s , J , T r . REPT Z F K - 3 8 5 , P 3 7 , H a g e m a n n . NUCLEAR REACTIONS n ~ , U g S n ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d ET,I7,7(0,H,t). ~7,~Te level d e d u c e d tz. REPT Z F K - 3 8 5 , P 4 2 , K a u b l e r .

A UaSn

116

NUCLEAR REACTIONS nu,'14,1'e,ns,12°Sn('e0,1°0'),E=48 MeV; m e a s u r e d E T , I T , d o u b l e C o u l o m b excitation,77-coin, l'a,'~4,n6,ua,12asn levels deduced B(E2),B(E3). REPT A - T L U - 8 0 1980, Annual Repor t,P49,Jonsson. NUCLEAR REACTIONS ~ ° , a ~ , 9 4 Z r , n ~ , u 6 , 1 ~ 4 S n ( p , n ) , E = 7 9 . 2 MeV; m e a s u r e d ~r(0). ll~,116,1a4Sn deduced neutron to p r o t o n r m s r a d i u s r a t i o . DWBA a n a l y s i s . BAPSA 27 2 6 , D F 7 , L i n d .

A ll7Cd

=

ONLY)

=

119

NUCLEAR REACTIONS 9°Zr,12OSn(polarized p,d),E=90 MeV; m e a s u r e d a n a l y z i n g p o w e r v s 0. 1'9Sn deduced broad structure,J. REPT IPN 1980 A n n u a l , P N 1 7 , C r a w l e y . NUCLEAR REACTIONS lZ°Sn(p,d),E=26.3 MeV; m e a s u r e d a(0). n g S n l e v e l s d e d u c e d C2S. DWBA c a l c u l a t i o n s . REPT D O E / E R / 4 0 0 1 4 - 3 , P 6 , D i c k e y . NUCLEAR REACTIONS UgSn(a,a%E=109 MeV; m e a s u r e d (xn-coin,a(0~),cr(0~,0n,E(x,En); d e d u c e d n e u t r o n e m i s s i o n m e c h a n i s m , n g S n d e d u c e d GQR d e c a y c h a r a c t e r i s t i c s f o l l o w i n g n e u t r o n d e c a y . Tof,NE213 l i q u i d s c i n t i l l a t o r s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 4 9 , 0 k a d a . NUCLEAR REACTIONS u2,ns,12°,124Sn(p,d),E=50-65 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l parameters, lll,115,119,12aSn deduced levels,L,Jjr. Zero-range DWBA,local a p p r o x i m a t i o n . REPT RCNP Osaka,1981 A n n , P 5 9 , H y a k u t a k e . NUCLEAR REACTIONS 112,us,120,i24Sn(p,d),E-50_ ,65 MeV; m e a s u r e d ~(Ed),a(0). ul,lls,llg,iZaSn d e d u c e d L=l,4 s p e c t r o s c o p i c s t r e n g t h f u n c t i o n s , h o l e state fragmentation. High resolution spectrograph. REPT RCNP Osaka,1981 A n n , P 6 1 , M a t o b a . NUCLEAR REACTIONS n 6 , u a , ' z ° , l e 2 , 1 e 4 S n ( n , n ) , E = l - 2 0 0 keV; m e a s u r e d a(E). nT,ng,lal,12a,leSSn deduced s-,p-wave strength functions,radius p a r a m e t e r s . REPT J I N R - P 3 - 8 2 - 4 3 6 , N i k o l e n k o . NUCLEAR REACTIONS U%n(a,a'n),E=109 MeV; m e a s u r e d a(0a,Ea),an(0), n g s n d e d u c e d CQR decay characteristics. REPT RCNP Osaka,1981 A n n , P 5 5 , 0 k a d a .

248

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

ligTe

R 79HaYF:

llgxe

R 80BaZJ:

R 82MaZW:

*aOSn

R 80LeZK:

80MoZE: 81DjZR:

81DjZT:

81JoZY:

8EGuZY: ~a0Sb

R 82MaZW:

82VaZR: 82VaZX:

~a91

R 81PiZZ

R 79BaYJ 82NiZX

i~lTe

R 79HaYF 79KaYX: 79KeZW:

82GaZZ:

R 81F1ZW:

122Te

R 810kZX:

=

120

=

121

NUCLEAR REACTIONS 12°,122,124Sn(n,'y),E=thermal; m e a s u r e d ET,Iy. 121 ~aa,leSSn d e d u c e d t r a n s i t i o n s . CONF R i g a , P 7 6 , B a r c h u k . NUCLEAR REACTIONS ll6,Hs,la°,'2z,le4Sn(n,n),E=l-200 keV; m e a s u r e d ¢(E). 117,1~9,1~i,le3,~25Sn d e d u c e d s - , p - w a v e s t r e n g t h f u n c t i o n s , r a d i u s p a r a m e t e r s . REPT J I N R - P 3 - 8 ~ - 4 3 6 , N i k o l e n k o . NUCLEAR REACTIONS Jls,'JT,~l%n(a,2n),E=27 MeV; m e a s u r e d ~y(t). i]~,'Jg,~a~Te d e d u c e d levels, isomer T,/2,-/-multipolarity,rotational bands,J,rr~ REPT Z F K - 3 8 5 , P 3 7 , H a g e m a n n . NUCLEAR REACTIONS ' l s , J t g s n ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d ET,I3',3'(0,H,t). llT,~aJTe l e v e l d e d u c e d /z. REPT Z F K - 3 8 5 , P 4 2 , K a u b l e r . NUCLEAR REACTIONS i°aRh,'igSn(a,2n),E=27 MeV; m e a s u r e d E % I % l i n e a r p o l a r i z a t i o n , ~ / ( 0 ) . J°SAg d e d u c e d l e v e l s , J , r r , ~ / - m u l t i p o l a r i t y , - y - b r a n c h i n g s , & 1CiTe d e d u c e d levels,ICC,J,~r, - / - m u l t i p o l a r i t y , ~ . REPT Z F K - 3 8 5 , P 3 2 , K e l l e r . NUCLEAR REACTIONS ~2~,~°Te(3He,a),E=70 MeV; J2e,124,~a°Te(p,d),E=40 MeV; m e a s u r e d (7(0), cr(Ea),a(Ed). *zJ , a a , J a g T e d e d u c e d levels,L,J,Tr,C~S. Enriched targets,magnetic s p e c t r o m e t e r . DWBA a n a l y s i s , i n n e r s h e l l e x c i t a t i o n . REPT I P N O - D R E - 8 2 - 0 6 , G a l e s .

A :22in

continued

NUCLEAR REACTIONS l~°Sn(~r+,rrO),(rr-,rr°),E=100-170 MeV; m e a s u r e d cr(E(vr)),cr(O), t2°In,lS°Sb d e d u c e d I A S , i s o v e c t o r g i a n t m o n o p o l e , d i p o l e r e s o n a n c e , C D R i s o s p i n s p l i t t i n g . BAPSA 27 509,EF9,Matis. NUCLEAR REACTIONS ~°Ni,9°Zr,l~SIn,le°Sn,144Sm,~SHo,197Au,2°spb(aHe,3He'),E=108.5 MeV; m e a s u r e d (7(E(aHe)),cr(0). 6°Ni d e d u c e d GQR,F. 9°Zr,tt5In,ie°Sn,144Sm,~SHo,'97Au d e d u c e d GQR, g i a n t m o n o p o l e r e s o n a n e e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS 9°Zr,ie°Sn,a°sPb(a,(x'),E=100,172 MeV; m e a s u r e d a(Ea'). 9°Zr,l~°Sn,eOspb d e d u c e d GQR,giant m o n o p o l e r e s o n a n c e s , F . REPT J U L - S p e z - 7 2 ~ P 8 , M o r s c h . NUCLEAR REACTIONS 4°Ca,SlV,SO,s6,6~Ni,SSZn,9°,9~,94,96zr,ga,94,96,ge,l°6Mo,12o,l~4Sn,14OCe(p,p,), E=201 MeV; m e a s u r e d cr(Ep'). 4°Ca,5~V,SS,69,SaNi,~SZn,go,9~,94,S6Zr 9~,94,96,9s 1OOMo,iao,~4Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS a°spb,197Au,ia°Sn(p,p'),E=201 MeV; m e a s u r e d ~r(Ep'),~(0). ~97Au,~2°Sn d e d u c e d g i a n t r e s o n a n c e F. ~°spb d e d u c e d g i a n t r e s o n a n e e , F , T , 7 - m u l t i p o l a r i t y . REPT ]PN 1981 A n n u a l , P N 5 8 , D j a l a l i . NUCLEAR REACTIONS ~l~,lx¢,l~6,t~,t~°Sn(~So,~So'),E=48 MeV; m e a s u r e d Ey,IT,double C o u l o m b e x c i t a t i o n , T T - c o i n . ~la,l'4,il6,11s,ie°Sn l e v e l s d e d u c e d B(E~),B(E3). REPT A - T L U - 8 0 1980, Annual Report,P49,Jonsson. NUCLEAR REACTIONS 54,SSFe,SSNi,l~°Sn,Z°sPb(polarized n,n'),E=10 MeV; m e a s u r e d A(O). 5¢,SSFe, 58Ni,le°Sn,e°oPb level d e d u c e d s p i n - o r b i t d e f o r m a t i o n p a r a m e t e r s . BAPSA 27 542,GYa2,Guss. NUCLEAR REACTIONS le°Sn(~r+,rr°),(rr-,~r°),E=100-170 MeV; m e a s u r e d a(E(rr)),a(0). ~Z°In,le°Sb d e d u c e d I A S j s o v e c t o r g i a n t m o n o p o l e , d i p o l e r e s o n a n c e , G D R i s o s p i n s p l i t t i n g . BAPSA 27 509,EFg,Matis. NUCLEAR REACTIONS llsCd(TLi,3n),E=29 MeV; m e a s u r e d n o t g i v e n , l~°Sb d e d u c e d l e v e l s , h i g h - s p i n s t a t e c o n f i g u r a t i o n s . I n - b e a m s p e c t r o s c o p y . BAPSA 27 728,EC9,Vajda. NUCLEAR REACTIONS ~16Cd(TLi,3n),E=39 MeV; m e a s u r e d ~r(ET),'~(0),TT(t). la°Sb d e d u c e d levels, b a n d s t r u c t u r e . BAPSA 27 517,EXa4,Vajda. NUCLEAR REACTIONS ~16Sn(TLi,3n),E=34 MeV; m e a s u r e d ~r(ET),7(0),77(t ). l~°I d e d u c e d levels, y-branching,band s t r u c t u r e . BAPSA 26 l147,DD8,Piel.

A ~aISn

119

NUCLEAR REACTIONS ~5,~'7,~'gSn(a,3n),E=27 MeV; m e a s u r e d a3,(t). 1~7,1~9,121Te d e d u c e d levels, isomer Tt/a,3,-multipolarity,rotational b a n d s , J , ~ . REPT Z F K - 3 8 5 , P 3 7 , H a g e m a n n . NUCLEAR REACTIONS H°Cd(~aC,3n),E n o t given; m e a s u r e d ~?-~-coin. ~9Xe d e d u c e d levels,J~Tr, 3,-multipolarity,band s t r u c t u r e . REPT ISN 80-01,P31,Barci.

A ~Oln

=

ONLY)

=

122

NUCLEAR REACTIONS 7°Zn,l°4Ru,ll°Pd,154Sm,iSs,16°Gd,186W,19s,198pt,zoe,ZO4Hg,244pu(polarized t,a), 1 9 8 P t , a 4 4 p u , 7 6 G e ( p o l a r i z e d t,p),E=17 MeV; 8a,S°Se,l°°Mo,ta~,la4Sn(polarized t aHe),E=22-25 MeV; m e a s u r e d a ( e ) , a n a l y z i n g p o w e r vs 0,a(Ea),a(Ep),cr(3He). 69CuloaTclOgRh,~Sapmlsv,~SgEu ' iSSTa,195,197Ir,2°l,2°aAu,a4aNp,a°°Pt,e46pu,VSGe,e°,~aAs,i°°Nb,iZ2,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r Voll PlO7, CERN 81-09. NUCLEAR.REACTIONS 5SNi,nSSn(lSO,l~C),E=80 MeV; m e a s u r e d G(E(12C)),a(e). 6aZn,~2ZTe d e d u c e d l e v e l s , p o s s i b l e J,Tr. REPT RCNP Osaka,1980 A n n , P 9 3 , 0 k u m a .

249

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A R 82QuZX

~aXe

R 80KuZR 82HaZV

82SoZZ

R 79BaYJ:

82HyZZ:

82MaZK:

82NiZX:

~3Te

R 82GaZZ:

R 81F1ZW:

la4Sn

R 791vZX:

81DjZR:

82LiZX: 8~eZT: 82WeZY: ~a~Sb

D 8IYoZX: R 79GuZV: 820hZX:

la4Te

R 79DeYS:

la4Xe

R 80KuZR: 82HaZV:

82SoZZ:

continued

=

1~3

NUCLEAR REACTIONS l a 6 , 1 a a , ' a 4 S n ( n , 7 ) , E = t h e r m a l ; measured E % I 7 . ~al,~aa,laSSn d e d u c e d transitions. CONF R i g a , P 7 6 , B a r c h u k . NUCLEAR REACTIONS u ~ , n ° , ~ ° , ~ 4 S n ( p , d ) , E = 5 0 - 6 5 MeV; m e a s u r e d a(0); d e d u c e d o p t i c a l m o d e l parameters. , u ~,5,ng,~aaSn d e d u c e d levels,L,J,Tr. Zero-range DWBA,local approximation. REPT RCNP O s a k a , 1 9 8 1 A n n , P 5 9 , H y a k u t a k e . NUCLEAR REACTIONS l ~ , n 6 , ~ a ° , l a 4 S n ( p , d ) , E = 5 0 , 6 5 MeV; m e a s u r e d a(Ed),a(0). 'u,l~5,ua,iaaSn deduced L=l,4 spectroscopic strength functions,hole state fragmentation. High resolution spectrograph. REPT RCNP O s a k a , 1 9 8 1 A n n , P 6 1 , M a t o b a . NUCLEAR REACTIONS u s , n s , ~ e ° , l e e , ~ a 4 S n ( n , n ) , E = l - 3 0 O k e Y ; m e a s u r e d a(E). '~,~9,~a~,~za,~Z~Sn deduced s-,p-wave strength functions,radius parameters. REPT J I N R - P 3 - 8 2 - 4 3 6 , N i k o l e n k o . NUCLEAR REACTIONS ~ 4 , ' a ° T e ( a H e , a ) , E = 7 0 MeV; l a a , ' 2 4 , 1 a ° T e ( p , d ) , E = 4 0 MeV; m e a s u r e d a(O), a(Ea),a(Ed). 'e~,'za,~Te deduced levels,L,J,~,CeS. Enriched targets,magnetic spectrometer. DWBA a n a l y s i s , i n n e r shell excitation. REPT I P N 0 - D R E - 8 2 - 0 6 , G a l e s .

A ~24in

132

NUCLEAR REACTIONS l ' s C d ( l ° B , 4 n ) , E = 5 1 MeV; n S s n ( T L i , 3 n ) , E = 3 4 MeV; m e a s u r e d cr(ET),77(t), T(0). ~aal d e d u c e d levels,Jjr,transitions,band structure,E2 crossovers,configurations. B A P S A 27 7 2 8 , E C 1 9 , Q u a d e r . NUCLEAR REACTIONS l z ~ a 4 ~aa,iaOTe(a,4n),E=49.95 MeV; m e a s u r e d ~ , ( 0 ) , 7 7 - c o i n , E % I % laa,ia4, ~aa,la°Xe d e d u c e d l e v e l s , J , ~ . REPT INS T o k y o 1980 A n n , P 3 9 , K u s a k a r i . NUCLEAR REACTIONS l ~ , l z 4 , ~ T e ( a H e , 3 n ) , E = 2 0 - 2 7 MeV; m e a s u r e d ET,IT,~/(0),a(E'y),77-coin, I(ce),Tl/a. ~u,l~4,~°Xe deduced levels,J,rr,ICC,7-multipolarity,(~. REPT J Y F L R R - 6 / 8 2 , Hattula. NUCLEAR REACTIONS ~a~,l~4Te(a,4n),E n o t g i v e n ; m e a s u r e d 7 ( 0 ) , 7 - , n e u t r o n - m u l t i p l i c i t i e s . ~az, ~a4Xe d e d u c e d l e v e l s , J , T r , b a c k b e n d i n g , b a n d structure. B A P S A 27 5 1 7 , E X a S , S o f i a .

A laaSn

=

ONLY)

=

134

NUCLEAR REACTIONS 7°Zn,1°4Ru,n°pd,154Sm,lSs,la°Gd,la6w,19a,laSpt,2°a,a°4Hg,a44Pu(polarized t,a), 19apt,S44pu,7aGe(polarized t,p),E=17 MeV; sa,a°se,i°°Mo,12a,la4Sn(polarized t,aHe),E=32-25 MeV; measured (~(0),analyzing power vs 0,a(Ea),a(Ep),G(aHe). SgCu,'°3Tc,1°gRh,lSaPm,lS7,1SgEu, IaSTa,19s,1971r,a°i,a°aAu,24aNp,2°°pt,246pu,7SGe,S°,SaAs,l°°Nb,i22,1241n deduced mass excess. CONF Helsingor Voll P107, CERN 81-09. NUCLEAR REACTIONS 92,gs,SSMo,nS,'a4Sn(a,a),(a,a'),E=29.3,40,45,50 MeV; measured cr(E,0). 92 98,gaMo,116,124Sn deduced d e f o r m a t i o n p a r a m e t e r ft. Blair phase method. CONF Riga,P321, Ivanov. NUCLEAR REACTIONS 4 ° C a , 5 1 v , S S , 6 ° , S a N i , s S z n , g ° , 9 2 , 9 4 , 9 6 Z r , g a , 9 4 , 9 6 , g s , l ° ° M o , l a ° , l a 4 S n , 1 4 ° C e ( p , P ' ) , E = 2 0 1 MeV; m e a s u r e d a ( E p ' ) . 49Ca,51v,SS,6°,62Ni,6SZn,9°,ga,94,96Zr,92,94,96,gs,l°°Mo,'2°,t24Sn d e d u c e d M1 r e s o n a n c e , F . REPT IPN 1981 A n n u a l , P N 6 2 , D j a l a l i . NUCLEAR REACTIONS 9 ° , 9 2 , 9 4 Z r , n S , ' l s , l a 4 S n ( p , n ) , E = 7 9 . 2 MeV; m e a s u r e d (r(0). u s , u s , 1 2 4 S n deduced neutron to p r o t o n r m s r a d i u s r a t i o . DWBA a n a l y s i s . B A P S A 27 2 6 , D F 7 , L i n d . N U C L E A R - R E A C T I O N S 124Sn(n,n'7),E=2.6,3.4 MeV; m e a s u r e d a(ET),~(0). 124Sn l e v e l d e d u c e d J, 7r. B A P S A 37 716,CE7,Weil. NUCLEAR REACTIONS 124Sn(n,n'~,),E=2.3-3.5 MeV; m e a s u r e d E%I%7(0). l a 4 s n d e d u c e d l e v e l s . B A P S A 27 5 4 4 , G Y a 1 2 , W e i l . R A D I O A C T I V I T Y la4Sb,166mHo,lSaTa; m e a s u r e d E%relative IT. REPT N E A N D C ( J ) - 7 5 / U , P 2 1 , Yoshizawa. NUCLEAR REACTIONS la3Sb(n,~,),E=thermal; m e a s u r e d 77(t). ~4Sb levels d e d u c e d T 1 / a , h i n d r a n c e f a c t o r s . CONF R i g a , P 7 8 , G u s e v a . NUCLEAR REACTIONS ~aaSb(n,X),E < 4 keV; m e a s u r e d t r a n s m i s s i o n , l~4Sb r e s o n a n c e s d e d u c e d parameters. REPT N E A N D C ( J ) - 8 3 / U , P 1 7 , 0 h k u b o . NUCLEAR REACTIONS ~ z 4 , ~ 2 ~ , ~ z s , ~ a ° T e ( n , n ' ~ / ) , E = f a s t ; measured ~(0). ~4 l~,aas,~a°Te transitions d e d u c e d d. CONF R i g a , P 5 6 2 , D e m i d o v . NUCLEAR REACTIONS laa,124,1as,~a°Te(a,4n),E=49.95 MeV; m e a s u r e d ~/(0),~,7-coin,E%IT. labia4 128,13°Xe d e d u c e d l e v e l s , J , T r . REPT INS T o k y o 1980 A n n , P 3 9 , K u s a k a r i . NUCLEAR REACTIONS t z ~ , l ~ 4 , ~ a ~ T e ( 3 H e , 3 n ) , E = ~ 0 - 2 7 MeV; m e a s u r e d E%l~,,'~(0),a(ET),77-coin, l ( e e ) , T t / ~ , laa,l~4,~a~Xe d e d u c e d levels,J,Tr,ICC,~/-multipolarity,(~. REPT JYFL RR-6/82, Hattula. NUCLEAR REACTIONS ~ a ~ , ~ T e ( a , 4 n ) , E n o t g i v e n ; m e a s u r e d - ~ ( 0 ) , - ~ - , n e u t r o n - m u l t i p l i e i t i e s . ~aa l~4Xe d e d u c e d levels,Jjr,baekbending,band structure. B A P S A 27 5 1 7 , E X a S , S o f i a .

250

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A leSSn

R 79BaYJ: 82NiZX:

1~sSb

D 82YoZZ: R 81MaZF:

12STe

D 79MaYW:

J

81DuZX:

R

79DeYS 81DuZW

taSXe

D 800hZY

R 82HaZV

talCs

D 800hZY

R 82KuZT:

J

81DuZX:

R 79DeYS: 81DuZW:

!28 I

R 81PoZW:

*28Xe

D 800hZY:

R 80KuZR: 83AuZW:

12SCs

D 800hZY:

la8Ce

R

82CaZZ: 82WeZZ:

126

=

127

NUCLEAR REACTIONS 1271(p,n),E=10.5 MeV; 12s 12s,la0Te(c~,n),E=14.1_18 MeV; m e a s u r e d E%Iv, y ( O ) , T y - c o i n . ,27 ,e9 la, 133 Xe d e d u c e d l e v e l s , J , T r , q u a s i p a r t i c l e c h a r a c t e r . REPT JYFL 1981 Ann,P59,Kumpulainen.

A leSTe

=

NUCLEAR MOMENTS 126,128,13°Te; m e a s u r e d g. T h i n t r i p l e - f o i l technique,transient field m e t h o d . DABBB 42 1 9 3 1 , D u n h a m . NUCLEAR REACTIONS 124 126 l~s 1 3 0 T e ( n , n , T ) , E = f a s t ; m e a s u r e d 7(0). i24,'es,~es,1a°Te transitions d e d u c e d 6. CONF R i g a , P 5 6 2 , D e m i d o v . NUCLEAR REACTIONS l~,l~8,13OTe(35Cl,a5cr),E=70 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , a S C l y - c o i n , 7(0,H). ~ s , ~ s , 1 3 ° T e l e v e l d e d u c e d g. T r i p l e - f o i l transient f i e l d m e t h o d . BAPSA 26 1147, DDg,Dunham. RADIOACTIVITY l~6,1ZSCs [ f r o m l~s,l~SBa d e c a y ] ; m e a s u r e d I(ce). laSXe d e d u c e d n o s t r o n g E0 transition, leSXe d e d u c e d B ( E 0 ) / B ( E 2 ) . S i - L i d e t e c t o r , m a g n e t i c mini-orange filter,iron f r e e ~r s q u a r e - r o o t t w o fl s p e c t r o m e t e r . REPT INS T o k y o 1980 A n n , F 4 0 , O h y a . NUCLEAR REACTIONS l ~ , l a 4 , 1 a S T e ( a H e , 3 n ) , E = 2 0 - 2 7 MeV; m e a s u r e d Ey,Iv,y(0),c~(Ev),VT-coin, I(ce),Tl/2. l~,la4,~SXe deduced levels,J,~,ICC,v-multipolarity,6. REPT JYFL R R - 6 / 8 2 , Hattula. RADIOACTIVITY lzs,~SCs C f r o m ~as,leSBa d e c a y ] ; m e a s u r e d I(ce). l~SXe d e d u c e d n o s t r o n g E0 transition. 12SXe d e d u c e d B ( E 0 ) / B ( E 2 ) . S i - L i d e t e c t o r , m a g n e t i c mini-orange filter,iron f r e e ~r s q u a r e - r o o t t w o fl s p e c t r o m e t e r . REPT INS T o k y o 1980 A n n , P 4 0 , O h y a .

A 127Xe

125

NUCLEAR REACTIONS l ~ ° , 1 2 ~ , ~ 4 S n ( n , T ) , E = t h e r m a i ; m e a s u r e d E7,I7. t~l,laa,'e5Sn d e d u c e d transitions. CONF R i g a , P 7 6 , B a r e h u k . NUCLEAR REACTIONS l i s , l ' s , ~ e ° , l a ~ , l ~ 4 S n ( n , n ) , E = l - 2 0 0 keV; m e a s u r e d a(E). n v , n g , l a l , ~ a , ~ S S n deduced s-,p-wave strength functions,radius p a r a m e t e r s . REPT J I N R - P 3 - 8 2 - 4 3 6 , N i k o l e n k o . RADIOACTIVITY 7 5 S e ( E C ) , l e s S b ( f l - ) , ' a a B a ( E C ) , l S ° T b ( f l - ) , l S S T m ( E C ) ; m e a s u r e d Ev,relative IV. REPT N E A N D C ( J ) - 8 3 / U , P 9 , Y o s h i z a w a . NUCLEAR REACTIONS ~SSi,54Fe,S8Ni(aHe,aHe),(SHe,d),E=89.3 MeV; 9°Zr,l~4Sn(aHe,aHe),(aHe,d), E=89.8 MeV; m e a s u r e d a(0). ~gP,55Co,59Cu,9~Nb,~5Sb l e v e l s d e d u c e d C~S. F i n i t e - r a n g e DWBA analysis,nonlocal p o t e n t i a l s . REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 9 , M a t s u o k a . R A D I O A C T I V I T Y le5mTe; m e a s u r e d T~/a. CONF R i g a , P 7 9 , M a k a r y u n a s .

A l~6Te

=

ONLY)

=

128

NUCLEAR MOMENTS 126,128,13°Te; m e a s u r e d g. T h i n t r i p l e - f o i l technique,transient field m e t h o d . DABBB 42 1 9 3 1 , D u n h a m . NUCLEAR REACTIONS 1 2 4 , 1 a s , 1 2 8 , l a ° T e ( n , n ' T ) , E = f a s t ; measured 7(6). 124 12s,128,130Te transitions d e d u c e d 6. CONF R i g a , P 5 6 2 , D e m i d o v . NUCLEAR REACTIONS 126,~as,lS°Te(aSC1,3sCl'),E=70 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , a S c 1 7 - c o i n , V(O,H). 126,128,1a°Te l e v e l d e d u c e d g. T r i p l e - f o i l transient f i e l d m e t h o d . BAPSA 26 1147, DD9,Dunham. NUCLEAR REACTIONS 1 3 3 C s , 1 2 7 I ( n , y ) , ( n , X ) , E = 2 0 - 2 5 0 eV; m e a s u r e d transmission. 134Cs,128I deduced resonances,F%resonance parameters. REPT J I N R - P 3 - 8 1 7 2 1 , P o p o v . R A D I O A C T I V I T Y 12s,12SCs E f r o m la6,'2SBa d e c a y ] ; m e a s u r e d I(ce). 12SXe d e d u c e d n o s t r o n g E0 transition. 128Xe d e d u c e d B ( E 0 ) / B ( E 2 ) . S i - L i d e t e c t o r , m a g n e t i c mini-orange filter,iron free ~ square-root t w o fl s p e c t r o m e t e r . REPT INS T o k y o 1980 A n n , P 4 0 , O h y a . NUCLEAR REACTIONS lee,le4,1as,13°Te(a,4n),E=49.95 MeV; m e a s u r e d T ( 0 ) , V V - c o i n , E % I % ,e2 124 ~28,~a°Xe d e d u c e d levels,J,Tr. REPT INS T o k y o 1980 A n n , P 3 9 , K u s a k a r i . NUCLEAR REACTIONS 7SGe,S~Se,las,laOTe(p,n),E=135 MeV; m e a s u r e d cr(0),cr(En). 76As,eeBr d e d u c e d L=0 G a m o w - T e l l e r s t r e n g t h . 128,1a°Xe d e d u c e d t w o - f l p r o c e s s v i r t u a l s t a t e G a m o w - T e l l e r strength. BAPSA 27 7 3 1 , E E 7 , A u s t i n . R A D I O A C T I V I T Y 126,128Cs ] - f r o m 126,128Ba decayS; m e a s u r e d I(ee). 12SXe d e d u c e d n o s t r o n g E0 transition. 128Xe d e d u c e d B ( E 0 ) / B ( E 2 ) . S i - L i d e t e c t o r , m a g n e t i c mini-orange filter,iron f r e e ~r s q u a r e - r o o t t w o fl s p e c t r o m e t e r . REPT INS T o k y o 1980 A n n , P 4 0 , O h y a . NUCLEAR REACTIONS n2Cd(2°Ne,4n),E=103 MeV. leSCe d e d u c e d l e v e l s , J w , y r a s t , t w o - q u a s i p r o t o n b a n d s . C r a n k i n g s h e l l m o d e l . BAPSA 27 5 1 8 , E X a 5 , C a r v a l h o . NUCLEAR REACTIONS 9 2 Z r ( 4 ° A r , 4 n ) , E = 1 5 9 MeV; m e a s u r e d E T , I y , r e e o i l . leSCe d e d u c e d y r a s t s t a t e TW2. BAPSA 27 518,EXa6,Wells.

251

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A lagsn

D 82HuZX:

129Sb

D 82HuZX:

lagTe

D 82HuZX: R 82GaZZ:

lagXe

R 82KuZT:

:agCs

D 80AbZS:

l~gBa

D 80AbZS:

J

81DuZX:

R 79DeYS: 81DuZW:

~aOXe

R 80KuZR: 81LoZW:

82AuZW:

D 81ScZT:

82HuZY:

i31Sb

D 81ScZT:

82HuZY:

131Xe

R 82KuZT:

D 80KaZ0:

R 82KuZT:

=

131

=

132

R A D I O A C T I V I T Y lS2Sn [ f r o m f i s s i o n p r o d u c t s e p a r a t o r J ; m e a s u r e d 77(t). m2Sn d e d u c e d T1/2,J,~,configurations. RPA calculations. REPT J U L - S p e z - 7 2 , P 6 5 , K a w a d e .

A

133Xe

130

R A D I O A C T I V I T Y 131Sn [ f r o m f i s s i o n p r o d u c t m a s s s e p a r a t o r 3 ; m e a s u r e d E y , I % f l y - c o i n , y y ( t ) . i3:Sb d e d u c e d levels,Jjr,isomer Tl/2,y-branching. Shell model,level systematics. REPT J UL-Spez-99,P85,Schussler. R A D I O A C T I V I T Y l a i s n ; m e a s u r e d E y , I % y y - c o i n , T l / a . '31Sb d e d u c e d l e v e l s , 7 - b r a n c h i n g . REPT INDC(ARG)-9/G,Pb47,Huek. RADIOACTIVITY 'a'sn [from fission product mass separator3; measured Ey,Iy,f17-coin,yy(t). la'Sb deduced levels,J,yr,isomer T~/2,7-branching. Shell model,level systematics. REPT JUL-Spez-99,P65,Schussler. R A D I O A C T I V I T Y l a l s n ; m e a s u r e d E 7 , I y , 7 7 - c o i n , T i / e . lalSb d e d u c e d l e v e l s , y - b r a n c h i n g . REPT INDC(ARG)-9/G,Pb47,Huck. NUCLEAR REACTIONS 127I(p,n),E=10.5 MeV; 126,128,13°Te((~,n),E=14.1-18 MeV; m e a s u r e d E7,I7, 7(0),y7-coin. i27 ~20*3~ ~aa Xe d e d u c e d levels,J,~r,quasiparticle character. REPT JYFL 1981 Ann,P59,Kumpulainen.

A la2sn

=

NUCLEAR MOMENTS *26,*2s,ia°Te; m e a s u r e d g. T h i n t r i p l e - f o i l technique,transient field method. DABBB 42 1 9 3 1 , D u n h a m . NUCLEAR REACTIONS lz4 l e 6 , 1 2 8 , l a O T e ( n , n , y ) , E = f a s t ; measured y(0). la4 1z6 128,*aOTe transitions d e d u c e d 6. CONF R i g a , P 5 6 2 , D e m i d o v . NUCLEAR REACTIONS 126,ias,la°Te(aSCl,asCl'),E=70 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , a S C l y - c o i n , y(0,H). 126,1~8,'36Te l e v e l d e d u c e d g. T r i p l e - f o i l transient field method. B A P S A 26 1147, DDg,Dunham. NUCLEAR REACTIONS ~zz,~a4,:z8,ia°Te(a,4n),E=49.95 MeV; m e a s u r e d 7 ( 0 ) , y y - e o i n , E 7 , I y . ~zz,z4 le8,13°Xe d e d u c e d l e v e l s , J , ~ r . REPT INS T o k y o 1980 A n n , P a 9 , K u s a k a r i . NUCLEAR REACTIONS ~ 3 ° T e ( a , 4 n ) , E = 4 2 - 5 1 MeV; m e a s u r e d Ey,Iy,ff(Ey),y(0),yy-coin. la°xe deduced levels,J,~r,rotational bands,two-quasiparticle configurations. REPT JYFL R R - 1 5 / 8 1 , Lonnroth. NUCLEAR REACTIONS 76Ge,8ZSe,la8,*a°Te(p,n),E=135 MeV; m e a s u r e d a ( 0 ) , a ( E n ) . 7~As,SZBr d e d u c e d L=0 G a m o w - T e l l e r strength. *e8,~a°Xe d e d u c e d t w o - f l p r o c e s s v i r t u a l state Gamow-Teller strength. B A P S A 27 7 3 1 , E E 7 , A u s t i n .

A la:Sn

129

R A D I O A C T I V I T Y lagsn,12gmsb [ f r o m aa5U(n,F),E=thermal3; m e a s u r e d T l / e , f l - , 7 - d e c a y ; ' d e d u c e d Ifl, log f t . ~a9Sb,iagTe d e d u c e d l e v e l s , y - b r a n c h i n g . REPT I N D C ( A R G ) - 9 / G , P b 4 9 , H u c k . R A D I O A C T I V I T Y *agsn,~agmSb [ f r o m e a 5 u ( n , F ) , E = t h e r m a l ] ; m e a s u r e d T , / a , f l - , y - d e c a y ; d e d u c e d Ifl, log f t . lagSb,iagTe d e d u c e d l e v e l s , y - b r a n c h i n g . REPT I N D C ( A R G ) - 9 / G , P b 4 9 , H u c k . R A D I O A C T I V I T Y ~9Sn,mgmsb [ f r o m eaSU(n,F),E=thermal3; m e a s u r e d T i / ~ , f l - , 7 - d e c a y ; d e d u c e d Ifl, log f t . *agSb,laVTe d e d u c e d l e v e l s , y - b r a n c h i n g . REPT I N D C ( A R G ) - 9 / G , P b 4 9 , H u c k . NUCLEAR REACTIONS ~a4,*3°Te(aHe,a),E=70 MeV; ~aa la4,~a0Te(p,d),E=40 MeV; m e a s u r e d a(0), a(Ea),a(Ed), i~,~aa,~agTe deduced levels,L,J,vr,CaS. Enriched targets,magnetic spectrometer. DWBA a n a l y s i s , i n n e r shell excitation. REPT I P N O - D R E - 8 2 - 0 6 , G a l e s . NUCLEAR REACTIONS ~a~I(p,n),E=10.5 MeV; *a6,~as,~a°Te(a,n),E=14.1-18 MeV; m e a s u r e d Ey,Iy, 7(0),yy-coin. ~ 7 leg*a* ,33 Xe d e d u c e d levels,J,~r,quasiparticle character. REPT JYFL 1981 Ann,P59,Kumpulainen. R A D I O A C T I V I T Y lagBa [ f r o m La(aHe,xn3p)3; m e a s u r e d (ce)7(t). ieOCs l e v e l s d e d u c e d Tl/~. REPT IPN 1980 A n n u a l , P N 3 6 , A b r e u . R A D I O A C T I V I T Y laOBa [ f r o m La(aHe,xn3p)]; m e a s u r e d (ce)7(t). ~agCs l e v e l s d e d u c e d T~/e. REPT IPN 1980 A n n u a l , P N 3 6 , A b r e u .

A laOTe

=

ONLY)

NUCLEAR

REACTIONS

=

133

s2~I(p,n),E=10.5

7(O),77-eoin. 1 2 ~ l a g l a l saa Xe d e d u c e d Ann,P59,Kumpulainen.

252

levels,

MeV;

le°,128,sa°Te(~,n),E=t4.t-18

levels,Jjr,quasiparticle

MeV;

character.

measured

REPT J Y F L

E7,I7,

1981

SECONDARY

SOURCES

(Reports,Abstracts,e~c

A i~3Cs

D 79NyZZ:

~33Ba

D 79HaYC: 79NyZZ: 80AnZG: 83HaZJ: 82YoZZ:

~33La

D 79BuZW: 82MoZW:

133Ce

R

80MoZH:

D

79BuZW:

D 80KaZN:

134Cs

R 79StZL: 81PoZW: 82NaZQ:

134Ba

R 80MoZG: 82BeZY:

~a4La

D 81AbZV: 81MoZS:

la4Ce

D 81AbZV: 81MuZX:

82MuZZ:

D 81KaZX:

135La

D 79AbZU: 81BuZW:

laSCe

D 79AbZU: 81BuZW:

D 80KaZN:

=

134

=

135

RADIOACTIVITY laSTe E f r o m f i s s i o n p r o d u c t m a s s s e p a r a t o r ] ; m e a s u r e d ? ( X - r a y ) - , ~ / ~ - c o i n ; d e d u c e d l e v e l s , T i / m I C C , B ( E 2 ) , ? - b r a n c h i n g , J , r r , c o n f i g u r a t i o n . REPT J U L - S p e z - 9 9 , P 6 7 , K a w a d e . RADIOACTIVITY t35Ce; m e a s u r e d E%I(ce),7~/(0). laSLa l e v e l s d e d u c e d J , T r , ? - m u l t i p o l a r i t y , & Ge(Li),NaI(T1) d e t e c t o r s , s p e c t r o g r a p h . CONF R i g a , P 8 2 , A b d u r a z a k o v . RADIOACTIVITY 135Ce; m e a s u r e d "y'y(O). 135La l e v e l s d e d u c e d J,~r,~/-multipolarity,& Quasiparticle-phonon m o d e l . REPT J I N R - P 6 - 8 1 - - 5 6 5 , B u d z y n s k i . RADIOACTIVITY ~35Ce; m e a s u r e d E%I(ce),'yT(0). 135La l e v e l s d e d u c e d J , ~ r , ' y - m u l t i p o l a r i t y , & Ge(Li),NaI(T1) d e t e c t o r s , s p e c t r o g r a p h . CONF R i g a , P 8 2 , A b d u r a z a k o v . RADIOACTIVITY 135Ce; m e a s u r e d ?~/(0). 135La l e v e l s d e d u c e d J,~r,?-multipolarity,8. Quasiparticle-phonon m o d e l . REPT J I N R - P 6 - 8 1 - 5 6 5 , B u d z y n s k i .

A 136Xe

continued

RADIOACTIVITY 134Te,~3aXe [ f r o m f i s s i o n p r o d u c t s e p a r a t o r ] ; m e a s u r e d ? ? ( t ) . ~34Te,~3SXe l e v e l s d e d u c e d TI/z,B(ES). REPT J U L - S p e z - 7 3 , P 6 7 , K a w a d e . NUCLEAR REACTIONS 133Cs(n,7),E n o t g i v e n ; m e a s u r e d E ' y , l % ~ / - / - c o i n . 134Cs d e d u c e d t r a n s i t i o n s . Ge(Li),NaI(T1) d e t e c t o r s . CONF R i g a , P 6 0 5 , S t o y a n o v i c h . NUCLEAR REACTIONS 133Cs,iZTI(n,~/),(n,X),E=30-250 eV; m e a s u r e d t r a n s m i s s i o n . 134Cs,lesI d e d u c e d r e s o n a n c e s , F % r e s o n a n c e p a r a m e t e r s . REPT J I N R - P 3 - 8 1 - 7 2 1 , P o p o v . NUCLEAR REACTIONS '33Cs(n,X),E < 5.8 keV; ~33Cs(n,'y),E < 2 keV; m e a s u r e d or. 134Cs r e s o n a n c e s d e d u c e d F n , F ? . REPT N E A N D C ( J ) - 8 3 / U , P I 7 , N a k a j i m a . NUCLEAR REACTIONS 133Cs(a,Snp),E=55 MeV; 134Ba(p,p'),E=17 MeV; m e a s u r e d n o t g i v e n . 134Ba deduced levels,Jjr,-/-branching,configurations. REPT J U L - S p e z - 7 2 , P 4 4 , M o r e k . NUCLEAR REACTIONS le4Sn(laC,3n),E=48 MeV; m e a s u r e d 7(t),~/(0,H,t). 134Ba level d e d u c e d TI/2, g , c o n f i g u r a t i o n . BAPSA 27 27,DF10,Bell. RADIOACTIVITY 13e,136Nd,la4Ce; m e a s u r e d E%I~/,l(ce),(ce)~/-coin; d e d u c e d log f t . 134La,138, 136pr d e d u c e d l e v e l s , I C C , - y - m u l t i p o l a r i t y , ? - b r a n c h i n g . REPT J I N R - P S - 8 1 - 4 8 9 , A b d u m a l i k o v . RADIOACTIVITY '34La [ f r o m 136Ba(p,3n),E=30 MeVJ; m e a s u r e d E%~/~/(t),'yT-coin; d e d u c e d levels, isomer T1/zj/-branching. REPT J U L - S p e z - 9 9 , P 4 7 , M o r e k . RADIOACTIVITY '3a,136Nd,134Ce; m e a s u r e d E T , I % I ( c e ) , ( c e ) ? - c o i n ; d e d u c e d log f t . 13~La,13a, laSPr d e d u c e d l e v e l s , I C C , ? - m u l t i p o l a r i t y , ~ / - b r a n c h i n g . REPT J I N R - P S - 8 1 - ¢ 8 9 , A b d u m a l i k o v . RADIOACTIVITY 134Ce [ f r o m 134Ba(a,4n),E=60 MeVJ; m e a s u r e d ET,IT,I(ce),~/?(t); d e d u c e d levels,J,rr,quasigamma bands,side feeding characterJstics,~/-multipolarity,B(ES), configuration. REPT J U L - S p e z - 9 9 , P 4 9 , M u l l e r - V e g g i a n . RADIOACTIVITY ~a~Ce [ f r o m ~3~Ba(a,4n),E=60 MeVJ; d e d u c e d l e v e l s , J , r r F / - b r a n c h i n g , i s o m e r configuration,band structure. In-beam spectroscopy. REPT J U L - S p e z - 1 4 6 , P 5 2 , Muller-Veggian.

A 135Te

133

RADIOACTIVITY 133Ba; m e a s u r e d ce~(t), laaCs level d e d u c e d T~/a. REPT NEANDC(E)-20RU,Vol III, P31,Nylandsled-Larsen. RADIOACTIVITY ~3Ba; m e a s u r e d T1/2. REPT NEANDC(E)-202U,Vol l l I , P 2 8 , H a n s e n . RADIOACTIVITY ~33Ba; m e a s u r e d ceT(t). 13aCs level d e d u c e d Tl/a. REPT NEANDC(E)-R02U,Vol Ill, P31,Nylandsled-Larsen. RADIOACTIVITY '3aBa [ f r o m Cs(p,n)J; m e a s u r e d E%I%isomer T~/z. REPT INS Tokyo 1980 A n n , P41,Ando. RADIOACTIVITY ~a3Ba; m e a s u r e d I(ce). REPT NEANDC(E)-332U,Vol I I 1 , P 4 9 , H a n s e n . RADIOACTIVITY 75Se(EC),tesSb(fl-),la3Ba(EC),lS°Tb(fl-),lSSTm(EC); m e a s u r e d E T , r e l a t i v e I% REPT N E A N D C ( J ) - 8 3 / U , P 9 , Y o s h i z a w a . RADIOACTIVITY 13aCe [ f r o m Cd(p,X),E=660 MeVJ; m e a s u r e d ~/~/(O,H); d e d u c e d Az. ~33La levels d e d u c e d J,6,g,/z. CONF R i g a , P 8 1 , B u d z y n s k i . RADIOACTIVITY ~aaLa [ f r o m t 3 3 C s ( a , 4 n ) , E = 5 5 MeVJ; d e d u c e d l e v e l s , J , ~ r , c o n f i g u r a t i o n , ~/-branching,band structure. I n - b e a m s p e c t r o s c o p y . REPT J U L - S p e z - 1 4 6 , P S 1 , M o r e k . NUCLEAR REACTIONS ~33Cs(a,4n),E=55 MeV; m e a s u r e d -~/-coin,-/(O). laaLa d e d u c e d levels,J,?r, band structure,~/-branching,configuration. REPT J U L - S p e z - 7 2 , P 4 4 , M o r e k . RADIOACTIVITY laaCe [ f r o m Cd(p,X),E=660 MeVJ; m e a s u r e d ?3~(0,H); d e d u c e d Az. ~33La levels d e d u c e d J,6,g,/~. CONF R i g a , P 8 1 , B u d z y n s k i .

A la4Te

=

ONLY)

=

136

RADIOACTIVITY 134Te,13SXe [ f r o m f i s s i o n p r o d u c t s e p a r a t o r ] ; l e v e l s d e d u c e d T1/z,B(E2). REPT J U L - S p e z - 7 2 , P 6 7 , K a w a d e .

253

measured

??(t).

134Te,136Xe

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 13aLa

D 81MoZR:

lSapr

D 81AbZV:

*3aNd

D 81AbZV:

D 81ArZW:

R 82KiZV: *3~'Ce

D 81ArZW:

R 82KoZY:

R 82PrZX:

*Sepr

D 81AbZV:

*SaNd

D 81AbZV: R 80MuZU:

D 81ArZW:

13apr

D 81ArZW:

R 80BaZI: 139Nd

R 80MuZU:

R 81BeYU:

137

=

138

=

139

R A D I O A C T I V I T Y 137Ce,lagPr; m e a s u r e d E%lT,I(ce),Efl+,(ce)7-,-yT-coin; deduced fl-endpoint e n e r g y . 137La d e d u c e d levels,Tl/a,-y-branehing. 139Ce d e d u c e d levels,-y-branching. REPT JINR-P6-81-524,Artamonova. R A D I O A C T I V I T Y 137Ce,139pr; m e a s u r e d E,y,I-y,I(ce),Efl+,(ce)7-,-y,y-coin; deduced fl-endpoint e n e r g y . 137La d e d u c e d levels,Tl/2,-y-branching. 139Ce d e d u c e d levels,-y-branching. REPT JINR-P6-81-524,Artamonova. NUCLEAR REACTIONS t 2 a T e ( 1 4 N , 3 n ) , E = 6 0 MeV. 139Pr d e d u c e d levels,J,~,-y-branching. 7-spectroscopic techniques. REPT ISN 8 0 - 0 1 , P 3 2 , B a r c i . NUCLEAR REACTIONS 1 4 ° C e ( a , x n ) , E = 8 5 MeV; m e a s u r e d n o t g i v e n , lSSNd d e d u c e d levels,J,~r, rotational bands,configurations. ~39Nd d e d u c e d levels,J,~r,ground state band, configuration. Weak-coupling,triaxial rotor-plus-particle m o d e l s . REPT J U L - S p e z - 7 2 , P 4 5 , Muller-Veggian.

A 140pm

=

NUCLEAR REACTIONS 13aXe(a,2n),E n o t g i v e n ; m e a s u r e d E,y,I,y,,y,y-coin,,yT(t),,y(O),cr(ET),DSA. ~SaBa d e d u c e d l e v e l s , r r , i s o m e r T 1 / a , , y - m u l t i p o l a r i t y , c o n f i g u r a t i o n . CONF Y a m a n a s h i ( D y n a m i c s Nucl.Collective Motion) Contrib,P34. R A D I O A C T I V I T Y iss,*3aNd,134Ce; m e a s u r e d E T , I , y , I ( c e ) , ( c e ) , y - c o i n ; d e d u c e d log f t . *S4La,*Ss, *3Spr d e d u c e d l e v e l s , I C C , , y - m u l t i p o l a r i t y , , y - b r a n c h i n g . REPT J I N R - P 6 - 8 1 - 4 8 9 , A b d u m a l i k o v . R A D I O A C T I V I T Y 13e,iSaNd,iS4Ce; m e a s u r e d E,y,I,y,l(ce),(ce)7-coin; deduced log f t . *34La,*Sa, *3SPr d e d u c e d l e v e l s , I C C , 7 - m u l t i p o l a r i t y , , y - b r a n c h i n g . REPT J I N R - P a - 8 1 - 4 8 9 , A b d u m a l i k o v . NUCLEAR REACTIONS * 4 ° C e ( a , x n ) , E = 8 5 MeV; m e a s u r e d n o t g i v e n . 13aNd d e d u c e d levels,J,Tr, rotational bands,configurations. 139Nd d e d u c e d levels,J,~r,ground state band, configuration. Weak-coupling,triaxiat rotor-plus-particle m o d e l s . REPT J U L - S p e z - 7 2 , P 4 5 , Muller-Veggian.

A 13SCe

continued

R A D I O A C T I V I T Y *STCe,lSgpr; m e a s u r e d E-y,I,y,I(ce),Efl+,(ce)-y-,7-y-coin; deduced fl-endpoint e n e r g y , i37La d e d u c e d levels,Ti/2,-y-branching. *39Ce d e d u c e d levels,77-branching. REPT JINR-P6-81-524,Artamonova. NUCLEAR REACTIONS 13OTe(nB,4n),E=45 MeV; m e a s u r e d 77-y-coin,a(E,y),,y(0,H,t). 13VLa d e d u c e d i s o m e r T1/2,g. B A P S A 27 7 2 8 , E C l l , K i s t n e r . R A D I O A C T I V I T Y *37Ce,*39pr; m e a s u r e d E-y,I%I(ce),Efl+,(ce)'),-,-yT-coin; deduced fl-endpoint e n e r g y , lSVLa d e d u c e d levels,T1/2,,y-branching. 139Ce d e d u c e d levels,77-branching. REPT JINR-P6-81-524,Artamonova. NUCLEAR REACTIONS 1 S T B a ( S H e , 3 n ) , E = 2 4 - 2 7 MeV; m e a s u r e d 77(0),,y,y-coin,a(E-y),I(ce). 13~Ce deduced levels,J,~v,,y-branching,7-multipolarity. REPT J Y F L 1981 A n n , P 6 4 , K o r t e l a h t i .

A 13aBa

136

R A D I O A C T I V I T Y *3gLa [ f r o m iSSBa(p,3n)]; measured E77,77,y(t),,y,y-coin,,y(O); d e d u c e d l e v e l s , isomer T,/z,-y-branching,configuration. REPT J U L - S p e z - 9 9 , P 4 8 , M o r e k . R A D I O A C T I V I T Y *3a,13aNd,*S4Ce; m e a s u r e d ET,I,y,I(ce),(ce),y-coin; deduced log f t . '34La,138, 13Spr d e d u c e d l e v e l s , I C C , 7 - m u l t i p o l a r i t y , , y - b r a n c h i n g . REPT J I N R - P 6 - 8 1 - 4 8 9 , A b d u m a l i k o v . R A D I O A C T I V I T Y *as,136Nd,134Ce; m e a s u r e d E , y , I - y , l ( c e ) , ( c e ) , y - c o i n ; d e d u c e d log f t . iS4La,i3a, *38pr d e d u c e d l e v e l s , I C C , 7 7 - m u l t i p o l a r i t y , v - b r a n c h i n g . REPT J I N R - P 6 - 8 1 - 4 8 9 , A b d u m a l i k o v .

A 137La

=

ONLY)

=

140

NUCLEAR REACTIONS laaTe(19F,5n),E=80-1O0 MeV; m e a s u r e d ,y-y(t),-y(0),-y-y(0),oriented n u c l e i . levels,J,~r,configuration. REPT IPN 1981 A n n u a l , P N 5 3 , B e c k .

14°pm d e d u c e d

A 141Cs

D 82YaZY:

~4iBa

D 82YaZY:

=

141

R A D I O A C T I V I T Y 141Cs [ f r o m m a s s s e p a r a t o r ] ; zr. B A P S A 27 5 1 8 , E X a 7 , Y a m a m o t o . R A D I O A C T I V I T Y 141Cs [ f r o m m a s s s e p a r a t o r ] ; ~r. B A P S A 27 5 1 8 , E X a 7 , Y a m a m o t o .

254

measured

y-decay,X-rays.

*41Ba d e d u c e d level,J,

measured

7-decay,X-rays.

i41Ba d e d u c e d

level,J,

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 14~pr

R 80KoZM:

D 82ChZW:

i42La

D 81MiZU:

82ChZW: 82ShZZ: 82WoZY: t~Ce

D 81MiZU:

82ShZZ: 82WoZY:

D 79WaZU

143Nd

R 82WrZY

143pro

R 79ZaZY 80StZM

82BoZV

14aSm

D 80AbZR:

D 79WaZU:

1~4Ba

D 8iChZ0: 82ChZW:

144La

D 81ChZ0: 81MiZU:

81WaZO: 8~ChZW: 82WaZY:

=

ET,IT,77(0),77-coin,I(ce). ~4tPr REPT J Y F L 1980 A n n , P 5 5 ,

14~

=

143

R A D I O A C T I V I T Y 94,gSRb,t43,144Cs [ f r o m on-line separation]; measured E7,I7; d e d u c e d fl-delayed neutron emission probability. CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products), P311,Warner. NUCLEAR REACTIONS 1 4 5 N d ( p , t ) , E = 2 5 MeV; m e a s u r e d cr(O),a(Et). 143Nd l e v e l s d e d u c e d L. Multi-wire proportional counter,high resolution spectrometer. REPT J U L - S p e z - 1 4 6 , P 6 , Wrzesinski. NUCLEAR REACTIONS 141Pr(a,2nT),E n o t g i v e n ; m e a s u r e d 7(8,H). 143pm l e v e l s d e d u c e d g. CONF Riga,PZ45,Zaly ubovskij. NUCLEAR REACTIONS 9 ° Z r , t 4 4 S m ( p o l a r i z e d d,3He),E=52 MeV; m e a s u r e d a(E(SHe)),a(O),iTtl(O); deduced spin-orbit splitting. SSy,t43Pm deduced hole-state dominance. Zero-range DWBA. REPT K f K - 3 0 6 8 , P 2 7 , S t u i r b r i n k . NUCLEAR REACTIONS ~4aNd(160,t°N),(tso,17N),E=120 MeV; t42Nd(12C,IIB),(t3C,t2B),E=90 MeV; measured a(E(15N)),a(E(*TN)),a(E(llB)),o'(E(~eB)). *43Pro d e d u c e d high-spin proton state population. B A P S A 27 7 0 7 , B D g , B o n d . R A D I O A C T I V I T Y 1~3Sm; m e a s u r e d 7 ( c e ) ( t ) . t 4 3 S m l e v e l d e d u c e d T~/s,B(),),8. I n t e r m e d i a t e coupling model,N=81 systematics. REPT IPN 1980 A n n u a l , P N 3 6 , A b r e u .

A t44Cs

continued

R A D I O A C T I V I T Y 142,144Ba [ f r o m on-line separation]; measured 77(0),77-coin. ~4a,*44La deduced l e v e l s , J , r t , I f l . B A P S A 27 5 1 8 , E X a l 0 , C h u n g . R A D I O A C T I V I T Y t4~,'4~La [ f r o m o n - l i n e s e p a r a t i o n ] ; m e a s u r e d ET,I%77(0),oriented nuclei; ta4La d e d u c e d Qfl. 14z,~4Ce d e d u c e d l e v e l s , J , ~ r , 7 - b r a n c h i n g . CONF H e l s i n g o r Vo12 P581, CERN 81-09. R A D I O A C T I V I T Y *4a,l~4Ba [ f r o m on-line separation]; measured 77(0),77-coin. 14a,~44La deduced l e v e l s , J , T r , I f l . B A P S A 27 5 1 8 , E X a l 0 , C h u n g . R A D I O A C T I V I T Y t4ULa; m e a s u r e d 77(0). 14ZCe l e v e l d e d u c e d J,Tr. BAPSA 27 5 1 8 , E X a 9 , S h m i d . R A D I O A C T I V I T Y ~2,t~s,taaCe,~au,~aULa; m e a s u r e d -/7(0). F i x e d a n g l e f o u r d e t e c t o r s y s t e m . B A P S A 27 5 2 1 , E X b 1 5 , W o l f . R A D I O A C T I V I T Y t4z,t44La [ f r o m o n - l i n e s e p a r a t i o n S ; m e a s u r e d ET,IT,77(0),oriented nuclei; 144La d e d u c e d Qfl. t~a,~aaCe d e d u c e d l e v e l s , J , r r , 7 - b r a n c h i n g . CONF H e l s i n g o r Vol2 P581, CERN 81-09. R A D I O A C T I V I T Y laSLa; m e a s u r e d 77(0). 14ZCe l e v e l d e d u c e d J,rr. BAPSA 27 5 1 8 , E X a 9 , S h m i d . R A D I O A C T I V I T Y t4a,t~s,taSCe,~a~,t4SLa; m e a s u r e d 7T(0). Fixed angle four detector system. B A P S A ~7 5 2 1 , E X b l S , W o l f .

A ~43Cs

141

NUCLEAR REACTIONS ~4aCe(p,Sn),E n o t g i v e n ; m e a s u r e d deduced levels,J,vr,7-branching,7-multipolarity,configuration. Kortelahti.

A ~4ZBa

=

ONLY)

=

144

R A D I O A C T I V I T Y s4,geRb,143,144Cs [ f r o m on-line separation]; measured E7,17; d e d u c e d fl-delayed neutron emission probability. CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n Products), P31l,Warner. R A D I O A C T I V I T Y 144Ba [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) . t44La d e d u c e d l e v e l s . B A P S A 26 l 1 4 7 , D D l l , C h u n g . R A D I O A C T I V I T Y 142,144Ba [ f r o m on-line separation]; measured 77(0),77-coin. 142,~"4La deduced l e v e l s , J , r r , I f l . B A P S A 27 5 1 8 , E X a l 0 , C h u n g . R A D I O A C T I V I T Y 144Ba [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) . ~44La d e d u c e d l e v e l s . B A P S A 26 l 1 4 7 , D D l l , C h u n g . R A D I O A C T I V I T Y 14a,i44La [ f r o m o n - l i n e s e p a r a t i o n ] ; m e a s u r e d E7,I7,~7(0),oriented nuclei; ~44La d e d u c e d Qfl. t42,t44Ce d e d u c e d l e v e l s , J , ? r , 7 - b r a n c h i n g . CONF H e l s i n g o r Vol2 P581, CERN 81-09. R A D I O A C T I V I T Y 144La; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) . t44Ce d e d u c e d l e v e l s , J j r . BAPSA 26 1147,DD12, Waiters. R A D I O A C T I V I T Y i42,144Ba [ f r o m on-line separation]; measured 77(0),77-coin. 142,144La deduced l e v e l s , J , T r , l f l . B A P S A 27 5 1 8 , E X a l 0 , C h u n g . R A D I O A C T I V I T Y t44La; m e a s u r e d 77(0),fl-decay. t¢4Ce d e d u c e d levels,Jjr,quasiparticle character. B A P S A 27 5 1 8 , E X a l l , W a l t e r s .

255

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A =

1440e

D 81MiZU

81WaZ0 82WaZY 144Nd

R 82QuZZ

144Sm

R 80LeZK

144Eu

R

144Gd

R 82SmZX

~44Tb

D 81NoZY:

80HaZB

D 82DeZX:

145Ba

D 82ChZV: 82DeZX:

t45La

D 82BrZX:

'~SNd

82ChZV: R 80HaYZ:

~45Sm

D 81DeZM:

81ScZR: 145Eu

D 81DeZM:

R 81GaZT: 82DaZT: 82GaZU:

145Gd

D 80PaZK: 81StZ0:

82StZU:

14~Tb

D 81AIZ0:

continued

RADIOACTIVITY 14e,144La [ f r o m o n - l i n e s e p a r a t i o n 3 ; m e a s u r e d E-f,l-f,-f-f(O),oriented n u c l e i ; ~44La d e d u c e d Qfl. *~z,i4~Ce d e d u c e d l e v e l s , J , ~ r , - f - b r a n c h i n g . CONF H e l s i n g o r Vo12 P581, CERN 81-09. RADIOACTIVITY 144La; m e a s u r e d -f-f-coin,-f(0). 144Ce d e d u c e d levels,J,Tr. BAPSA 26 1147,DD12, Walters. RADIOACTIVITY t44La; m e a s u r e d -f-f(O),fl-decay. t4¢Ce deduced l e v e l s , J , ~ r , q u a s i p a r t i e l e c h a r a c t e r . BAPSA 27 518,EXa11,Walters. NUCLEAR REACTIONS t3°Te(tao,4n),E=70 MeV; m e a s u r e d E-f,I-f,-f(0),-f-f(t). l~4Nd d e d u c e d levels, band strueture,7-multipolarity. BAPSA 27 519,EXat6,Quader. NUCLEAR REACTIONS e°Ni,9°Zr,t~SIn,t2°Sn,~44Sm,~e5Ho,teTAu,~°spb(aHe aHe'),E=108.5 MeV; m e a s u r e d cr(E(aHe)),~r(0), 6°Ni d e d u c e d GQR,F. aezr,nSln,~Z°Sn,t44Sm,~SSHo,t97Au d e d u c e d GQR, g i a n t m o n o p o l e r e s o n a n c e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS ~47Sm(p,4n),E=40 MeV; m e a s u r e d E-f,I-f,I(ce). ~44Eu d e d u c e d levels,J,~, - f - b r a n c h i n g , T l / z , c o n f i g u r a t i o n s . I r o n - f r e e o r a n g e t y p e f l - s p e c t r o m e t e r . REPT J U L - S p e z - 7 2 , P48,Haenni. NUCLEAR REACTIONS ~07Ag(aTCl,X),E=130-215 MeV; m e a s u r e d -/-multiplicity; deduced m u l t i p l i c i t y m o m e n t s . *44Gd d e d u c e d s p i n d i s t r i b u t i o n c u t o f f c h a r a c t e r i s t i c s . BAPSA 27 707,BD8,Smith. RADIOACTIVITY ~Smpd [ f r o m SaNi(4°Ca,n8p),E=133-173 MeV]; m e a s u r e d fl-delayed Ep,lp, f l - d e l a y e d pT(t); d e d u c e d log f t . aSRh,sgRu l e v e l s d e d u c e d - f - b r a n c h i n g . t4SDy [ f r o m 9°Zr(SSNi,2p)3; ~SeEr [ f r o m a¢Mo(SSNi,2p),gZMo(S°Ni,2p)]; m e a s u r e d ~(E7),-fT-coin,-f-f(t),DSA, fl-delayed p-f(t). ~4SDy,tSOEr d e d u c e d levels,J,rr, te°Tm,t¢4Tb,t~SHo,t4SEr; m e a s u r e d f l - d e c a y . CONF H e l s i n g o r Voll P253, CERN 81-09.

A

t~SCs

144

ONLY)

=

145

RADIOACTIVITY 14SCs [ f r o m m a s s s e p a r a t o r ] ; m e a s u r e d ET,IT,77-coin; d e d u c e d T1/2. 14SBa d e d u c e d l e v e l s . BAPSA 27 5 1 9 , E X a l 2 , D e j b a k h s h . RADIOACTIVITY 14SBa; m e a s u r e d E7,IT,77-coin. t45La deduced levels. BAPSA 27 519,EXal3,Chu. RADIOACTIVITY i4SCs [ f r o m m a s s s e p a r a t o r S ; m e a s u r e d ET,I?,77-coin; d e d u c e d T1/2. t45Ba d e d u c e d l e v e l s . BAPSA 27 5 1 9 , E X a l 2 , D e j b a k h s h . RADIOACTIVITY 14s,t46,t4SLa [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d f l - e n d p o i n t energies; d e d u c e d qfl. H y p e r p u r e Ge f l - s p e c t r o m e t e r . BAPSA 27 5 1 9 , E X a l 4 , B r e n n e r . RADIOACTIVITY J~SBa; m e a s u r e d ET,17,77-coin. '~SLa deduced levels. BAPSA 27 519,EXal3,Chu. NUCLEAR REACTIONS m6Xe(13C,xn),E=52,60 MeV; m e a s u r e d a(E7),7(0),T7-coin, t45,i46Nd deduced l e v e l s , J , ~ , T - b r a n c h i n g . REPT JYFL 1980 A n n , P 6 0 , H a m m a r e n . RADIOACTIVITY i45Eu; m e a s u r e d 7(0),oriented n u c l e i . 14SSm d e d u c e d l e v e l s , J , ~ , ( ~ . Implantation in Fe,low temperatures. Quasiparticle plus phonon m o d e l . REPT JI N R - P 6 - 8 1 - 5 6 0 , D e r y u g a . RADIOACTIVITY 14s,t47Gd,t47Eu,'45Sm,'4aDy,14a,'4~Tb; m e a s u r e d f l + / E C , K - e a p t u r e p r o b a b i l i t y ; d e d u c e d Q(EC). 14e,t47Gd,t47Eu,t4SDy,147Tb d e d u c e d m a s s e s . CONF H e l s i n g o r Voll P148, CERN 81-09. RADIOACTIVITY 145Eu; m e a s u r e d 7(0),oriented n u c l e i . 14SSm d e d u c e d l e v e l s , J , ~ , 6 . Implantation in Fe,low temperatures. Quasiparticle plus phonon m o d e l . REPT JI N R - P 6 - 8 1 - 5 6 0 , D e r y u g a . NUCLEAR REACTIONS 144Sm,Z°sPb(a,t),E=80 MeV; m e a s u r e d a(Et). 14SEu deduced levels. REPT IPN 1981 A n n u a l , P N 6 9 , G a l e s . NUCLEAR REACTIONS '44Sm(t,2n),E=17 MeV; m e a s u r e d 7 7 - c o i n , 7 7 ( t ) . '4SEu d e d u c e d levels. BAPSA 27 675,GYc3,Dave. NUCLEAR REACTIONS l~Sm(a,t),E=80 MeV; '44Sm(3He,t),E=240 MeV; m e a s u r e d a(Et),a(O). 145Eu d e d u c e d levels,L,J,Tr,F,C2S,proton s t r e n g t h . REPT I P N O - D R E - 8 2 - 1 6 , G a l e s . RADIOACTIVITY t45Gd [ f r o m i44Sm(aHe,2n)3; m e a s u r e d ET,17,a(E-f),7(0),77-coin,I(ce); d e d u c e d levels,J,zr,ICC,T1/2,7-multipolarity,7-branching. REPT JYFL 1980 A n n , P 5 7 , P a k k a n e n . RADIOACTIVITY 145,t47,14eTb [ f r o m tSiEu(a,n),t52Gd(t~,xnp),E=90-130 MeV]; m e a s u r e d E7,1")',')'7-, - f ( X - r a y ) - c o i n f o l l o w i n g f l - d e c a y ; d e d u c e d N=82 s i n g l e p a r t i c l e e n e r g y gap. la6Tb d e d u c e d Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . 145Tb d e d u c e d TI/2,Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . 147,146,145Gd d e d u c e d l e v e l s , - f - b r a n e h i n g , c o n f i g u r a t i o n . CONF H e l s i n g o r Vol2 P548, CERN 81-09. RADIOACTIVITY 145,14a,147Tb [ f r o m ia2Gd,tStEu(a,xnyp),E=90,130 MeV]; m e a s u r e d E-f,17,7T-coin f o l l o w i n g f l - d e c a y . 14STb d e d u c e d Q(EC),T1/2, 14aTb level deduced J,Tr. J46Gd d e d u c e d levels, J,~,7-branching. 14s,147Gd d e d u c e d levels,J,~r,7-branching,-f-multipolarity. REPT JUL-Spez-146,P56,Styczen. RADIOACTIVITY t45Tb(EC),(lI+),t46Dy(EC),(fl +) [ f r o m o n - l i n e s e p a r a t i o n ] ; m e a s u r e d E-f,17, E ( X - r a y ) , I ( X - r a y ) , T l / 2 . CONF S a m a r k a n d , P 9 7 , A l k h a z o v .

256

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

145Tb

D 81StZ0:

83StZU:

D 83ChZR:

146La

D 82BrZX: 8~ChZR:

82WoZY: i4SCe

D 82WoZY:

14SNd

R

80HaYZ: 81AnZU:

i46Sm

D 8~RoZZ:

~46Eu

D 80AdZX: R 80ErZW:

t46Gd

D 81ScZR:

81StZ0:

R 80BrZQ:

81WiZL:

~46Tb

D 81StZ0:

82StZU:

146Dy

D

81AIZ0:

continued

=

!46

RADIOACTIVITY 146Ba(fl-); m e a s u r e d E7,IT,77(t),77(0),7(t); d e d u c e d TI/2. 148La d e d u c e d levels,J,Tr. BAPSA 27 728,EC12,Chung. RADIOACTIVITY 145t46,14aLa [ f r o m o n - l i n e m a s s separation3; m e a s u r e d f l - e n d p o i n t energies; d e d u c e d Qfl. H y p e r p u r e Ge f l - s p e c t r o m e t e r . BAPSA 27 5 1 9 , E X a 1 4 , B r e n n e r . RADIOACTIVITY 146Ba(fl-); m e a s u r e d ET,IT,77(t),77(0),7(t); d e d u c e d TI/2. 146La d e d u c e d l e v e l s , J , w . BAPSA 27 738,EC1E,Chung. RADIOACTIVITY 142,148,148Ce,14a,14SLa; m e a s u r e d 77(0). F i x e d a n g l e f o u r d e t e c t o r s y s t e m . BAPSA 27 521,EXb15,Wolf. RADIOACTIVITY 142,146,148Ce,142,146La; m e a s u r e d 77(0). F i x e d a n g l e f o u r d e t e c t o r s y s t e m . BAPSA 27 521,EXb15,Wolf. NUCLEAR REACTIONS 136Xe(lac,xn),E=52,60 MeV; m e a s u r e d ff(ET),7(O),77-coin. 145,146Nd deduced levels,J,rr,7-branching. REPT JYFL 1980 A n n , P S 0 , H a m m a r e n . NUCLEAR REACTIONS 77Se(n,a),E=l12-1265 eV; 145Nd(n,a),E=4.35-306 eV; m e a s u r e d cr(Ec~), t i m e - s p e c t r a . 78Se d e d u c e d r e s o n a n c e s , F a . 14~Nd d e d u c e d r e s o n a n c e s . REPT J I N R - P 3 - 8 1 - 3 4 8 , Antonov. RADIOACTIVITY 146Sm [ f r o m i2SLa(nB,4n)]; 147Eu [ f r o m laSLa(laC,4n)]; m e a s u r e d recoil. 14%m, 147Eu l e v e l s d e d u c e d T1/2. I n t e r a c t i n g boson,cluster vibrator,core-particle coupling m o d e l s . DABBB 42 2888,Rozak. RADIOACTIVITY 146Eu(B +) [ f r o m 146Gd d e c a y ] ; m e a s u r e d E%I% C0NF L e n i n g r a d , P 9 9 , A d a m . NUCLEAR REACTIONS 147Sm(p,2n),E=19-23 MeV; m e a s u r e d I(ce),77-coin,IT. t46Eu deduced levels, T1/z,J,rr,7-multipolarity,configurations. E n r i c h e d m e t a l t a r g e t . REPT J U L - S p e z - 7 2 , P 5 6 , Ercan. RADIOACTIVITY 146,147Gd,147Eu,145Sm,148Dy,i4s,147Tb; m e a s u r e d B + / E C , K - c a p t u r e p r o b a b i l i t y ; d e d u c e d Q(EC). 146,147Gd,147Eu,t48Dy,147Tb d e d u c e d m a s s e s . CONF H e l s i n g o r Voll P148, CERN 81-09. RADIOACTIVITY 145147,146Tb [ f r o m *51Eu(a,n),lSeGd(c~,xnp),E=90-130 MeV]; m e a s u r e d E7,I%77-, 7 ( X - r a y ) - e o i n f o l l o w i n g B - d e c a y ; d e d u c e d N=82 s i n g l e p a r t i c l e e n e r g y gap. 146Tb d e d u c e d Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . 145Tb d e d u c e d TI/a,Q(EC),Iog f t , I f l , G a m o w - T e l l e r b r a n c h . 147,146,11SOd d e d u c e d l e v e l s , 7 - b r a n c h i n g , e o n f i g u r a t i o n . CONF H e l s i n g o r Vo12 P548, CERN

82StZU:

145

RADIOACTIVITY 'g5,~4~,14OTb [ f r o m ~5~Eu(a,n),~52Gd(a,xnp),E=90-130 MeV]; m e a s u r e d E7,I%77-, 7 ( X - r a y ) - c o i n f o l l o w i n g f l - d e e a y ; d e d u c e d N=82 s i n g l e p a r t i c l e e n e r g y gap. ~46Tb d e d u c e d Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h , t45Tb d e d u c e d T~/a,Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . ~4~ 146,145Gd d e d u c e d l e v e l s , 7 - b r a n e h i n g , c o n f i g u r a t i o n . CONF H e l s i n g o r Vol2 P548, CERN 81-09. RADIOACTIVITY ~45,~4~,~7Tb [ f r o m ~SZGd,15tEu(a,xnyp),E=90,130 MeV]; m e a s u r e d ET,I%77-eoin f o l l o w i n g f l - d e c a y . ~45Tb d e d u c e d Q(EC),T~/2. i46Tb level d e d u c e d J,Tr. ~4~Gd d e d u c e d levels, J,rr,7-branching. 145,147Od d e d u c e d levels,J,rr,7-branching,7-multipolarity. REPT JUL-Spez-146,P56,Styczen.

A 146Ba

=

ONLY)

81-09.

RADIOACTIVITY 145,146,147Tb [ f r o m 15~Gd,lSIEu(a,xnyp),E=90,130 MeV]; m e a s u r e d E%IT,77-eoin f o l l o w i n g f l - d e c a y . ~4STb d e d u c e d Q(EC),TI/~. 146Tb level d e d u c e d J,Tr. 14~Gd d e d u c e d levels, J,rr,7-branching. ~45,147Gd d e d u c e d levels,J,rr,7-branching,7-multipolarity. REPT JUL-Spez-146,P56,Styczen. NUCLEAR REACTIONS ~4a,~49Sm((x,6n),E=76-90 MeV; m e a s u r e d 7 ( 0 ) , 7 7 - c o i n , I T , T ~ ( t ) . ~46Gd d e d u c e d l e v e l s , T ~ / z , J , r r , y r a s t b a n d . REPT J U L - S p e z - 7 2 , P 5 0 , B r o d a . NUCLEAR REACTIONS ~mTa(p,X),E=800 MeV; m e a s u r e d c u m u l a t i v e yields for A=130-180. ~4aOd(p, t),E=26 MeV; m e a s u r e d a ( E t ) , a ( 0 ) . 14~Gd d e d u c e d l e v e l s , J jr. T a r g e t *~Gd f r o m s p a l l a t i o n r e a c t i o n , c h e m i c a l s e p a r a t i o n , Q 3 D s p e c t r o m e t e r . CONF H e l s i n g o r Vol2 P684, CERN-81-09. RADIOACTIVITY ~45i47,~4STb [ f r o m i5~Eu(a,n),lS~Gd(~,xnp),E=90-130 MeV]; m e a s u r e d E7,I7,77-, 7 ( X - r a y ) - c o i n f o l l o w i n g f l - d e c a y ; d e d u c e d N=82 s i n g l e p a r t i c l e e n e r g y gap. 14OTb d e d u c e d Q(EC),Iog f t , I f l , G a m o w - T e l l e r b r a n c h , t45Tb d e d u c e d Tl/~,Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . 147,14s,145Gd d e d u c e d l e v e l s , 7 - b r a n c h i n g , e o n f i g u r a t i o n . CONF H e l s i n g o r Vol2 P548, CERN 81-09. RADIOACTIVITY ~5,~46,~47Tb [ f r o m 15~Gd,~5~Eu(a,xnyp),E=90,130 MeV]; m e a s u r e d E7,IT,77-coin f o l l o w i n g f l - d e c a y . 145Tb d e d u c e d Q(EC),T~/z. 14~Tb level d e d u c e d J,rr. 14~Od d e d u c e d levels, J,rr,7-branching. ~45,~YGd d e d u c e d levels,J,rr,7-branching,7-multipolarity. REPT J U L - S p e z - 146,P56,Sty c z e n . RADIOACTIVITY ~45Tb(EC),(fl+),~4~Dy(EC),(fi+) [ f r o m o n - l i n e s e p a r a t i o n 3 ; m e a s u r e d E7,I7, E ( X - r a y ) , I ( X - r a y ) , T ~ / ~ . CONF S a m a r k a n d , P 9 7 , A l k h a z o v .

25'7

SECONDARY

(Reports,Abstracts,etc.

SOURCES

A 14SDy

D 81NoZY:

R 81NoZY:

i~SHo

D 81NoZY:

D 79ErZS: 79VyZX: 81DeZJ:

R 80PiZU: 147Eu

D 79BuZT: 79ErZS: 79SaZF: 79VyZX: 81DeZJ:

81ScZR:

82RoZZ:

R 81RoZS: 147Gd

D 79VyZW: 81ScZR:

81StZ0:

82StZU

R 80MuZS 82KIZX 82KIZY

146

continued

RADIOACTIVITY 95mpd [ f r o m 58Ni(4°Ca,n2p),E=133-173 MeV]; m e a s u r e d f l - d e l a y e d Ep,Ip, f l - d e l a y e d p7(t); d e d u c e d log f t . 95Rh,94Ru l e v e l s d e d u c e d T - b r a n c h i n g . i46Dy [ f r o m 9°zr(aSNi,2p)3; 'S°Er [ f r o m 94Mo(SSNi,2p),geMo(S°Ni,2p)3; m e a s u r e d a ( E - / ) , 7 7 - e o i n , T T ( t ) , D S A , f l - d e l a y e d pT(t), i4SDy,i5°Er d e d u c e d levels,J,rr. 150Tm,'44Tb,*4SHo,148Er; m e a s u r e d f l - d e c a y . CONF H e l s i n g o r Voll P253, CERN 81-09. NUCLEAR REACTIONS 94Mo,9%r(SSNi,2p),E=230-250 MeV; 9aMo(6°Ni,2p),E=240-859 MeV; m e a s u r e d a ( E - / ) , 7 - / - c o i n , 7 - / ( t ) , D S A , f l - d e l a y e d p-/(t). *46DyJS°Er d e d u c e d l e v e l s , 7 - b r a n c h i n g , J , ~ r , T l / z . CONF H e l s i n g o r Voll P253, CERN 81-09. RADIOACTIVITY 95mpd [ f r o m 58Ni(4°Ca,n2p),E=133-173 MeV]; m e a s u r e d f l - d e l a y e d Ep,Ip, f l - d e l a y e d p-/(t); d e d u c e d log f t . 95Rh,94Ru l e v e l s d e d u c e d - / - b r a n c h i n g . 14SDy [ f r o m 9°Zr(SSNi,2p)3; lS°Er [ f r o m 9~Mo(SSNi,2p),gaMo(S°Ni,2p)3; m e a s u r e d a ( E T ) , T V - c o i n , 7 - / ( t ) , D S A , f l - d e l a y e d p-/(t). ~4SDy,~S°Er d e d u c e d l e v e l s , J j r , l~°Tm,i44Tb,146Ho,148Er; m e a s u r e d f l - d e c a y . CONF H e l s i n g o r Voll P253, CERN 8 i - 0 9 .

A ~47Sm

=

ONLY)

= 147

RADIOACTIVITY 147Eu; m e a s u r e d 7(0,H); d e d u c e d ix. 147Sm t r a n s i t i o n s d e d u c e d (~. O r i e n t e d n u c l e i , s o u r c e i n Cd,Ge(Li) d e t e c t o r s . CONF R i g a , P 2 4 0 , E r z i n k y a n . RADIOACTIVITY 147Eu; m e a s u r e d E % I T , I ( c e ) , - / c e - c o i n , ( K X - r a y ) ( 7 ) ( t ) , I ( K X - r a y ) . 14VSm d e d u c e d levels,J,~,T1/a. CONF R i g a , P 8 7 , V y l o v . RADIOACTIVITY 147Eu; m e a s u r e d 7(0),oriented nuclei,Fe,Gd hosts; d e d u c e d ix. 147Sin d e d u c e d levels,J,Tr,6(E2/M1),6(M2/E1). Q u a s i p a r t i c l e p l u s p h o n o n m o d e l . REPT J I N R - P 6 - 8 1 - 5 6 6 , Deryuga. NUCLEAR REACTIONS 146,'4SNd(a,3n),(a,5n),E=35-57 MeV; m e a s u r e d 7(0),77-coin. *47Sm deduced l e v e l s , J , v r , 7 - b r a n c h i n g , e o n f i g u r a t i o n s . REPT J U L - S p e z - 7 2 , P 5 5 , P i i p a r i n e n . RADIOACTIVITY 147Eu; m e a s u r e d Efl+,Ifl+; deduced Q. Mass-separator,toroid s p e c t r o m e t e r . CONF Riga,PSB,Budzyak. RADIOACTIVITY ~47Eu; m e a s u r e d -/(0,H); d e d u c e d ix. 147Sin t r a n s i t i o n s d e d u c e d 8. O r i e n t e d n u c l e i , s o u r c e i n Cd,Ge(Li) d e t e c t o r s . CONF R i g a , P 2 4 0 , E r z i n k y a n . RADIOACTIVITY 147Eu; m e a s u r e d -/7(0); d e d u c e d A2,A 4. CONF R i g a , P 8 5 , S a r z h i n s k i . R A D I O A C T I V I T Y 147Eu; m e a s u r e d E % I T , I ( c e ) , v c e - c o i n , ( K X - r a y ) ( 7 ) ( t ) , I ( K X - r a y ) . 147Sin d e d u c e d levels,J,Tr,Tt/a. CONF R i g a , P 8 7 , V y l o v . RADIOACTIVITY 147Eu; m e a s u r e d 7(0),oriented nuelei,Fe,Gd hosts; d e d u c e d ix. 14~Sm d e d u c e d levels,J,rr,~(E2/M1),d(M2/E1). Q u a s i p a r t i c l e p l u s p h o n o n m o d e l . REPT J I N R - P 6 - 8 1 - 5 6 6 , Deryuga. RADIOACTIVITY 146,147Gd,147Eu,i4SSm,148Dy,i4s,147Tb; m e a s u r e d f l + / E C , K - c a p t u r e p r o b a b i l i t y ; d e d u c e d Q(EC). 146j47Gd,147EuJ48Dy,147Tb d e d u c e d m a s s e s . CONF H e l s i n g o r Voll P148, CERN 81-09. RADIOACTIVITY 146Sm [ f r o m la%a(llB,4n)]; '47Eu [ f r o m mgLa('2C,4n)]; m e a s u r e d recoil. 14SSm, 147Eu l e v e l s d e d u c e d Ti/2. I n t e r a c t i n g boson,eluster vibrator,core-particle coupling m o d e l s . DABBB 42 2888,Rozak. NUCLEAR REACTIONS La(t2C,4n),E=62 MeV; m e a s u r e d DSA. 147Eu l e v e l s d e d u c e d TI/2,B(E2 ) enhancement,configuration. N a t u r a l t a r g e t . BAPSA 26 l155,ED1,Rozak. RADIOACTIVITY 147Gd [ f r o m Ta,Er(p,X),E=660 MeV3; m e a s u r e d I(K X-ray),Efl+,Ifl+; d e d u c e d Q. CONF R i g a , P 8 8 , V y l o v . RADIOACTIVITY 146,147Gd,147Eu,145Sm,148Dy,148,147Tb; m e a s u r e d f l + / E C , K - c a p t u r e p r o b a b i l i t y ; d e d u c e d Q(EC). i46,147Gd,147Eu,14SDy,147Tb d e d u c e d m a s s e s . CONF H e l s i n g o r Voll P148, CERN 81-09. RADIOACTIVITY 145,147,146Tb [ f r o m lS~Eu(a,n)J52Gd(a,xnp),E=90-130 MeV]; m e a s u r e d E7,17,-/7-, 7 ( X - r a y ) - c o i n f o l l o w i n g f l - d e c a y ; d e d u c e d N=82 s i n g l e p a r t i c l e e n e r g y gap. 14STb d e d u c e d Q(EC),log f t , I f l , G a m o w - T e l l e r b r a n c h . 145Tb d e d u c e d TI/2,Q(EC),log f t , l f l , G a m o w - T e l l e r b r a n c h . 147,146,145Gd d e d u c e d l e v e l s , 7 - b r a n c h i n g , e o n f i g u l ~ a t i o n . CONF H e l s i n g o r Vo12 P548, CERN 81-09. RADIOACTIVITY 145,146,147Tb [ f r o m 15~GdJS~Eu(c~,xnyp),E=90,130 MeV]; m e a s u r e d ET,I%-/7-coin f o l l o w i n g B - d e c a y . 145Tb d e d u c e d Q(EC),T,/~. 14~Tb level d e d u c e d J,~r. 146Gd d e d u c e d levels, J,~r,7-branching. 145,147Gd d e d u c e d levels,J,~r,7-branching,7-multipolarity. REPT JUL-Spez-146,P56,Styczen. NUCLEAR REACTIONS ~4~Sm(aHe,n),E=20-27 MeV; m e a s u r e d ET,I%a(E3,),T(0),7(t),TT-coin,I(ce). l¢TGd d e d u c e d l e v e l s , y r a s t b a n d , J , r r , 7 - b r a n c h i n ~ . REPT JYFL 1980 A n n , P 6 4 , M u h o n e n . NUCLEAR REACTIONS 147Sm(3He,3n),E=22,27 MeV; m e a s u r e d I(ce),ce(t). 14~Gd level deduced T~/~, 7 - b r a n c h i n g , B ( E 3 ) , t w o p h o n o n c h a r a c t e r . REPT J U L - S p e z - 1 4 6 , P 5 8 , K l e i n h e i n z . NUCLEAR REACTIONS 147Sm(3He,3n),E=22,27 MeV; m e a s u r e d ce(t), i47Gd level deduced TI/~,B(E3), two-phonon octupole character. Centroid,slope analyses,magnetic lens,Si-Li s p e c t r o m e t e r s . REPT JYFL 1981 A n n , P 8 7 , K l e i n h e i n z .

258

SECONDARY

SOURCES

(Reporks,Abstracts,etc.

A 147Tb

D 81NaZR: 81ScZR:

8tStZO:

81ToZY: 82StZU

=

/47

ONLY)

continued

R A D I O A C T I V I T Y ~47Tb [ f r o m *44Sm(%i,3n),E=29 MeV]; m e a s u r e d l ( c e ) , T V - , v ( X - r a y ) - c o i n , E % I - / ; deduced levels,J,rr,7-multipolarity,T~/a,configuration. REPT J U L - S p e z - 9 9 , P 5 1 , N a g a i . R A D I O A C T I V I T Y t4s,~4~Gd,~?Eu,14SSm,~aDy,l~a,14?Tb; m e a s u r e d fl+/EC,K-eapture probability; d e d u c e d Q(EC). ~46,*47Gd,147Eu,14SDy,14?Tb d e d u c e d m a s s e s . CONF H e l s i n g o r V o l l P148, CERN 81-09. R A D I O A C T I V I T Y 145,147,146Tb [ f r o m ~5~Eu(c~,n),tSaGd(a,xnp),E=90-130 MeV]; m e a s u r e d E"/,I7,-/-/-, 7(X-ray)-coin f o l l o w i n g f l - d e c a y ; d e d u c e d N=8~ s i n g l e p a r t i c l e e n e r g y gap. 146Tb d e d u c e d Q(EC),log f t , I f l , G a m o w - - T e l l e r branch. 145Tb d e d u c e d Ti/a,Q(EC),log ft,Ifl,Gamow-Teller b r a n c h . 147,146,145Gd d e d u c e d l e v e l s , v - b r a n c h i n g , c o n f i g u r a t i o n . CONF H e l s i n g o r V o l e P 5 4 8 , CERN 8 1 - 0 9 . R A D I O A C T I V I T Y ~47Dy [ f r o m o n - l i n e s e p a r a t i o n ] ; m e a s u r e d - / " / - c o i n . 147Tb d e d u c e d s i n g l e p r o t o n s t a t e s . B A P S A ~6 I 1 5 5 , E D R , T o t h . R A D I O A C T I V I T Y 145,146,147Tb [ f r o m 15aGd,~SlEu(a,xnyp),E=90,130 MeV]; m e a s u r e d ET,l%"/"/-coin f o l l o w i n g f l - d e c a y . ~45Tb d e d u c e d Q(EC),TI/~. 146Tb l e v e l d e d u c e d J,~r. 146Gd d e d u c e d l e v e l s , J,~r,3,-branching. 145,147Gd d e d u c e d levels,J,~r,"/-branching,-/-multipolarity. REPT

JUL- Spez-146,P56,Styczen. R 81PaZS

t47Dy

D 81ToZY

NUCLEAR REACTIONS ~4Sm(~4N,~Be),E=83 MeV; m e a s u r e d cr(E(l~Be)). 147Tb d e d u c e d l e v e l s , m a s s e x c e s s . Q3D m a g n e t i c speetrograph,AE-E p o s i t i o n s e n s i t i v e d e t e c t o r s . B A P S A 26 1155,ED3, Parks. R A D I O A C T I V I T Y ~4?Dy [ f r o m o n - l i n e s e p a r a t i o n ] ; m e a s u r e d "/"/-coin. 147Tb d e d u c e d s i n g l e p r o t o n s t a t e s . B A P S A ~6 l 1 5 5 , E D 2 , T o t h .

A ~48La

D 82BrZX

i4~Ce

8~GiZZ D 82GiZZ 82WoZY

t4aSm

R 79MuZR

148Eu

R 80PiZT

148Gd

D 79ShZF

14STb

D 79ShZF 80AnZD

81ScZR

14aDy

D 81ScZR

R 82ErZX

~48Er

D 81NoZY

D 79VyZV

149Eu

D 79VyZU:

148

R A D I O A C T I V I T Y 145,146,14SLa [ f r o m o n - l i n e m a s s s e p a r a t i o n ] ; m e a s u r e d f l - e n d p o i n t e n e r g i e s ; d e d u c e d Qfl. H y p e r p u r e Ge f l - s p e c t r o m e t e r . B A P S A 27 5 1 9 , E X a l 4 , B r e n n e r . R A D I O A C T I V I T Y 14SLa; m e a s u r e d -/-/(0). 14aCe l e v e l d e d u c e d J,rr. B A P S A 27 519,EXa15,Gill. R A D I O A C T I V I T Y 14SLa; m e a s u r e d 7-/(0). 148Ce l e v e l d e d u c e d J,Tr. B A P S A 27 5 1 9 , E X a l 5 , G i l l . R A D I O A C T I V I T Y 14a,146,14SCe,14a,~46La; m e a s u r e d "/7(0). F i x e d a n g l e f o u r d e t e c t o r s y s t e m . B A P S A 27 5 2 1 , E X b 1 5 , W o l f . NUCLEAR REACTIONS 147Sm(n,"/),E=24.5 keV; m e a s u r e d E%I"/. 14eSm d e d u c e d t r a n s i t i o n s . Ge(Li) d e t e c t o r . CONE R i g a , P 3 9 2 , M u r z i n . NUCLEAR REACTIONS 1 4 9 , i S ° s m ( p , 2 n ) , ( p , 3 n ) , E = 1 7 MeV; m e a s u r e d I(ce),"/"/(t),"/(ee)(t),E"/,"/(0), p " / ( t ) . 14SEu d e d u c e d levels,J,~r,T1/2,T-branching,-/-multipolarity,configurations. REPT JUL-Spez-72,P58,Piiparinen. R A D I O A C T I V I T Y 14STb; m e a s u r e d ET,I"/,I(K X - r a y ) , v - / - c o i n . t4aGd d e d u c e d levels,ICC. Ge(Li) d e t e c t o r s . CONF R i g a , P g 0 , S h c h u s . R A D I O A C T I V I T Y 148Tb; m e a s u r e d EV,I-/,I(K X - r a y ) , v V - c o i n . 14SGd d e d u c e d levels,ICC. Ge(Li) d e t e c t o r s . CONF R i g a , P 9 0 , S h c h u s . R A D I O A C T I V I T Y 151,15a,iSaEr,15°,isl,152,i5aHo,i49Dy,14STb [ f r o m 141pr,144,147Sm(14C,X),(14N,X),(i60, X)]; measured cr(E-/),T"/-coin,T~/2,delayed T-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . R A D I O A C T I V I T Y 146,147Gd,147Eu,145Sm,i48Dy,148,147Tb; m e a s u r e d fl+/EC,K-capture probability; d e d u c e d Q(EC). 146,147Gd,147Eu,148Dy,147Tb d e d u c e d m a s s e s . CONF H e l s i n g o r V o l l P148, CERN 81-09. R A D I O A C T I V I T Y 146,147Gd,147Eu,145Sm,i48Dy,14e,147Tb; m e a s u r e d fl+/EC,K-capture probability; d e d u c e d Q(EC). 146,147Gd,1~TEu,146Dy,1~?Tb d e d u c e d m a s s e s . CONF H e l s i n g o r V o l l P148, CERN 81-09. NUCLEAR REACTIONS la4Sn(aTC1,X),E n o t g i v e n ; u~,l~°,lZ4Sn(3ZS,X),E=130-202 MeV; m e a s u r e d (X-ray)(X-ray)-,X-ray(evaporation residue)-coin; deduced X-ray multiplicity,production or. 161Ho,148,152,156Dy d e d u c e d d e c a y m e c h a n i s m . REPT A N L - 8 1 - Y 9 , P 3 7 , E r n s t . R A D I O A C T I V I T Y 95mpd [ f r o m 5 8 N i ( 4 ° C a , n 2 p ) , E = 1 3 3 - 1 7 3 MeV]; m e a s u r e d fl-delayed Ep,Ip, fl-delayed p"/(t); d e d u c e d log f t . 9 5 R h , 9 4 R u l e v e l s d e d u c e d v-branching. 14SDy [ f r o m 9 ° Z r ( 5 8 N i , 2 p ) ] ; 156Er [ f r o m 94Mo(58Ni,2p),SeMo(6°Ni,2p)]; m e a s u r e d a(ET),T-/-coIn,-/"/(t),DSA, B-delayed p v ( t ) , l~6Dy,~S°Er d e d u c e d l e v e l s , J , w . ~5°Tm,i4~Tb,146Ho,i4SEr; m e a s u r e d fl-decay. CONF H e l s i n g o r V o l l P253, CERN 8 1 - 0 9 .

A t49Sm

=

=

149

RADIOACTIVITY t49Eu [ f r o m Ta,Er(p,X),E=660 MeV]; m e a s u r e d I(K X - r a y ) , ? V ( t ) . 149Sm d e d u c e d l e v e l s , J , T r , T i / a , I C C . CONF R i g a , P 9 3 , V y l o v . R A D I O A C T I V I T Y 149Gd; m e a s u r e d Ev,I-/,I(ce),~/-/ coin. l~aEu deduced levels,T~/a,!CC, T multipolarity. CONF R i g a , P g 3 , V y l o v .

259

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 149Eu

D 79VyZV: D 79VyZU: R 80PiZV:

149Tb

D 81HoZM:

*49Dy

D 80AnZD:

D 82HiZX:

*SONd

D 82HiZX: R 82AhZZ:

15OSm

D 80PaZJ:

R 82IsZZ: ~5OEu

D 80PaZJ:

R 82SoZX:

15OGd

D 82LiZT:

82LiZU:

R 81CaZU: 15OTb

D 79BrZH:

82LiZT:

82LiZU: 15ODy

D 79LuZZ: 81HoZM:

149

continued

RADIOACTIVITY *49Eu [ f r o m Ta,Er(p,X),E=660 MeV]; m e a s u r e d I(K X-ray),77(t). 14SSm deduced levels,J,rr,T1/a,ICC. CONF R i g a , P 9 2 , V y l o v . RADIOACTIVITY ~49Gd; m e a s u r e d E T , I T , I ( c e ) , 7 7 - c o i n . *49Eu d e d u c e d levels,T,/2,ICC, 7-multipolarity. CONP R i g a , P 9 3 , V y l o v . NUCLEAR REACTIONS ~48,~49,*5°Sm(a,3n),(a,4n),(a,5n),E=38-69 MeV; m e a s u r e d ct(ET),7(0),linear polarization,??-coin. 149Gd d e d u c e d l e v e l s , J , r r , y r a s t c o n f i g u r a t i o n s , 7 - b r a n c h i n g . Shell m o d e l , kEPT J U L - S p e z - 7 2 , P 5 3 , P i i p a r i n e n . RADIOACTIVITY ~62,16*Re,l°~,*64W,*59,*58,~5?Ta,~Ss,~5?,156Hf,155,156Lu,*55,154Yb; measured Ea, a - d e c a y T ~ / 2 , a - b r a n c h i n g ; 166,*65W,~6°,~SSHf,*57Lu,*56yb,154,153Tm,~52Er,15°Dy; m e a s u r e d Ea, a - b r a n c h i n g ; 16~,~6°Ta,*53Lu,*53,*5ayb,~52Tm,*SSEr,15*Ho,~5*Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, ~s°mHf; m e a s u r e d E a , a - d e c a y T,/~; d e d u c e d Qa s y s t e m a t i c s . CONF Helsingor Voll P190, CERN 81-09. RADIOACTIVITY *sl,l°z,*53Er,*S°,~s~,*5a,*53Ho,*49Dy,~48Tb [ f r o m 141Pr,*44,*4?Sm(*4C,X),(*4N,X),(*60, X)]; m e a s u r e d a(ET),77-coin,Tl/z,delayed 7-multiplicities; d e d u c e d J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e .

A i5Opr

=

ONLY)

=

150

RADIOACTIVITY 15°pr [ f r o m Z35U(n,F),E=thermal]; m e a s u r e d ET,IT,TT-coin. 15°Nd d e d u c e d l e v e l s . BAPSA 27 521,EYal,Hill. R A D I O A C T I V I T Y 15°pr [ f r o m 235U(n,F),E=thermal]; m e a s u r e d ET,IT,77-coin. 15°Nd d e d u c e d l e v e l s . BAPSA 27 521,EYal,Hill. NUCLEAR REACTIONS ?°Zn(12C,2n),E=38.4 MeV; m e a s u r e d E?,I7,7(0). 8°Kr d e d u c e d levels,J,~r, rotational bands,configuration,yrast back bend. Two-quasiparticle plus rotor c a l c u l a t i o n s . 5SNi(14N,np),E=38 MeV; m e a s u r e d 7 ( 0 ) , 7 7 - c o i n , 7 7 ( 0 ) , o r i e n t e d n u c l e i . ?°Se d e d u c e d l e v e l s , J , r r , y r a s t b a n d , b a n d c r o s s i n g . I n t e r a c t i n g b o s o n m o d e l c a l c u l a t i o n s . 142*44 146,*4s,lS°Nd(a,a'),E n o t given; m e a s u r e d C o u l o m b e x c i t a t i o n . 15°Nd d e d u c e d E2,E4 m o m e n t s . S e m i - c l a s s i a l m o d e l . DABBB 42 2 8 8 8 , A h m e d . RADIOACTIVITY 15°mEu [ f r o m 15°Sm(p,n),E=9.5 MeV]; 152mEu [ f r o m 151Eu n e u t r o n irradiation]; m e a s u r e d l(ce),ET,IT,(ce)(K X - r a y ) - c o i n . 15°,lSeSm l e v e l s d e d u c e d B(E2),B(E2)/B(E0). REPT JYFL 1980 A n n , P 6 8 , P a s s o j a . NUCLEAR REACTIONS 152Sm(p,t),E=165 MeV; m e a s u r e d a(Et),a(O); d e d u c e d optical p a r a m e t e r s . 15°Sm d e d u c e d l e v e l s , J , T r , c o n f i g u r a t i o n . DWBA a n a l y s i s . REPT RCNP Osaka,1981 A n n , P 6 7 , lshizaki. RADIOACTIVITY 15°mEu [ f r o m 15°Sm(p,n),E=9.5 MeV]; 152mEu [ f r o m 151Eu n e u t r o n irradiation]; m e a s u r e d I(ce),ET,IT,(ce)(K X - r a y ) - c o i n . 15°,15eSm l e v e l s d e d u c e d B(E2),B(E2)/B(EO). REPT JYFL 1980 A n n , P 6 8 , P a s s o j a . NUCLEAR REACTIONS 152Sm(p,3n),E=29 MeV; m e a s u r e d E%IT,TT-coin,7(O),I(ce). 15°Eu d e d u c e d isomer Ti/2,1evels,Jjr,T-branching,7-multipolarity. REPT J U L - S p e z - 1 4 6 , P 5 5 , S o r a m e l . RADIOACTIVITY 15°,15~,154,15STb; m e a s u r e d 7(0),oriented nuclei,Gd host. 15°Gd d e d u c e d levels, J,Tr,band s t r u c t u r e , 8 , B ( E 0 ) / B ( E 2 ) , l°e,154,156Gd d e d u c e d b a n d s t r u c t u r e . Boson m o d e l s . REPT JYFL 1981 A n n , P 3 0 , L i p a s . RADIOACTIVITY 15°15a,154,156Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d 7(0),oriented n u c l e i i n Gd. 15°,15z,154,15°Gd l e v e l s d e d u c e d J , r r , 8 , 7 - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 2 , Lipas. NUCLEAR REACTIONS 82Se(6SZn,xn)147Gd/146Gd/145Gd/,E ~ 200-330 MeV; measured production or(E) f o r 147,146,145Gd. ~ ° G d d e d u c e d f u s i o n b a r r i e r . REPT IPN 1981 A n n u a l , P R 7 , C a b o t . RADIOACTIVITY 15°Tb [ f r o m 151Eu(a,5n),136Ce(180,3np)]; m e a s u r e d I ( c e ) , T T - , 7 ( c e ) - c o i n , 7 ( 0 ) , recoil; deduced levels,Tl/z,J,~,7-branching,configuration,yrast sequence. CONF A r g o n n e ( H i g h - S p i n P h e n o m e n a in Nuclei) Proc,P401,Broda. RADIOACTIVITY 15°,lsz,154,156Tb; m e a s u r e d 7(0),oriented nuclei,Gd host. 15°Gd d e d u c e d levels, J,Tr,band s t r u c t u r e , d , B ( E 0 ) / B ( E 2 ) . 15a,154,i56Gd d e d u c e d b a n d s t r u c t u r e . Boson m o d e l s . REPT JYFL 1981 A n n , P 3 0 , L i p a s . RADIOACTIVITY l°°,~sz,154,~5°Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d 7(0),oriented n u c l e i in Gd. ~5°,~5~,154,~5~Gd l e v e l s d e d u c e d J , ~ r , d , 7 - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 ~ , Lipas. RADIOACTIVITY ~S°Dy / f r o m 152Gd(a,6n),E=75-98 MeV; ~3SCe(~SO,4n),E=83 MeV]; m e a s u r e d I(ce), ce(t); deduced levels,Tl/z,ICC,7-multipolarity,configuration. On-line orange s p e c t r o m e t e r . CONF A r g o n n e ( H i g h - S p i n P h e n o m e n a i n Nuclei) P r o c , P 4 0 3 , L u n a r d i . RADIOACTIVITY le2,JSlRe,163,1e4W,J59,158,157Ta,158,157,156Hf,Z55,156Lu,155,154yb; m e a s u r e d EQ, a - d e c a y T , / ~ , a - b r a n c h i n g ; ~68,~65W,~6°,15SHf,~5?Lu,156yb,154,153Trn,15~Er,~5°Dy; m e a s u r e d Ea, c ~ - b r a n c h i n g ; ~6t,lSOTa,J53Lu,15~,*5~yb,15~Tm,~53Er,151Ho,~5*DY,t4~Tb; m e a s u r e d Ea; 154Lu,155,154, ~56mHf; m e a s u r e d E a , a - d e c a y T~/~; d e d u c e d Qa s y s t e m a t i c s . CONF Helsingor Voll P190, CERN 81-09.

260

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A t50Dy

R 80LuZV:

I5OHo

D

EOAnZD:

82CaZY: ~50Er

D 81NoZY:

82CaZY: R

81ChZN:

8INoZY: tSOTm

D 81NoZY:

=

150

ONLY)

continued

NUCLEAR REACTIONS th~Gd(a,6n),E=90 MeV; 13SCe(~SO,4n),E=83 MeV; m e a s u r e d I(ce). t5°Dy d e d u c e d l e v e l s , I C C , T l / u , d , B ( E 2 ) , v - b r a n c h i n g . REPT J U L - S p e z - 7 2 , P 5 2 , L u n a r d i . RADIOACTIVITY tsi,15a,15aEr,iS%tsi,isz,15aHo,~SDy,14~Tb [ f r o m 141pr,144,147Sm(14C,X),(14N,X),(160, X)]; m e a s u r e d a(Ev),././-eoin,T1/e,delayed v-multiplicities; d e d u c e d J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . RADIOACTIVITY ~5°Er [ f r o m i44Sm(1eC,X)3; m e a s u r e d TI/e,E%I7; d e d u c e d log ft,J,~r, c o n f i g u r a t i o n . 15°Ho d e d u c e d l e v e l , J , ~ r , c o n f i g u r a t i o n . EAPSA 27 522,EYag,Carter. RADIOACTIVITY 95mpd [ f r o m 5SNi(4eCa,n2p),E=133-173 MeVJ; m e a s u r e d B - d e l a y e d Ep,Ip, B - d e l a y e d p v ( t ) ; d e d u c e d log f t . ~ S R h , ~ R u l e v e l s d e d u c e d v - b r a n c h i n g . 14~Dy [ f r o m 9°Zr(SaNi,2p)]; iS°Er [ f r o m 94Mo(SaNi,2p),SeMo(dONi,2p)]; m e a s u r e d cr(Ev),yV-coin,./7(t),DSA, B - d e l a y e d pv(t). '4~Dy,15°Er d e d u c e d levels,J,rr. 15eTm,l~4Tb,l~Ho,l~SEr; m e a s u r e d B - d e c a y . CONF H e l s i n g o r Voll P253, CERN 81-09. RADIOACTIVITY 15°Er [ f r o m 144Sm(12C,X)]; m e a s u r e d Tl/a,Ev,l-y; d e d u c e d log ft,J,rr, c o n f i g u r a t i o n . ~S°Ho d e d u c e d l e v e l , J , r r , c o n f i g u r a t i o n . BAPSA 27 522,EYa2,Carter. NUCLEAR REACTIONS Zr,Nb,Mo(SSNi,X),(eONi,X),E n o t g i v e n ; m e a s u r e d 7(t). ~5eEr d e d u c e d l e v e l s , T t / e , B ( E 2 ) , c o n f i g u r a t i o n . Recoil c a t c h e r - f o i l technique,NaI sum spectrometer. S h e l l m o d e l . BAPSA 26 l155,ED4,Chung. NUCLEAR REACTIONS e4Mo,SOZr(S~Ni,2p),E=230-250 MeV; 9aMo(eONi,2p),E=240-259 MeV; m e a s u r e d cr(E'Y),~/v-eoin,7"~(t},DSA,B-delayed p v ( t ) , i46Dy,iSOEr d e d u c e d levels,y-branching,J,~r,T]/~. CONF H e l s i n g o r Voll P253, CERN 81-09. RADIOACTIVITY 95mpd [ f r o m 5aNi(4OCa,n~p),E=133-173 MeV]; m e a s u r e d B - d e l a y e d Ep,Ip, B - d e l a y e d p./(t); d e d u c e d log f t . ~5Rh,94Ru l e v e l s d e d u c e d - / - b r a n c h i n g . 14eDy [ f r o m ~°Zr(5°Ni,2p)J; 156Er [ f r o m 94Mo(SSNi,2p),SeMo(~ONi,2p)]; m e a s u r e d cr(Ev),VV-coin,v./(t),DSA, B - d e l a y e d pv(t). 14~Dy,15OEr d e d u c e d levels,J,rr. 150Tm,144Tb,14SHo,14eEr; m e a s u r e d B - d e c a y . CONF H e l s i n g o r Volt P253, CERN 81-09.

A = 151 15~Nd

D 79WaZT: R 8OKaZK:

15~pm

D 79WaZT:

15~Eu

D 79VyZT: 82BaZX:

i51Gd

D 79VyZT 8tBaZP

82~BaZX ~SiTb

D 8tBaZP

~5~Dy

D 8]HoZM:

~iHo

D 8CAnZD:

81HoZM:

R 80GiZU:

RADIOACTIVITY 151Nd; m e a s u r e d n o t a b s t r a c t e d ; d e d u c e d log f t . l S i p m d e d u c e d l e v e l s , 7 - b r a n c h i n g , J , v r . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n P r o d u c t s ) , P 3 0 3 , W a l t e r s . NUCLEAR REACTIONS lS°Nd(d,pv),E=10 MeV; m e a s u r e d vv(t). 15iNd deduced levels,v-branching,J, rr. I n - b e a m " / - s p e c t r o s c o p y . REPT JYFL 1980 A n n , P 6 6 , K a t a j a n h e i m o . RADIOACTIVITY ih'Nd; m e a s u r e d n o t a b s t r a c t e d ; d e d u c e d log f t . l S l p m d e d u c e d l e v e l s , . / - b r a n e h i n g , J , w . CONF G r e n o b l e ( N u c l . S p e c t r o s c . F i s s i o n P r o d u c t s ) , P 3 0 3 , W a l t e r s . RADIOACTIVITY 151Gd [ f r o m Ta,Er(p,X),E=660 MeVJ; m e a s u r e d E%I%I(ce),I(K X - r a y ) . 151Eu d e d u c e d levels,J,vr,T1/2,ICC. CONF R i g a , P 9 4 , V y l o v . RADIOACTIVITY 151Gd; measured E./,l%l(ce),(ce)~/-coin; deduced log ft. t5tEu deduced levels, ICC,J,~,Nilsson a s s i g n m e n t s , . / - m u l t i p o l a r i t y .REPT JINR-P6-82-8,Badalov. RADIOACTIVITY 151Gd [ f r o m Ta,Er(p,X),E=660 MeV3; measured E./,I%I(ce),I(K X-ray). 151Eu deduced levels,J,vr,Ti/2,1CC. CONF Riga,P94,Vylov. RADIOACTIVITY 15iTb [ from Ta(p,X),E=660 MeV]; measured E./,I%I(ee),v(ee)-coin; deduced log ft. 151Gd deduced ]evels,J,vr. Toroidal fl-spectrometer,Ge(Li),Si(Li) detectors. REPT JINR-P6-81-345,Badalov. RADIOACTIVITY ISIGd; measured E%Iv,I(ce),(ce)./-coin; deduced log ft. 151Eu deduced levels, ICC,J,vr,Nilsson a s s i g n m e n t s , . / - m u l t i p o l a r i t y .REPT JINR-P6-82-8,Badalov. RADIOACTIVITY 151Tb [ from Ta(p,X),E=660 MeV]; measured Ev,l./,I(ce),7(ce)-coin; deduced log ft. 15tGd deduced levels,J,vr. Toroidal fl-spectrometer,Ge(Li),Si(Li) detectors. REPT JINR-P6-Sl-345,Badalov. RADIOACTIVITY 162,161Re,i63,164w,lS9,158,157Ta,158,157,156Hf,155,156Lu155,154yb; measured Ea, a - d e c a y T ~ / a , ( x - b r a n c h i n g ; 16s,~65W,16o,isSHf,lSVLu,tSeyb,tS4,1S~Tm,i52Er,~SODy; m e a s u r e d Ea, a - b r a n c h i n g ; 16i,160Ta,153Lu,]53,/52yb,iS2Tm,153Er,lSlHo,lSlDy,i49Tb., m e a s u r e d Ea; 154Lu,I55,154, lsdmHf; m e a s u r e d E a , a - d e c a y Tl/% d e d u c e d Qa s y s t e m a t i c s . CONF Hetsingor Volt PI90, CERN 81-09. RADIOACTIVITY 151,J52,iS3Er,15°,lsl,is2,153Ho,149Dy,14STb [ f r o m 14ipr,144,14VSm(14C,X),(14N,X),(lSo, X)J; m e a s u r e d a(E./),7./-eoin,Tl/2,delayed -/-multiplicities; d e d u c e d J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . RADIOACTIVITY 162,16tRe,163,164W,159,15s,lS7Ta,158,157,156Hf,ls5,156Lu,lSh,lS4yb; measured Ea, a-decay Tl/z,a-branching; 166,16Sw,le°,laSHf i57Lu,156yb,iS4,153Tm,iS2Er ihODy; m e a s u r e d Ea, a - b r a n c h i n g ; ~si,td°Ta,15aLu,153,th~yb,iS~Tm,~S3Er,~hlHo,~SiDy,149Tb; m e a s u r e d Ea; 154Lu,155,154, i56mHf; m e a s u r e d E a , a - d e e a y Tl/2; d e d u c e d Qa s y s t e m a t i c s . CONF Helsingor Volt P190, CERN 81-09. NUCLEAR REACTIONS 144Sm(lZC,4np),E=98 MeV; 141pr(160,6n),E=131 MeV; m e a s u r e d E%Iv,./(t), . / v ( t ) , ~ / . / - c o i n , . / ( 0 ) , l i n e a r p o l a r i z a t i o n , d e l a y e d . / - m u l t i p l i c i t i e s . iSlHo d e d u c e d levels,J,vr, i s o m e r T t / 2 , . / - b r a n c h i n g , c o n f i g u r a t i o n s . REPT ISN 80-01,P35,Gizon.

261

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

151Er

D 80AnZD:

151Tm

R 81HeZU:

D 82HiZV:

~SaSm

D 79TrZM: 80PaZJ:

82HaZI: R 82PuZZ:

15ZEu

D 79AnZH: 79TrZM: 8OPaZJ:

82HaZI: R 81PiZX:

~SaGd

D 79DuZU: 79TrZM: 82LiZT:

82LiZU:

~SaTb

D 79DuZU: 82LiZT:

82LiZU:

~52Dy

D 81StZT: R 80NaZ0: 82ErZX:

~52Ho

D 80AnZD:

82E1ZW:

151

continued

R A D I O A C T I V I T Y ~5~,152,~53Er,~S°,~51,15a,15~Ho,149Dy,148Tb [from 141Pr,144,~a7Sm('4C,X),(~4N,X),(ISO, X)3; m e a s u r e d a(E?),??-coin,T~/a,delayed ?-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . NUCLEAR REACTIONS Nb,Mo(SeNi,X),(SONi,X),E n o t g i v e n ; m e a s u r e d ? ( X - r a y ) - c o i n , c o i n c i d e n t s u m s p e c t r a . 'S~Tm d e d u c e d i s o m e r J j r , B ( E 2 ) , c o n f i g u r a t i o n . Recoil catcher-foil technique, NaI s u m s p e c t r o m e t e r . S h e l l m o d e l . B A P S A 26 l 1 5 5 , E D 5 , H e l p p i .

A ~Sapr

=

ONLY)

=

152

R A D I O A C T I V I T Y 'SZPr(fl-) [ f r o m a 3 5 U ( n , F ) , E = t h e r m a l , o n - l i n e s e p a r a t i o n 3 ; m e a s u r e d T1/2,E%I?, ??-coin. B A P S A 27 7 0 4 , B C 3 , H i l l . RADIOACTIVITY 152,15amEu; m e a s u r e d E ? , I ( c e ) . 152Sm,15aGd t r a n s i t i o n s deduced ICC, ?-multipolarity,E0-matrix element. CONF R i g a , P 9 5 , T r o i t s k a y a . R A D I O A C T I V I T Y 15°mEu [ f r o m 15°Sm(p,n),E=9.5 MeV]; ls2mEu [ f r o m lSlEu n e u t r o n i r r a d i a t i o n 3 ; measured I(ce),E?,lV,(ce)(K X-ray)-coin. 15°,15eSm l e v e l s d e d u c e d B ( E 2 ) , B ( E 2 ) / B ( E 0 ) . KEPT JYFL 1980 A n n , P 6 8 , P a s s o j a . R A D I O A C T I V I T Y lSaEu; m e a s u r e d I(ce). ~SaSm t r a n s i t i o n s d e d u c e d s u b s h e l l ICC r a t i o . KEPT NEANDC(E)-233U,Vol III,P56,Hansen. NUCLEAR REACTIONS '52Sm(p,p'),E=50 MeV; m e a s u r e d a(0). 15aSm l e v e l s d e d u c e d d e f o r m a t i o n parameters for fl-vibration. Coupled-channels m o d e l . KEPT KVI 1981 A n n , P 1 0 , P u t . R A D I O A C T I V I T Y 152Eu; m e a s u r e d E(ce). D o u b l e f o c u s i n g b e t a - s p e c t r o m e t e r . CONF Riga,P518, Andreev. R A D I O A C T I V I T Y 15a,15amEu; m e a s u r e d E ? , I ( c e ) . 152Sm,152Gd t r a n s i t i o n s deduced ICC, ?-multipolarity,E0-matrix element. CONF K i g a , P 9 5 , T r o i t s k a y a . R A D I O A C T I V I T Y ls°mEu [ f r o m lS°Sm(p,n),E=9.5 MeV3; ls2mEu [ f r o m 151Eu n e u t r o n i r r a d i a t i o n ] ; measured I(ce),E?,I?,(ce)(K X-ray)-coin. 15°,15aSm l e v e l s d e d u c e d B ( E 2 ) , B ( E 2 ) / B ( E 0 ) . KEPT JYFL 1980 A n n , P 6 8 , P a s s o j a . RADIOACTIVITY lSaEu; m e a s u r e d I(ce). lSaSm t r a n s i t i o n s d e d u c e d s u b s h e l l ICC r a t i o . KEPT NEANDC(E)-232U,Vol III,P56,Hansen. NUCLEAR REACTIONS ' 5 ° N d ( T L i , 5 n ) , 1 4 s , l S ° N d ( U B , 5 n ) , E n o t g i v e n ; m e a s u r e d not abstracted. 154Tb,lSaEu d e d u c e d high-spin levels,configuration,angular momentum alignment vs rotational frequency. REPT ISN 8 1 - 0 1 , P 3 3 , P i n s t o n . R A D I O A C T I V I T Y lSaTb; m e a s u r e d 7(0); deduced Ae,A4, # . 'SaGd l e v e l s deduced J,~r, ?-multipolarity,6. Oriented nuclei,source i n Cd. CONF R i g a , P 9 6 , D u p a k . R A D I O A C T I V I T Y 152,15amEu; m e a s u r e d E ? , I ( c e ) . 15aSm,lSZGd t r a n s i t i o n s deduced ICC, ?-multipolarlty,E0-matrix element. CONF R i g a , P 9 5 , T r o i t s k a y a . R A D I O A C T I V I T Y 150,152,154,156Tb; m e a s u r e d ? ( 0 ) , o r i e n t e d n u c l e i , G d h o s t . 15°Gd d e d u c e d l e v e l s , J,w,band structure,d,B(E0)/B(E2). 152,154,156Gd d e d u c e d b a n d s t r u c t u r e . B o s o n m o d e l s . KEPT JYFL 1981 A n n , P 3 0 , L i p a s . R A D I O A C T I V I T Y 15o,lsa,'54,15STb [ f r o m Ta(p,X),E=660 MeV3; m e a s u r e d ? ( 0 ) , o r i e n t e d n u c l e i i n Gd. 15°,lsa,154,1S°Gd l e v e l s d e d u c e d J,rr,~,?-multipolarity,B(E2) r a t i o s . KEPT JYFL R R - 4 / 8 2 , Lipas. R A D I O A C T I V I T Y 15aTb; m e a s u r e d 7(0); deduced Aa,A4, # . l ~ G d levels deduced J,w, 7-multipolarity,& Oriented nuclei,source i n Cd. CONF R i g a , P 9 6 , D u p a k . R A D I O A C T I V I T Y 15o,lsz,154,156Tb; m e a s u r e d ? ( 0 ) , o r i e n t e d n u c l e i , G d h o s t . 15°Gd d e d u c e d l e v e l s , J , w , b a n d structure,6,B(EO)/B(E2). 152,15%'SSGd d e d u c e d b a n d s t r u c t u r e . B o s o n m o d e l s . KEPT J Y F L 1981 A n n , P 3 O , L i p a s . R A D I O A C T I V I T Y 15°,152,154,15STb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d ~ / ( 0 ) , o r i e n t e d n u c l e i i n Gd. ls°,15a,'s4,15SGd l e v e l s d e d u c e d J , l r , 6 , ? - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . KEPT JYFL R R - 4 / 8 2 , Lipas. R A D I O A C T I V I T Y 15aDy [ f r o m 'SZGd(a,4n)]; measured I ( c e ) , ? ( 0 ) , T V - c o i n ; d e d u c e d levels,ICC, ?-multipolarity,band structure,Tl/2,J,Tr. KEPT J U L - S p e z - 9 9 , P 5 4 , S t y c z e n . NUCLEAR REACTIONS lS2Gd(a,4n),E=60 MeV; m e a s u r e d ? 7 - c o i n , E % I ? , ~ ? ( t ) . 152Dy d e d u c e d levels, T,/a,?-multipolarity. Enriched t a r g e t . KEPT J U L - S p e z - Y 2 , P 5 9 , N a g a i . NUCLEAR REACTIONS Ia4Sn(3?C1,X),E n o t g i v e n ; u6,12o,Ia4Sn(3ZS,X),E=I30-202 MeV; m e a s u r e d (X-ray)(X-ray)-,X-ray(evaporation residue)-coin; deduced X-ray multiplicity,production a. lS~Ho,148,15a,15ODy d e d u c e d d e c a y m e c h a n i s m . REPT A N L - 8 1 - 7 9 , P 3 7 , E r n s t . R A D I O A C T I V I T Y ~s~,~sa,lS3Er,lS°,~5',~sa,~S3Ho,~49Dy,~aSTb [ f r o m '4~pr,~44,14?Sm(14C,X),(~4N,X),(I60, X)]; measured a(ET),?7-coin,T~/2,delayed ?-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . R A D I O A C T I V I T Y 152Er(fl+),~54Er(fl+) [ f r o m ~44,~47Sm(~eC,xn)]; measured E?,I?,7?-, ?(X-ray)-coin; deduced dominant d e c a y . 152,154Ho l e v e l s d e d u c e d p r o l a t e c o n f i g u r a t i o n . Helium jet capillary s y s t e m . B A P S A 27 7 0 5 , B C 4 , E l l i s - A k o v a l i .

262

SECONDARY

SOURCES

(Reports,Abstracks,etc.

A ~52Er

D 80AnZD:

81HoZM:

82E1ZW:

82MIZZ:

R 82ChZQ: ~SZTm

D 81HoZM:

152yb

D 81HoZM:

=

R

t53Eu

D 79MaYV:

81F1ZW:

R ?9BoZH: 153Gd

D 79MaYV: 80KoZL:

153Tb

D 8OKoZL:

153HO

D 80AnZD:

153Er

D 80AnZD :

81KoZM:

continued

RADIOACTIVITY 15t,~sa,~53Er,~5°,~5~,~sa,tSaHo,t49Dy,~4~Tb [ f r o m 141pr,144,I47Sm(14C,X),(14N,X),(160, X)]; m e a s u r e d ~r(E-/),~/-coin,T~/a,delayed ~/-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . RADIOACTIVITY lez,tSlRe,ies,~64W,159,15~,~57Ta,~Ss,~57,15~Hf,i55,t56Lu,155,t54yb; m e a s u r e d Ea, a-decay T~/~,a-branching; tee,~eSW,~6°,~59Hf,157Lu,~Seyb,154,tSaTm,tSaEr,~5°Dy; m e a s u r e d Ea, a-branching; t61,~6°Ta,~SSLu,~Ss,~saYb,tSaTm,~SaEr,tS~Ho,~5~Dy,~49Tb; m e a s u r e d Ea; 154Lu,155,154, ~56mHf; m e a s u r e d E a , a - d e e a y T~/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09. RADIOACTIVITY tS2Er(fl+),~S4Er(fl +) [ f r o m t**,'4~Sm(~eC,~n)]; measured E3',I3','/7-, -?(X-ray)-coin; deduced dominant d e c a y . ~sa,~S4Ho l e v e l s d e d u c e d p r o l a t e c o n f i g u r a t i o n . H e l i u m j e t c a p i l l a r y s y s t e m . BAPSA 27 7 0 5 , B C 4 , E l l i s - A k o v a l i . RADIOACTIVITY tssYb [ f r o m t4VSm(t60,Tn)3; m e a s u r e d Tt/a,Ea,Ia,I%E%E(X-ray),l(X-ray),fl-, E C - d e c a y ; d e d u c e d log f t . t56Tm d e d u c e d level,J,zr. ~5aEr,tSeyb,~SeTm d e d u c e d a - b r a n c h i n g r a t i o . BAPSA 27 5 a a , E Y a 4 , M l e k o d a j . NUCLEAR REACTIONS 9aZr(64Ni,4n),E=B93 MeV; m e a s u r e d E-y,Iv,v'y-coin,',/3,(t). tfiaEr d e d u c e d i s o m e r s . Recoil i n t o v a c u u m , s u m e n e r g y t e c h n i q u e . REPT ANL-81-79,P42,Chowdhury. RADIOACTIVITY 16a,l~lRe,~ea,la4W,~59,tsa,tSTTa,~Ss,157,1SeHf,tss,iSeLu,~Ss,t54yb; m e a s u r e d Ea, a-decay Tt/a,a-branching; ~s6,~65W,~e°,tSgHf,~57LuJ56yb,~S4,tSaTm,iSZEr,iS°Dy; m e a s u r e d Ea, a-branching; ~e~,te°Ta,tSaLu,tSa,~saYb,tSaTm,lSaEr,~5~Ho,~StDy,~4eTb; m e a s u r e d Ea; 154Lu,tS5,154 tSbmHf; m e a s u r e d E a , a - d e c a y T~/a; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Voll P190, CERN 81-09. RADIOACTIVITY ~6a,leiRe,t63,t64w,~SS,~ss,~57Ta,tSs,lsT,~SeHf,tss,iSeLu,i55,~54yb; measured Ea, a-decay Tl/a,a-branching; ~seJeSW,~e°,tSaHf,~SVLu,~56Yb,~54,tSSTn%tSZEr,~5°Dy; m e a s u r e d Ec~, a-branching; isl,i6°Ta,~53Lu,i53,15ayb,t5aTm,i53Er,i51Ho,15tDy,i49Tb; m e a s u r e d Ea; 154Lu,155,154 tsemHf; m e a s u r e d E a , a - d e c a y T~/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Volt PI90, CERN 81-09.

A = 153pro

152

ONLY)

153

NUCLEAR REACTIONS 7°Zn,t°4Ru,u°pd,154Sm,i5s,16°Gd,isSW,t96,198Pt,2°a,aO4Hg,a44pu(polarized t,a), 1 9 S P t , a 4 4 p u , ~ 6 G e ( p o l a r i z e d t , p ) , E = 1 7 MeV; 8a,SOSe,~°°Mo,laa,t24Sn(polarized t , 3 H e ) , E = 3 3 - 8 5 MeV; m e a s u r e d c r ( 0 ) , a n a l y z i n g p o w e r v s 0,(r(Ea),a(Ep),cr(aHe). SgCu,l°aTc,l°gRh,153pm,157,159Eu, lSSTa,195,197Ir,2°l,a°SAu,~43Np,2°°Pt,246pu,78Ge,S°,SaAs,lO°Nb,122,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . RADIOACTIVITY ~SSGd; m e a s u r e d I(ce). t53Eu t r a n s i t i o n s d e d u c e d ICC,6. CONF Riga,P98, Marchilashvili. NUCLEAR REACTIONS 153Eu(n,n'-/),E=fast; m e a s u r e d E%I% 154Sm(d,3n'y),E=13.5 MeV; m e a s u r e d E%I% 153Eu d e d u c e d l e v e l s , J j r . CONF R i g a , P 9 9 , B o n d a r e n k o . RADIOACTIVITY 153Gd; m e a s u r e d I(ce). 153Eu t r a n s i t i o n s d e d u c e d ICC,d. CONF Riga,P98, Marchilashvili. RADIOACTIVITY 153Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d E-/,I-/,-I,(0,H,T); d e d u c e d n u c l e a r orientation p a r a m e t e r . 153Gd l e v e l s d e d u c e d J,Tr,d. REPT JYFL 1980 Ann,P72,Konicek. RADIOACTIVITY 153Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d E%I%~(0,H,T); d e d u c e d n u c l e a r o r i e n t a t i o n p a r a m e t e r . 153Gd l e v e l s deduced J,Tr,d. REPT JYFL 1980 A n n , P 7 2 , K o n i c e k . RADIOACTIVITY ~5~,15e,153Er,15~,lst,15z,153Ho,l~gDy,14STb [ f r o m 14~Pr,144j47Sm(14C,X),(14N,X),(160, X)]; m e a s u r e d cr(E~/),~-/-coin,Twa,delayed 7-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - O l , P 3 4 , A n d r e . RADIOACTIVITY 151,152,t53ErJS°,lsi,15a,153Ho,t49Dy,t48Tb [ f r o m 14tpr,144,I47Sm(~4C,X),(~N,X),(160, X)]; m e a s u r e d G(E~),-I,7-coin,Twa,delayed "/-multiplicities; deduced J. M u l t i p l i c i t y f i l t e r . REPT ISN 8 0 - 0 1 , P 3 4 , A n d r e . RADIOACTIVITY 16a,'61Re,lS3,164W,159,15~,~57Ta,~58,t57,~SeHf,'ss,~SeLu,~55,~54yb; measured Ea, a - d e c a y Ti/a,a-branching; ~6~,t~SW,le°,lSSHf,i57Lu,156yb,154,'53Tm,i52Er,~5°Dy; measured Ea, a-branching; 16~,16°TaJSaLu,tSa,lseYb,taaTm,~SSEr,~SlHo,~SlDy,14~Tb; m e a s u r e d Ear 154Lu,155,154 ~56mHf; m e a s u r e d E a , a - d e e a y T~/z; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN

81-09. t53Tm

D

79BeYR: 81HoZM:

RADIOACTIVITY 157Lu [ f r o m Ta(p,X),E=I GeV]; m e a s u r e d T~/a,Ea. 1SaTin [ f r o m 157Lu a - d e c a y ] ; m e a s u r e d E~,Ia. M a s s - s e p a r a t o r . CONF R i g a , P 1 0 6 , B e r l o v i e h . RADIOACTIVITY ~sz,ifiIRe,16~,~64 W,~59,~ss,157Ta,lSS,~ 5v,156Hf,155,~56Lu,~ ~5,154 y b; measured Ea, a-decay Tl/a,a-branching; la6,tSSW,ie°,lSgHf,~57Lu,15syb,iS4,1SaTmJSZErJ5°Dy; measured Ea, a-branching; ~s~,~S°Ta,~SaLu,~53,~5~Yb,~SaTm,~53ErJSlHo,~5~Dy,~49Tb; m e a s u r e d Ear 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e e a y T~/2; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Voll P190, CERN 81-09.

263

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

t53yb

D

153Lu

D 81HoZM:

81HoZM:

D 8gLeZW: R 79BaYI: 79HeZG:

154Gd

D 82LeZW: 82LiZT:

82LiZU: J ~5+Tb

81LaZX:

D 8~LiZT:

82LiZU:

R 81PiZX: t54Dy

R

81PaZT:

82KuZS:

82PaZS:

15+Ho

D 82ElZW:

*~4Er

D 82EIZW:

R 81NgZX: 82KuZZ:

~54Tm

D 81HoZM:

153

continued

R A D I O A C T I V I T Y 162,t61Re,163,164W,159,158,157Ta,158,157,156Hf,155,t56Lu,155,154yb; m e a s u r e d Ea, a-decay T1/a,a-branching; 166,t65W,16°,i59Hf,157Lu,15eyb,~54,153Tm,15aEr,156Dy; m e a s u r e d Ea, a-branching; lel,lS°Ta,15aLu,~Sa,15aYb,15eTm,15aEr,t51Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e c a y T1/2; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09. R A D I O A C T I V I T Y lsa,161Re,163,1~4W,i5~,lhs,~57Ta,15s,~57,t56Hf,155,156Lu,155,t54yb; m e a s u r e d Ea, a-decay Tl/z,a-branching; 166,185W,16°,159Hf,157Lu,156yb,154,153Tm,152Er,15°Dy; m e a s u r e d Ea, a-branching; 161,16°Ta,153Lu,153,152yb,15~Tm,153Er,151Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 15~mHf; m e a s u r e d E a , a - d e c a y T~/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

A

154Eu

=

ONLY)

=

154

R A D I O A C T I V I T Y 154Eu; m e a s u r e d - / - / - / ( 0 ) , o r i e n t e d n u c l e i . 154Gd t r a n s i t i o n d e d u c e d 6(E2/M1). Ge(Li),NaI(T1) d e t e c t o r . DABBB 42 4 4 6 8 , L e w i s . NUCLEAR REACTIONS 1 5 a E u ( n , - y ) , E = t h e r m a l ; m e a s u r e d E'hI'v. 154Eu d e d u c e d levels,J,~r,K, T-multipolarity. CONF R i g a , P 1 0 0 , B a l o d i s . NUCLEAR REACTIONS 1 5 a E u ( n , - / ) , E = t h e r m a l ; m e a s u r e d -y-y-coin. lS+Eu d e d u c e d level,Tl/2. REPT ZFK-385,P50,Heiser. R A D I O A C T I V I T Y 154Eu; m e a s u r e d - / 7 - / ( 0 ) , o r i e n t e d n u c l e i . 154Gd t r a n s i t i o n d e d u c e d 6(E2/M1). Ge(Li),NaI(T1) d e t e c t o r . DABBB 42 4 4 6 8 , L e w i s . R A D I O A C T I V I T Y 15°,152,154,156Tb; m e a s u r e d -/(O),oriented n u c l e i , G d h o s t . 15°Gd d e d u c e d l e v e l s , J,rr,band structure,~,B(E0)/B(E2), tha,154,156Gd d e d u c e d b a n d s t r u c t u r e . B o s o n m o d e l s . REPT JYFL 1981 A n n , P 3 0 , L i p a s . R A D I O A C T I V I T Y 15°,15a,154,156Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d 7 ( 0 ) , o r i e n t e d n u c l e i i n Gd. 15°,15a,154,156Gd l e v e l s d e d u c e d J , r r , 6 , ~ - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 2 , Lipas. NUCLEAR MOMENTS 154,15s,158,lS°Gd; m e a s u r e d m u o n i c X - r a y s , i s o m e r s h i f t s ; d e d u c e d r m s r a d i i differences,quadrupole moments. Model independent a n a l y s i s . DABBB 4 2 1 9 3 2 , L a u b a c h e r . R A D I O A C T I V I T Y 15°,15a,15+,156Tb; m e a s u r e d - / ( 0 ) , o r i e n t e d n u c l e i , G d h o s t . 15°Gd d e d u c e d l e v e l s , J,~r,band structure,6,B(E0)/B(E2), lsa,154,15~Gd d e d u c e d b a n d s t r u c t u r e . B o s o n m o d e l s . REPT JYFL 1981 A n n , P 3 0 , L i p a s . R A D I O A C T I V I T Y 15o,152,154,t56Tb E f r o m Ta(p,X),E=660 MeV]; m e a s u r e d - / ( 0 ) , o r i e n t e d n u c l e i i n Gd. 15°,t5a,154,15eGd l e v e l s d e d u c e d J , r r , 6 , 7 - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 2 , Lipas. NUCLEAR REACTIONS 15°Nd(TLi,5n),14s,~5°Nd(t*B,5n),E n o t g i v e n ; m e a s u r e d not abstracted. 154Tb,152Eu d e d u c e d high-spin levels,configuration,angular momentum alignment vs rotational frequency. REPT ISN 8 1 - 0 1 , P 3 3 , P i n s t o n . NUCLEAR REACTIONS l a 4 S n ( a 4 S , 4 n ) , E = 1 4 5 - 1 6 5 MeV; m e a s u r e d r e c o i l , ~ - s p e c t r a . 154Dy d e d u c e d levels,J,rt,Tl/2,prolate to oblate transition along yrast line. B A P S A 26 1116,AD2, Pakkanen. NUCLEAR REACTIONS t59Tb(a,p),(a,np),(a,2np),(a,3np),(a,4np),(a,5np),(a,6np),(a,d),(a,nd), (a,2nd),(a,3nd),(a,4nd),(a,hnd),(a,t),(a,nt),(a,2nt),(a,3nt),(a,4nt),E=75 MeV; m e a s u r e d p-/-,d~/-,t~/-eoin,a(Ep,O),a(Ed,O),a(Et,O); d e d u c e d reaction mechanism. 162,1s°,lhs,154Dy deduced yrast band side feeing distributions. REPT J U L - S p e z - 1 4 6 , P 3 7 , K u t s a r o v a . NUCLEAR REACTIONS 124Sn(34S,4n),E=145-165 MeV; m e a s u r e d - / - / - c o i n . 154Dy d e d u c e d l e v e l s , yrast sequence,J,rr,effective moment o f i n e r t i a . REPT A N L - 8 1 - 7 9 , P 4 1 , P a k k a n e n . R A D I O A C T I V I T Y l ~ a E r ( f l + ) , ~ 5 4 E r ( f l +) [ f r o m 144,1478m(laC,xn)]; measured 27,17,77-, y(X-ray)-coin; deduced dominant d e c a y , t52,154Ho l e v e l s d e d u c e d p r o l a t e c o n f i g u r a t i o n . Helium jet capillary s y s t e m . B A P S A 27 7 0 5 , B C 4 , E l l i s - A k o v a l i . RADIOACTIVITY 15aEr(fl+),154Er(fl+) [from 144,147Sm(laC,xn)3; measured 2%I%77-, -/(X-ray)-coin; deduced dominant d e c a y . 152,154Ho l e v e l s d e d u c e d p r o l a t e c o n f i g u r a t i o n . Helium jet capillary s y s t e m . B A P S A 27 7 0 5 , B C 4 , E l l i s - A k o v a l i . NUCLEAR REACTIONS 126Te(aas,4n),E=148 MeV; m e a s u r e d -/(0,H,t). 154Er d e d u c e d i s o m e r g,J,~r, configuration. REPT IPN 1981 A n n u a l , P N 5 4 , N g u y e n . NUCLEAR REACTIONS S°Zr(64Ni,xnT),E=250 MeV; m e a s u r e d n T - c o i n . 1542r d e d u c e d d o m i n a n t d e c a y channel,excitation energy angular momentum d e p e n d e n c e . Tof. BAPSA 27 4 7 5 , B X a 1 5 , K u h n . R A D I O A C T I V I T Y lS2,161Re,163,164W,15s,158,157Ta,l~S,157,15~Hf,155,156Lu,155,154yb; m e a s u r e d Ea, a-decay Ti/e,a-branching; tss,*ShW,16°,lS9Hf,~57Lu,1Ssyb,*54,iSaTm,~SaEr,lS°DY; m e a s u r e d Ea, a-branching; 161,1e°Ta,15aLu,153,15~yb,152Tm,t5aEr,lSlHo,151Dy,~49Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E ~ , a - d e c a y Tl/2; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09,

264

SECONDARY

SOURCES

(Reports,Abstracks,etc.

A 154yb

D 81HoZM:

154Lu

D 81HoZM:

154Hf

D 81HoZM:

R 79PrZX:

155Gd

J

155Tb

D 79BuZE:

82TaZZ:

79BuZF

~55Dy

D 79BuZN

t55HO

D

79DzZZ

155Er

D

79DzZZ

~55yb

D 81HoZM:

~55Lu

D 81HoZM:

~55Hf

D

154

continued

RADIOACTIVITY 162,161Re,163,164w,t59,158,157Ta,158,157,156Hf,t55,156Lu,155,154yb; measured Ea, a-decay Ti/~,a-branching; i66,~65W,~6°,~59Hf,157Lu,i56yb,154,153Tm,~52Er,15°DY; measured Ec~, a - b r a n c h i n g ; 16t,~6°Ta,~53Lu,i53,15zYb,~SZTm,153Er,tSIHo,151Dy,i49Tb; measured Ea; ~54Lu,i55,154, i56mHf; measured Ea,a-decay Ti/~; deduced Qa systematics. CONF Helsingor VoIl PIg0, CERN 82-09. RADIOACTIVITY t6z,16~Re,~n3,i64w,i59,~58,157Ta,i58,157,156Hf,~55,156Lu,i55,i54yb; measured Ec(, a-decay Ti/z,a-branching; 166,~65W,tS°,~59Hf,t57Lu,~56yb,154,i53Tm,~5ZEr,~SODy; measured Ea, a - b r a n c h i n g ; 161,16°Ta,153Lu,153,152yb,152Tm,153Er,151Ho,151Dy,t49Tb;measured Ea; 154Lu,155,154, i56mHf; measured Ea,a-decay Ti/2; deduced Qa systematics. CONF Helsingor Voll P190, CERN 81-09. R A D I O A C T I V I T Y is~,t61Re,i63,iS4w,~59,~58,157Ta,158,~57,~56Hf,~ss,~56Lu,155,154yb; m e a s u r e d Ea, a-decay T i / a , a - b r a n e h i n g ; ~66,165W,ie°,159Hf,~SVLu,~SeYb,~54,~53Tm,~52Er,15°Dy; m e a s u r e d Ea, a--branching; l~t,~6OTa153Lu153,~seyb,iSaTm,153Er,15~Ho,15~Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d Ea,a-decay Tt/a; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Voll P l g 0 , CERN 82-09.

A ~55Eu

=

ONLY)

=

155

NUCLEAR REACTIONS t 5 4 E u ( n , v ) , E = t h e r m a l ; measured V - s p e c t r a . 155Eu d e d u c e d l e v e l s , J , ~ , rotational b a n d . CONF R i g a , P l 0 1 , P r o k o f e v . NUCLEAR MOMENTS 155,157Gd; m e a s u r e d m u o n i e X - r a y s , h f s ; d e d u c e d q u a d r u p o l e m o m e n t s . BAPSA 37 5 2 3 , E Y a 3 , T a n a k a . R A D I O A C T I V I T Y 155Tb; m e a s u r e d 77(0,H,T); d e d u c e d h y p e r f i n e f i e l d s f o r 155Gd. S o u r c e in Fe. CONF R i g a , P 4 5 1 , B u d z y n s k i . R A D I O A C T I V I T Y 155Tb; m e a s u r e d 77(0,H,T); d e d u c e d h y p e r f i n e f i e l d s f o r 155Gd. S o u r c e in Cd. CONF R i g a , P 4 5 0 , B u d z y n s k i . R A D I O A C T I V I T Y 155Dy; m e a s u r e d Efl+,lfl +. CONF R i g a , P 1 9 2 , B u d z y a k . R A D I O A C T I V I T Y 155,15v,lsg,161,t6aEr; m e a s u r e d Ev,lv,Vee-eoin,I(K X-ray),I(ce),7~-eoin. 155 157H0 d e d u c e d levels,J,rr,T-multipolarity, i59,162H0 d e d u c e d l e v e l s , J , w . 16IHo d e d u c e d transitions,T-multipolarity. CONF R i g a , P 1 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y 155,i57,159,161,163Er; m e a s u r e d Ev,Iv,vce-coin,I(K X-ray),I(ce),v~-coin. t55, i5~Ho d e d u c e d levels,J,Tr,v-rnultipolarity, t59,163Ho d e d u c e d levels,J,~, ieiHo d e d u c e d transitions,v-multipolarity. CONF R i g a , P 1 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y ls2,i6tRe,la3,164W,159,156,~57Ta,158,i57,1SeHf,i55,15SLu,i55,i54yb; measured E(x, a-decay Tt/2,a-branching; I66,165W,16°,159Hf,157Lu,156yb,154,153Tm,152Er,15°Dy; m e a s u r e d Ea, a-branching; 161,tS°Ta,153Lu,153,152yb,15ZTm,153Er,15tHo,i51Dy,i49Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d Ea,a-decay Tl/z; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

81HoZM:

R A D I O A C T I V I T Y t62,161Re,163,tedW,15g,tss,157Ta,158,157,'56Hf,155,iSeLu,i55,154yb; measured Ea, a-decay Tl/2,a-branehing; 166,i65W,16°,159Hf,15~Lu,t56yb,~54,~53Tm,i5~Er,iS°Dy; m e a s u r e d Ea, a-branching; 16i,16°Ta,15aLu,153,15~yb,15ZTm,153Er,iS~Ho,~S~Dy,i49Tb; m e a s u r e d Ea; 154Lu,155,154, t56mHf; m e a s u r e d Ea,a-decay Tl/~; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Voll P190, CERN 82-09. RADIOACTIVITY t6~,t6tRe,/63,164w,tse,t58,157Ta,158,157,156]-If,t55,156Lu,155,154yb; m e a s u r e d E(x,

a-decay T~/z,a-branching; 166,t65W,16°,I59Hf,157LLI,156yb,154,i53Tm,152EF,15°Dy; measured Ea, a - b r a n c h i n g ; 161,16°Ta,153Lu,153,152yb,152Tm,153Er,151Ho,151Dy,149Tb; measured Ea; I54Lu,155,154, 156mHf; m e a s u r e d 81-09.

Ea,a-deeay

T1/z; d e d u c e d

A

15SEu

D 80lwZW:

156Gd

D 89IwZW: 8~LiZT:

82LiZU:

3 8:LLaZX :

=

Qa s y s t e m a t i c s .

CONF H e l s i n g o r

V o l l P190, CERN

156

R A D I O A C T I V I T Y tSSTb [ f r o m 156Gd(p,n)]; 156Eu; m e a s u r e d E7,I 7. iSSGd d e d u c e d B(E2),B(E1). Perturbation band-mixing calculations. REPT INS T o k y o 1980 A n n , P 4 1 , I w a t a . R A D I O A C T I V I T Y t56Tb [ f r o m 15SGd(p,n)]; 15SEu; m e a s u r e d ET,I T. 156Gd d e d u c e d B(E2),B(EI). Perturbation band-mixing calculations. REPT INS T o k y o 1980 A n n , P 4 1 , I w a t a . R A D I O A C T I V I T Y 15°,isz,15~,~56Tb; m e a s u r e d T ( 0 ) , o r i e n t e d n u c l e i , G d h o s t . iS°Gd d e d u c e d l e v e l s , J , r r , b a n d structure,6,B(EO)/B(E2), lsz,154,'SSGd d e d u c e d b a n d s t r u c t u r e . B o s u n m o d e l s . REPT J Y F L 1982 A n n , P 3 0 , L i p a s . R A D I O A C T I V I T Y 15°,t52,154,15STb [ f r o m Ta(p,X),E=660 MeV3; m e a s u r e d 7 ( 0 ) , o r i e n t e d n u c l e i i n Gd. 150,t5z 154~56Gd l e v e l s d e d u c e d J j r , 6 , 7 - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 2 , Lipas. NUCLEAR MOMENTS 154,156,15s,16°Gd; m e a s u r e d m u o n i c X - r a y s , i s o m e r s h i f t s ; d e d u c e d r m s r a d i i differences,quadrupole moments. Model independent a n a l y s i s . DABBB 42 1 9 3 2 , L a u b a c h e r .

265

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A = ISSGd

R 82RiZW:

ISSTb

D 80IwZW: 82LiZT:

82LiZU:

15SDy

R 82ErZX:

156Tm

D 82M1ZZ:

156yb

D 81HoZM:

82M1ZZ:

15OLu

D 81HoZM:

156Hf

D 81HoZM:

R 81FIZW:

157Gd

J

157Ho

D 79DzZZ:

157Er

D 79DzZZ

82TaZZ:

81AbZU

157Tm

D 81AbZU

157Lu

D 79BeYR 81HoZM

continued

NUCLEAR REACTIONS t S S G d ( p , t ) , E = 4 0 MeV; m e a s u r e d a(Et),a(0). 156Gd l e v e l s d e d u c e d population strengths. DWBA,coupled-channels a n a l y s e s . KEPT KVI 1981 A n n , P R 0 , R i e z e b o s . R A D I O A C T I V I T Y lSSTb [ f r o m 156Gd(p,n)]; lSSEu; m e a s u r e d E7,I7. 15SGd d e d u c e d B(E~),B(E1). Perturbation band-mixing calculations. REPT INS T o k y o 1980 A n n , P 4 1 , I w a t a . R A D I O A C T I V I T Y ts°,15z,154,156Tb; m e a s u r e d 7 ( O ) , o r i e n t e d n u c l e i , G d h o s t . 15°Gd d e d u c e d l e v e l s , J , r r , b a n d structure,~,B(EO)/B(E2). 15z,154,156Gd deduced b a n d s t r u c t u r e . B o s o n m o d e l s . KEPT JYFL 1981 A n n , P 3 0 , L i p a s . R A D I O A C T I V I T Y 15°,15z,ls4,15~Tb [ f r o m Ta(p,X),E=660 MeV]; m e a s u r e d 7 ( 0 ) , o r i e n t e d n u c l e i i n Gd. 150 15e,15a,lSSGd l e v e l s d e d u c e d J , T r , ( ~ , - / - m u l t i p o l a r i t y , B ( E 2 ) r a t i o s . REPT JYFL R R - 4 / 8 2 , Lipas. NUCLEAR REACTIONS la4Sn(37C1,X),E n o t g i v e n ; u°,lz°,le4Sn(3aS,X),E=130-202 MeV; m e a s u r e d (X-ray)(X-ray)-,X-ray(evaporation residue)-coin; deduced X-ray multiplicity,production a. 161Ho,14e,152,tSeDy d e d u c e d d e c a y m e c h a n i s m . KEPT A N L - 8 1 - 7 9 , P 3 7 , E r n s t . R A D I O A C T I V I T Y 156Yb [ f r o m 147Sm(160,7n)]; m e a s u r e d Tl/z,Ea,Ia,I%Ev,E(X-ray),l(X-ray),fl- , E C - d e c a y ; d e d u c e d log f t . 15STm d e d u c e d l e v e l , J j r . 15ZEr,15syb,156Tm d e d u c e d a - b r a n c h i n g r a t i o . B A P S A 27 5 2 2 , E Y a 4 , M l e k o d a j .

RADIOACTIVITY

Isz,161Re,lS3,164W,lSg,lss,157Ta,15s,157,15SHf,ls5,15SLu,155,154yb;measured

Ea,

a-decay Tl/a,a-branching; les,lSSW,16°,lSSHf,157Lu,15°yb,tS~,~53Tm,~SZEr,15°Dy; m e a s u r e d Ea, a-branching; ~61,1°°Ta,153Lu,153,~sayb,15ZTm,t53Er,151Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e c a y TI/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09. R A D I O A C T I V I T Y 15syb ] - f r o m 147Sm(lSO,7n)]; m e a s u r e d T1/a,Ea,Ia,I%ET,E(X-ray),I(X-ray),fl-, E C - d e c a y ; d e d u c e d log f t . 1SaTin d e d u c e d l e v e l , J j r . 15aEr,15syb,15STm d e d u c e d a - b r a n c h i n g r a t i o . B A P S A 27 5 2 2 , E Y a 4 , M l e k o d a j . R A D I O A C T I V I T Y tsz,'eIRe,lS3,~64W,159,t58,157Ta,158,ls7,15SHf,155,156Lu,155,15~Yb; m e a s u r e d Ea, a-decay T1/z,a-branching; 16s,'SSW,~S°,159Hf,157Lu,15syb,'54,153Tm,15ZEr,iS°Dy; m e a s u r e d Ea, a-branching; 161,1S°Ta,153Lu,153,15ayb,15aTm,153Er,151Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e c a y TI/2; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll Pl90, CERN 81-09. R A D I O A C T I V I T Y 16a,l°IRe,163,164w,lSg,158,157Ta,158,157,156Hf,155,156Lu,155,154yb; measured Ea, a-decay T1/z,a-branching; 166,165W,16°,159Hf,157Lu,156yb,15~,'53Tm,152Er,15°Dy; m e a s u r e d Ea, a-branching; 1~l,1~°Ta,15aLu,15a,152yb,lSZTm,~SaEr,a51Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 15(~mHf; m e a s u r e d E a , a - d e c a y T1/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r V o l l PI90, CERN 81-09.

A

157Eu

156

ONLY)

=

157

NUCLEAR REACTIONS 7°Zn,l°4Ru,n°pd,154Sm,i58,1S°Gd,isSw,196,19Spt,e°z,2°4Hg,Z44Pu(polarized t,a), 198pt,Z44pu,76Ge(polarized t , p ) , E = 1 7 MeV; 8 z , 8 ° S e , l ° ° M o , 1 2 a , l Z 4 S n ( p o l a r i z e d t,3He),E=22-25 MeV; m e a s u r e d o ' ( 0 ) , a n a l y z i n g p o w e r v s 0,0"(Ea),o'(Ep),o'(aHe). 69Cu,l°aTc,l°SRh,lS3pm,157,159Eu, lSSTa,195,197Ir,2°l,e°3Au,a43Np,a°°Pt,a4Spu,78Ge,8°,SaAs,l°°Nb,lZ2,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . NUCLEAR MOMENTS 155,157Gd; m e a s u r e d m u o n i c X - r a y s , h f s ; d e d u c e d q u a d r u p o l e m o m e n t s . BAPSA 27 5 2 2 , E Y a 3 , T a n a k a . R A D I O A C T I V I T Y 155,157,159,161,103Er; m e a s u r e d E-/,I%Tce-coin,I(K X-ray),I(ce),77-coin. 155 157H0 d e d u c e d levels,Jjr,7-multipolarity. 159,1SaHo d e d u c e d levels,Jjr. 1ellis d e d u c e d transitions,7-multipolarity. CONF Riga,PlO3,Dzhelepov. R A D I O A C T I V I T Y 155,157,159,161,lSaEr; m e a s u r e d ET,IT,yce-coin,l(K X-ray),I(ce),'yT-coin. 155 157H0 d e d u c e d levels,J,~T,7--multipolarity. 159,163Ho d e d u c e d levels,Jjr, lSlHo d e d u c e d transitions,7-multipolarity. CONF R J g a , P l 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y 157,161Tm E f r o m E r ( p , x n ) , E = 2 0 0 MeV3; m e a s u r e d 7 ( c e ) ( t ) , ( c e ) ( c e ) ( t ) , E T . 161Er deduced levels,T1/a,B(k),-/-multipolarity. 157Er d e d u c e d transitions,T1/2. KEPT IPN 1981 Annual,PN37,Abreu. R A D I O A C T I V I T Y 157,161Tm [ f r o m E r ( p , x n ) , E = 2 0 0 MeV3; m e a s u r e d 7 ( c e ) ( t ) , ( c e ) ( c e ) ( t ) , E % 16lEt deduced levels,Tt/a,B(k),7-multipolarity. 157Er d e d u c e d transitions,T1/2. REPT IPN 1981 Annual,PN37,Abreu. R A D I O A C T I V I T Y 157Lu [ f r o m Ta(p,X),E=I GeV3; m e a s u r e d TI/z,Ea. 1SaTin [ f r o m 157Lu a decay3; measured Ea,Ia. Mass-separator. CONF R i g a , P 1 0 6 , B e r l o v i c h .

RADIOACTIVITY is2,161Re,lS3,164 W,159,158,157Ta,lSs,157,156H f,155,15SL u,155,154 Yb; m e a s u r e d

Ea,

a-decay T1/z,a-branching; 16s,165w,la°,159Hf,157Lu,156yb,154,153Tm,152Er,15°Dy; measured Ea, a-branching; 161,16°Ta,15aLu,t53,152yb,15ZTm,153Er,tSlHo,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 15°mHf; m e a s u r e d E a , a - d e c a y TI/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

266

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 157Hf

157Ta

D 8IHoZM

D

82HoZM

RADIOACTIVITY

J

~58Dy

D 79GoZS

82LaZX

R 82KuZS

157

continued

162,161Re,163,~64W,159,158,157Ta,~5S,lS7,156Hf,155,158Lu,~-55,154yb;

a decay Ti/~,a-branching; 1~,~65W,16°,i59Hf,~57Lu,156yb,154,~53Tm,15~Er,15°Dy; a-branching; 161,~S°Ta,153Lu,~53,15ayb,15~Tm,~53Er,~51Ho,151Dy,t49Tb; measured ~56mHf; measured Ea,a-deeay Ti/a; deduced Qa systematics. CONF Helsingor 81-09. RADIOACTIVITY 16~,l~IRe,163,164W,159,t58,157Ta,15s,157,156Hf,~55,15~Lu,t55,154yb; a-decay Ti/a,a-branehing; 16°,165W,~6°,i59Hf,~57Lu,156yb,~54,~53Tm,152Er,15°Dy; a-branching; ~61,1~°Ta,~S3Lu,~53,152yb,~52Tm,153Er,15~Ho,151Dy,i49Tb; measured 15smHf; measured Ea,a-decay Ti/a; deduced Qa systematics. CONF Helsingor 81-09.

A 158Gd

=

ONLY)

=

measured

Ea, measured Ea, Ea; 154Lu,155,154, VoI2 P190, CERN measured Ea, measured Ea, Ea; ~54Lu,~5s, ~54, Vo12 PIg0, CERN

158

NUCLEAR MOMENTS 154,156,158,16°Gd; measured m u o n i e X - r a y s , i s o m e r s h i f t s ; d e d u c e d r m s radii differences,quadrupole moments. Model i n d e p e n d e n t a n a l y s i s . DABBB 42 1 9 3 2 , L a u b a c h e r . RADIOACTIVITY 15SmHo; m e a s u r e d E v , I v , I ( c e ) , v V - c o i n . 158Dy d e d u c e d levels,J,rr. CONF Riga, P107,Gonusek.

NUCLEAR

REACTIONS

159Tb(a,p),(a,np),(a,2np),(a,3np),(a,4np),(a,5np),(a,6np),(a,d),(a,nd),

(a,2nd),(a,3nd),(a,4nd),(a,5nd),(a,t),(a,nt),(a,2nt),(a,3nt),(a,4nt),E=75 p~/-,dv-,t-y-coin,a(Ep,O),a(Ed,O),a(Et,O); d e d u c e d r e a c t i o n m e c h a n i s m . 158Ho

D 79GoZS

15SEt

R 82YaZT

15ayb

R 80HaZC

158Hf

D 82HoZM

~SSTa

D

81HoZM

MeV; m e a s u r e d 16a,16°,158,154Dy deduced yrast band side feeing distributions. KEPT J U L - S p e z - 1 4 6 , P 3 7 , K u t s a r o v a . RADIOACTIVITY 158mHo; m e a s u r e d E v , I v , I ( e e ) , v - y - c o i n . 15SDy d e d u c e d levels,J,vr. CONF Riga, P20Y,Gonusek. NUCLEAR REACTIONS 154Sm(14N,xnp),(14N,xnd),(14N,xnt),E n o t given; m e a s u r e d p - / - , d ' y - , t v - e o i n , v-multiplicity. ~5SEr d e d u c e d h i g h - s p i n p h a s e t r a n s i t i o n . P a r t i a l f u s i o n r e a c t i o n . BAPSA 27 7 1 5 , C D 2 1 , Y a m a d a . NUCLEAR REACTIONS 142Nd(2°Ne,4n),E=120-150 MeV; 144Sm(lSO,2n),E=80-120 MeV; m e a s u r e d 7 7 - c o i n . 15syb d e d u c e d l e v e l s . REPT I P C R - 8 0 , P 5 9 , H a s h i z u m e . RADIOACTIVITY ls2,161Re,163,~S4W,Isg,15s,157Ta,158,157,156Hf,155,156Lu~I55,154yb; measured Ea, a-decay Tl/2,~-branching; tos,165W,~S°,159Hf,~SVLu,iSsyb,iS4,t53Tm,~5~Er,~S°Dy; m e a s u r e d E~, a-branching; 161,~S°Ta,~53Lu,153,152yb,~SaTm,~53Er,~51Ho,~5~Dy,149Tb; m e a s u r e d Ea; 154Lu,I55,154, 156mHf; m e a s u r e d E a , a - d e e a y T~/a; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Vo12 PI90, CERN 81-09. RADIOACTIVITY 16a,lOlRe,163,t64W,159,158,157Ta,15s,157,156Hf,155,156Lu,155,154yb; measured Ea, a-decay Tl/a,a-branching; 166,165W,16°,159Hf,157Lu,156yb,lS4,153Tm,152Er,15°Dy; m e a s u r e d Ea, a-branching; 161,16°Ta,153Lu,153,152yb,152Tm,lS3Er,151Ho,t51Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e c a y T~/a; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Vo12 P290, CERN 82-09.

A

159Eu

R 81F1ZW

150Ho

D 79BuZM 79DzZZ

159Er

D

79BuZM 79DzZZ

80FrZQ 159Tm

D 80FrZQ

=

159

NUCLEAR REACTIONS 7°Zn,l°4Ru,ll°Pd,154Sm,158,1S°Gd,iaSW,196,198pt,2°a,a°4Hg,a44pu(polarized t,a), 1 9 S p t , a 4 4 p u , V 6 G e ( p o l a r i z e d t , p ) , E = 2 7 MeV; a a , S O S e , l ° ° M o , l a a , i a 4 S n ( p o l a r i z e d t , 3 H e ) , E = 2 2 - 2 5 MeV; m e a s u r e d a ( 0 ) , a n a l y z i n g p o w e r v s 0,a(Ea),cr(Ep),a(3He). 69Cu,l°3Tc,l°gRh,153Pm,157,159Eu, 185Ta,195,197Ir,a°l,203Au,a43Np,a°°Pt,246pu,78Ge,S°,SaAs,t°°Nb,12a,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r Vo12 P107, CERN 8 2 - 0 9 . R A D I O A C T I V I T Y 159Er; m e a s u r e d Efl+,lfl+; d e d u c e d Q. 159H0; m e a s u r e d Eft +. M a s s - s e p a r a t o r , toroid spectrometer. CONF R i g a , P 2 0 9 , B u d z y a k . R A D I O A C T I V I T Y 155,157,159,161,163Er; m e a s u r e d E-/,Iv,vce-coin,l(K X-ray),I(ce),vV-coin. 155 1~7H0 d e d u c e d levels,J,rr,-/-multipolarity. 159,163Ho d e d u c e d l e v e l s , J , z r , t61Ho d e d u c e d transitions,-y-multipolarity. CONF R i g a , P 2 0 3 , D z h e l e p o v . RADIOACTIVITY 159Er; m e a s u r e d Efl+,lfl+; d e d u c e d Q. 159H0; m e a s u r e d Eft +. Mass s e p a r a t o r , toroid spectrometer. CONF R i g a , P 1 0 9 , B u d z y a k . RADIOACTIVITY 155,157,159,161,163Er; m e a s u r e d E-/,Iv,vee-eoin,l(K X-ray),I(ce),vv-eoin. 155 157Ho d e d u c e d levels,J,rr,~-multipolarity. 159,163Ho d e d u c e d l e v e l s , J , r r . 1~1Ho d e d u c e d transitions,v-multipolarity. CONF R i g a , P 2 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y 159,161Tm [ - f r o m E r ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d -/(ce)(t). 159,161Er l e v e l s d e d u c e d TI/2. REPT IPN 2980 A n n u a l , P N 3 7 , F r a n s s o n . R A D I O A C T I V I T Y 159,161Tm E f r o m E r ( p , x n ) , E = 2 0 0 MeV3; m e a s u r e d 7 ( c e ) ( t ) . 159,161Er l e v e l s d e d u c e d TI/2. REPT [PN 2980 A n n u a l , P N 3 7 , F r a n s s o n .

267

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

~SSHf

D 81HoZM:

159Ta

D 81HoZM:

J

16OTb

D 82YoZZ:

tOODy

D 79BuZH:

81LaZX:

R 82KuZS:

ISOHo

D 79BuZH:

~soyb

D 82FeZZ:

~SOHf

D 81HoZM:

16OTa

D 81HoZM:

D 79DzZZ:

R 83ErZX:

16lEt

D 79DzZZ:

80FrZQ: 81AbZU:

ISITm

D 80FrZQ: 81AbZU:

16iTa

D 81HoZM:

continued

=

160

NUCLEAR MOMENTS 154,156,158,16°Gd; m e a s u r e d m u o n i c X - r a y s , i s o m e r s h i f t s ; deduced r m s radii differences,quadrupole m o m e n t s . Model i n d e p e n d e n t a n a l y s i s . DABBB 42 1 9 3 2 , L a u b a c h e r . RADIOACTIVITY 75Se(EC),JesSb(fl-),IaaBa(EC),iS°Tb(fl-),168Tm(EC); m e a s u r e d E v , r e l a t i v e IV. REPT NEA ND C ( J ) - 8 3 / U , P 9 , Y o s h i z a w a . RADIOACTIVITY 16°Ho,17°,172Lu,lS2Ta; m e a s u r e d I(ce). 16°Dy,17°,172yb,18aW t r a n s i t i o n s d e d u c e d s u b s h e l l i n t e n s i t y r a t i o s . D o u b l e f o c u s i n g s p e c t r o m e t e r . CONF R i g a , P 2 3 8 , B u l g a k o v . NUCLEAR REACTIONS lSOTb(a,p),(a,np),(a,2np),(a,3np),(a,4np),(a,5np),(a,6np),(a,d),(a,nd), (a,2nd),(a,3nd),(a,4nd),(a,5nd),(a,t),(a,nt),(a,2nt),(a,3nt),(a,4nt),E=75 MeV; m e a s u r e d pT-,dT-,tT-coin,a(Ep,O),a(Ed,O),a(Et,O); d e d u c e d r e a c t i o n m e c h a n i s m . 's2,1s°,lse,154Dy deduced yrast band side feeing distributions. REPT J U L - S p e z - 1 4 6 , P 3 7 , K u t s a r o v a . RADIOACTIVITY 16°Ho,17°,lTaLu,ieaTa; m e a s u r e d I(ce). iS°Dy,17°,172Yb,182W t r a n s i t i o n s d e d u c e d s u b s h e l l i n t e n s i t y r a t i o s . D o u b l e f o c u s i n g s p e c t r o m e t e r . CONF R i g a , P 2 3 8 , B u l g a k o v . RADIOACTIVITY ~s°Yb [ f r o m uSCd(4eTi,4n)]; m e a s u r e d E T , 1 7 , 7 7 - c o i n , r e c o i l . 16°yb d e d u c e d y r a s t l e v e l s , T , / ~ . BAPSA 27 5 2 2 , E Y a h , F e w e l l . RADIOACTIVITY 16a,161Re,163,164w,lSS,~58,157Ta,158,157,156Hf,lSS,156Lu,155,154yb; m e a s u r e d Ea, a-decay T1/2,a-branching; ls6,~SW,16°,15~Hf,'5~Lu,~S6yb,15a,~53Tm,15~Er,'S°Dy; m e a s u r e d Ea, a-branching; 161,16°Ta,153Lu,153,152yb,152Tm,153Er,151Ho,15IDy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 15~mHf; m e a s u r e d E a , a - d e c a y T~/~; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09. RADIOACTIVITY 16a,161Re,i63,164W,lSs,158,157Ta,lSS,157,156Hf,155,156Lu,i55,154yb; m e a s u r e d Ea, a-decay T~/a,a-branching; 166,tSSw,iS°,159Hf,157Lu,156yb,154,153Tm,15aEr,15°Dy; m e a s u r e d Ea, a-branching; 'si,iS°Ta,153Lu,'53,'5~yb,lSaTm,~53Er,i51Ho,'SlDy,'49Tb; m e a s u r e d Ea; 154Lu,155,154, ~56mHf; m e a s u r e d E a , a - d e c a y T1/z; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

A 161Ho

159

RADIOACTIVITY lsa,iSlRe,~S3,164w,i59,ise,isTTa,158,lST,lSSHf,ihS,ihSLu,155,i54yb; m e a s u r e d Ea, a-decay T~/a,a-branching; 16s,lSSw,16°,159Hf,lSTLu,lSsyb,t54,tS3Tm,ihaEr,'5°Dy; m e a s u r e d Ea, a-branching; lal,~S°Ta,iS3Lu,iSa,lsayb,15aTm,iSaEr,tSlHo,iSlDy,~49Tb; m e a s u r e d Ea; 154Lu,155,154, ~5amHf; m e a s u r e d E a , a - d e c a y T,/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09. RADIOACTIVITY ~6a,16iRe,163,164W,159,158,157Ta,158,157,156Hf,155,156Lu,155,154yb; m e a s u r e d Ea, a-decay T~/z,a-branching; iss,'SSw,'S°,lSSHf,lSVLu,~5syb,154,lS3Tm,'SaEr,~S°Dy; m e a s u r e d Ea, a-branching; lSl,16°Ta,153Lu,153,15ayb,152Tm,lS3Er,151Ho,151Dy,149Tb; measured Ea; 154Lu,155,154, ~56mHf; m e a s u r e d E a , a - d e c a y T~/a; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll PI90, CERN 81-09.

A

I66Gd

=

ONLY)

=

161

RADIOACTIVITY 155,157,159,1sl,163Er; m e a s u r e d E T , I ~ ' , T c e - c o i n , I ( K X - r a y ) , I ( c e ) , 7 7 - c o i n . i55 157Ho d e d u c e d l e v e l s , J , T r , 7 - m u l t i p o l a r i t y . 159,163H0 d e d u c e d levels,J,Tr, i61Ho d e d u c e d transitions,7-multipolarity. CONF R i g a , P l 0 3 , D z h e l e p o v . NUCLEAR REACTIONS Ia4Sn(3VC1,X),E n o t g i v e n ; ~16,1ao,la4Sn(3~S,X),E=130-202 MeV; m e a s u r e d (X-ray)(X-ray)-,X-ray(evaporation residue)-coin; deduced X-ray multiplicity,production or. lSiHo,148,15z,iSSDy d e d u c e d d e c a y m e c h a n i s m . REPT A N L - 8 1 - 7 9 , P 3 7 , E r n s t . RADIOACTIVITY 15s,lsv,i59,'sl,lS3Er; m e a s u r e d E T , I T , T c e - c o i n , I ( K X - r a y ) , I ( c e ) , 7 7 - c o i n . lss, iSTHo d e d u c e d levels,JJr,7-multipolarity. '59,163Ho d e d u c e d l e v e l s , J , ~ . 161Ho d e d u c e d transitions,7-multipolarity. CONF R i g a , P 1 0 3 , D z h e l e p o v . RADIOACTIVITY 15g,16'Tm [ f r o m E r ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d 7 ( c e ) ( t ) . l s s , l ° ' E r l e v e l s d e d u c e d Tl/2. REPT IPN 1980 A n n u a l , P N 3 7 , F r a n s s o n . RADIOACTIVITY 15~,lSiTm [ f r o m E r ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d 7(ce)(t),(ce)(ce)(t),ET. iSIEr deduced levels,Tl/z,B(k),7-multipolarity15VEr d e d u c e d t r a n s i t i o n s , T 1 / 2 . REPT IPN 1981 Annual,PN37,Abreu. RADIOACTIVITY 159,161Tm [ f r o m E r ( p , x n ) , E = 2 0 0 MeV3; m e a s u r e d 7 ( c e ) ( t ) . 159,16'Er l e v e l s d e d u c e d Tl/a. REPT IPN 1980 A n n u a l , P N 3 7 , F r a n s s o n . RADIOACTIVITY ]57,1mTm [ f r o m E r ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d -/(ce)(t),(ce)(ce)(t),E% 161Er deduced levels,Tl/2,B(),),7-multipolarity. ~57Er d e d u c e d t r a n s i t i o n s , T , / 2 . REPT IPN 1981 Annual,PN37,Abreu. RADIOACTIVITY i62,1SlRe,iS3,'64W,159,i5s,lS~Ta,lSs,157,156Hf,ths,iSSLu,155,154yb; m e a s u r e d Ea, a-decay Tl/a,a-branching; lSS,lShw,]Se,lSSHf,i57Lu,15°Yb,154,153Tm,152Er,15°Dy; m e a s u r e d Ea, a-branching; 161,iS°Ta,153Lu,iS3,152Yb,l°2Tm,'°aErJhlHo,'hlDy,'49Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d E a , a - d e c a y Ti/2; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

268

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 16~Re

D 81HoZM:

=

161

ONLY)

continued

RADIOACTIVITY ~se,lSIRe,~S3,~64W,~59,15s,157Ta,158,~57,156Hf,155,156Lu,~55,i54yb; measured Ea, a-decay T~/z,a-branching; ~66,165W,IS°,ISSHf,157Lu,~56yb,I54,~53Tm,15~Er,15°Dy; m e a s u r e d Ea, a-branching; lsl,~6°Ta,lSaLu,~Sa,~SzYb,~5ZTm,~53Er,15~Ho,tSlDy,149Tb; m e a s u r e d Ea; 154Lo,15s,154, 15SmHf; m e a s u r e d Ea,a-deeay T~/z; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r V o l l P190, CERN 81-09.

A

~6ZDy

R 8~BoZW:

8~KuZS:

ISeTm

D 81AdZY:

~zyb

D 81AdZY:

16~ W

D 8IDeZA:

8IDeZL: t~aRe

D 81HoZM:

=

NUCLEAR REACTIONS '59Tb(a,p),(a,np),(a,2np),(a,3np),(a,4np),(a,5np),(a,6np),(a,7np),(a, 8 n p ) , E = l l O MeV; m e a s u r e d p T - c o i n , a ( O , E p ) . ~SZDy d e d u c e d g i a n t r e s o n a n c e e f f e c t s i n ( a , p ) channel. R E P T JUL-Spez-146,P38,Bochev. N U C L E A R R E A C T I O N S 159Tb(a,p),((x,np),(a,2np),(a,3np),(a,4np),(a,Snp),(a,6np),(a,d),(a,nd), (a,~nd),(a,3nd),(a,4nd),(a,5nd),(a,t),(a,nt),(a,2nt),(a,3nt),(a,4nt),E=75 MeV; m e a s u r e d p 7-,d 7-,t 7-coin,or (E p,0),(y(Ed,0),(r(Et,0); deduced reaction m e c h a n i s m . 162,160,158,154Dy deduced yrast band side feeing distributions. REPT J U L - S p e z - 1 4 6 , P 3 7 , K u t s a r o v a . R A D I O A C T I V I T Y t~aYb F f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d E%I%77-,7(ce)-eoin,I(X-ray). ~ZTm deduced levels,ICC,~,7-multipolarity. REPT J I N R - P S - 8 1 - 4 5 7 , A d a m . R A D I O A C T I V I T Y ~6zyb [ f r o m T a ( p , X ) , E = 6 6 0 MeV3; m e a s u r e d ET,I%77-,7(ce)-coin,I(X-ray). ~ZTm deduced levels,ICC,6,~/-~multipolarity. REPT J I N R - P 6 - 8 1 - ¢ 5 7 , A d a m . R A D I O A C T I V I T Y ~6z~63~64~66~67~68~69Re~67~9~7~6~69~7~72~?3Ir~75~76~t ~from ~°7,~°SAg,l°s,~toCd,~3In,l~u,ltaSn(a3Cu,X)]; measured Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. RADIOACTIVITY 162,163,164 W,166,167,168,169Re,167,168,169,17°0s,168,169,17°,171,172,t73I r,175,176Pt; measured Ea. Standard Z~eBi,ziePo s o u r c e c a l i b r a t i o n . REPT I P N 0 - R C - B I - 0 7 , D e l l a N e g r a . R A D I O A C T I V I T Y *~e,~Re,~3,~6~W,15~,~s,tSTTa,~Ss,~s7,~56Hf,155,156Lu,~55,~54yb; m e a s u r e d Ea, a-decay Tl/z,a-branching; 166,16Sw,lS°,~59Hf,~57Lu,iSSyb,~54,'53Tm,15~Er,t5°Dy; m e a s u r e d Ea, a-branching; l~,'~°Ta,'S3Lu,~Sa,~sZyb,~SZTm,153Er,~5~Ho,lSIDy,~4STb; measured Ea; 154Lu,15s~t54, *56mHf; measured Ea,a-decay T~/z; deduced Qa systematics. CONF He]singor Voll PI90, CERN 81-09.

A = ~S3Ho

D 79DzZZ

~63EF

D 79DzZZ

79GoZR tS3Tm

D 79GoZR

163Lu

D 82RoZX

163 w

D 81DeZA

81DeZL 8 1HoZM

R 8 0 ] eZZ

IS4Er

R 81BaZK

163

R A D I O A C T I V I T Y ~55,157,159,161,183Er; m e a s u r e d ET,IT,Tce-coin,I(K X-ray),I(ce),77-coin. 155 157Ho d e d u c e d levels,J,~,7-multipolarity. 159,163Ho d e d u c e d levels,J,~, i61Ho d e d u c e d transitions,7-multipolarity. CONF R i g a , P 1 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y t55,157,t59,16i,taaEr; m e a s u r e d ET,IT,Tee-coin,I(K X-ray),I(ce),77-coin. t55 157Ho d e d u c e d levels,J,Tr,7--multipolarity. 159,t63Ho d e d u c e d l e v e l s , J , ~ r . 161Ho d e d u c e d transitions,7-multipolarity. CONF R i g a , P 1 0 3 , D z h e l e p o v . R A D I O A C T I V I T Y 163Tm [ - f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d Tl/a,ET,IT,I(ce). 163Er d e d u c e d l e v e l s . CONF R i g a , P l l 0 , G o r o z h a n k i n . R A D I O A C T I V I T Y ~63Tm [ f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d T , / a , E % I % I ( e e ) . ~63Er d e d u c e d l e v e l s . CONF R i g a , P l l 0 , G o r o z h a n k i n . R A D I O A C T I V I T Y 163Lu [ - f r o m 148Sm(19F,4n)3; m e a s u r e d E % I T , 7 ( 0 ) , 7 7 - c o i n ; d e d u c e d l e v e l s , J d r . B A P S A 27 5 Z 2 , E Y a 6 , R o s e n t h a l . RADIOACTIVITY 162,163,164 W,166,167,168,169Re,167,168,169,17°Os,168,169,17°,170,17~,173I r , 1 7 5 , 1 7 6 P t [from I°7,1O9Ag,l°s,'l°Cd,133In,HU,itSSn(63Cu,X)J; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. R A D I O A C T I V I T Y ~62,~63~64W'~66~67~68~69Re~67~68~69~l7~s~8~169~7~7~72~73I~I75~7~t; measured Ea. Standard elZBi,z~ZPo s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 1 - 0 7 , D e l l a Negra. RADIOACTIVITY 162,161Re,163,~W,'59,'58,157Ta,iSa,157,~5~Hf,15s,'S~Lu,~55,'54yb; measured E a , a-decay T~/a,a-branching; 16s,t65w,16°,IS9Hf,157Lu,156yb,154,153Tm,15ZEF,15°Dy; measured Ea, a-branching; ~m,~SOTa,153Lu,'53,iSZYb,~52Tm,iSaEr,~5~Ho,15~Dy,~49Tb; m e a s u r e d Ea; 154Lu,155,t54, 156mHf; m e a s u r e d Ea,a-decay Tl/z; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r Voll P199, CERN 81-09.

A i64Dy

162

=

164

NUCLEAR REACTIONS 1 5 9 T b ( 1 4 N , x n l Z C ) , ( 1 4 N , x n a ) , ( 1 4 N , 5 n a ) , ( 1 4 N , x n ' 3 C ) , E = l 1 5 MeV; m e a s u r e d 7(particle)(0),7(particle)(~). 164Dy,lSdyb deduced spin alignment parameter,width. REPT IPCR-80,P31,Ieki. NUCLEAR REACTIONS ta°Te(a4S,3n),(34S,4n),E=141 MeV; m e a s u r e d E7,17. 164Er d e d u c e d g i a n t dipole resonance 7-decay characteristics. B A P S A 26 1 1 4 3 , D B 1 4 , B a r r e t t e .

269

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A *64Er

R 82NaZW:

~64Tm

D 8~AdZZ:

ta4yb

D 82AdZZ:

R 80IeZZ:

1~4Hf

D 80DeZG:

~W

D 81DeZA:

81DeZL: 81HoZM:

R 80LeZK:

~65Er

D 79GoZH:

~5Tm

D 79GoZH:

i~hyb

D 79A1YZ:

~65Lu

D 79AIYZ:

1OSHf

D 80DeZG:

165 W

D 81HoZM:

D 81YoZX: R 82MeZY:

*ssyb

R 82NaZW:

166 W

D 8]HoZM:

166Re

D 81DeZA:

81DeZL:

continued

=

165

NUCLEAR REACTIONS 6°Ni,9°Zr,l*Sln,12°Sn,la4Sm,165Ho,197Au,2°apb(3He,3He'),E=[08.5 MeV; measured (7(E(3He)),o'(0). 6°Ni d e d u c e d GQR,F. 9°Zr,*lSIn,12°Sn,144Sm,i65Ho,*97Au d e d u c e d GQR, giant monopole r e s o n a n c e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . R A D I O A C T I V I T Y 165Tm; m e a s u r e d T i / 2 , I ( c e ) , E T , I T , 7 7 - c o i n , T e e - c o i n . lShEr d e d u c e d l e v e l s , J , ~ . CONF R i g a , P l l l , G o r o z h a n k i n . RADIOACTIVITY 16STm; m e a s u r e d T1/z,I(ce),ET,IT,77-coin,Tce-coin. 16SEr d e d u c e d l e v e l s , J , ~ . CONF R i g a , P l l l , G o r o z h a n k i n . R A D I O A C T I V I T Y *SSLu; m e a s u r e d 7 c e - c o i n . '65Yb d e d u c e d l e v e l s , J , T r , T l / 2 , 7 - m u l t i p o l a r i t y . Iron-free toroid spectrometer,Ge(Li) d e t e c t o r . CONF R i g a , P l l ~ , A l i k o v . R A D I O A C T I V I T Y *SSLu; m e a s u r e d 7 c e - c o i n . 165yb d e d u c e d l e v e l s , J , ~ , T ~ / 2 , 7 - m u l t i p o l a r i t y . Iron-free toroid spectrometer,Ge(Li) d e t e c t o r . CONF R i g a , P l l ~ , A l i k o v . R A D I O A C T I V I T Y 164,165Hf [ f r o m 13°Te(4OCa,X),E=200 MeV3; m e a s u r e d 7 7 - e n e r g y correlation. REPT IPN 1980 A n n u a l , P N 2 4 , D e l e p l a n q u e . RADIOACTIVITY l~,~6~Re,~63,~64W,~Sg,~se,~S7Ta,~Se,~57,~S6Hf,~s,iS6Lu,~Ss,~54yb; m e a s u r e d Ea, a - d e c a y T~/a,a-branching; 166,165W,16°,159Hf,157Lu,156yb,lS4,153Tm,lS2Er,15°Dy; measured Ea, a-branching; ~si,~S°Ta,~haLu,'SS,theyb,'SeTm,'hZEr,~5~Ho,~51Dy,~49Tb; m e a s u r e d Ea; 154Lu,155,154, ~hSmHf; m e a s u r e d m s , a - d e c a y T~/z; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r V o l l PI90, CERN 81-09.

A 166Ho

164

NUCLEAR REACTIONS *6~Er,164Dy(a,4n),E=47 MeV; m e a s u r e d 7 7 - c o i n , 7 ( 0 ) . '6~Yb,~4Er d e d u c e d interband,intraband transitions,7-multipolarity. REPT RCNP O s a k a , 1 9 8 1 A n n , P 1 2 5 , N a g a i . RADIOACTIVITY *s4yb; measured ET,IT,I(ce),77-,(ce)7-coin. 'SaTin deduced levels, 7-multipolarity,6. Ge(Li),Si-Li detectors,fl-spectrometer,fl-spectrograph,toroidal magnetic f i e l d s . REPT J I N R - P 6 - 8 ~ - 1 2 7 , A d a m . RADIOACTIVITY 164yb; measured ET,IT,I(ce),77-,(ce)7-coin. *~4Tm deduced levels, T-multipolarity,~. Ge(Li),Si-Li detectors,fl-spectrometer,fl-spectrograph,toroidal magnetic f i e l d s . REPT J I N R - P 6 - 8 ~ - 1 2 7 , A d a m . NUCLEAR REACTIONS i ~ g T b ( t 4 N , x n ' e C ) , ( ~ 4 N , x n a ) , ( t 4 N , 5 n ~ ) , ( l ~ N , x n ~ 3 C ) , E = l l 5 MeV; m e a s u r e d 7(particle)(0),7(particle)(~). ~64Dy,lSaYb d e d u c e d spin alignment parameter,width. REPT IPCR-80,P31,Ieki. R A D I O A C T I V I T Y ls4,~65Hf [ f r o m *3°Te(4°Ca,X),E=200 MeV]; m e a s u r e d 77-energy correlation. REPT IPN 1980 A n n u a l , P N 2 4 , D e l e p l a n q u e . RADIOACTIVITY ~6z~63~64W~6~67~68~69Re~7~68~I6~I7~s~t69~7~73~r~75~7~Pt [from 1°7,1°9Ag,l°8,11°Cd,133In,tla,tlSSn(63Cu,X)3; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. RADIOACTIVITY ~63~64W~66~67~8~69Re~7~68~9~7~8~6~7~7~72~7~I~75~Pt; measured Ea. Standard Z~ZBi,a~ZPo source calibration. REPT IPNO-RC-81-07,Della Negra. R A D I O A C T I V I T Y 16~,161Re,163,164W,159,158,157Ta,158,157,156Hf,las,156Lu,155,154yb; m e a s u r e d Ea, a - d e c a y Ti/z,a-branching; 166,165W,16Q,lS9Hf,lSTLu,156yb,154,/53Tm,/haEr,15°Dy; m e a s u r e d Ea, a-branching; 161,t6°Ta,153Lu,t53,15ayb,thaTm,*53Er,15/Ho,'5~Dy,~a9Tb; m e a s u r e d Ea; 154Lu,155,154, '56mHf; m e a s u r e d m s , a - d e c a y Ti/~; d e d u c e d Qa s y s t e m a t i c s . CONF H e l s i n g o r Voll P190, CERN 81-09.

A 165Ho

=

ONLY)

=

166

R A D I O A C T I V I T Y 124Sb,iSSmHo,lSZTa; m e a s u r e d Ev,relative I7. REPT N E A N D C ( J ) - 7 5 / U , P 2 1 , Yoshizawa. NUCLEAR REACTIONS lSSHo,238U(n,v),E=7-15 MeV; m e a s u r e d E7,I7; d e d u c e d (7(0) v s E , r e a e t i o n mechanism. 239U,166Ho t r a n s i t i o n s deduced inital,final state Nilsson assignments. Direct-semidirect m o d e l . REPT LA-9093-MS,MeDaniels. NUCLEAR REACTIONS 166Er,164Dy(a,4n),E=47 MeV; m e a s u r e d 7 7 - c 0 i n , 7 ( 0 ) . 186Yb,164Er d e d u c e d interband,intraband transitions,7-multipolarity. REPT RCNP O s a k a , 1 9 8 1 A n n , P 1 2 5 , N a g a i . R A D I O A C T I V I T Y 16a,161Re,163,164W,159,15°,'STTa,15a,'57,156Hf,lsh,156Lu,15s,154yb; m e a s u r e d Ea, a-decay Tl/a,a-branehing; t66,165W,16°,159Hf,157Lu,lSSyb,154,i53Tm,15aEr,15°Dy; m e a s u r e d Ea, a-branching; 161,16°Ta,lS3Lu,153,152yb,152Tm,153Er,151Ho,151Dy,149Tb; m e a s u r e d Ea; 154Lu,155,154, 156mHf; m e a s u r e d m s , a - d e c a y T,/z; d e d u c e d Qa s y s t e m a t i e s . CONF H e l s i n g o r V o l l P190, CERN 81-09. R A D I O A C T I V I T Y 162,163,164 W,166,167,168,169R e,167,168,169,17°Os,t68,1f19,17°,17°,17~:,1731 r , 1 7 5 , 1 7 6 p t [from lo7,1O9Ag,l°s,ll°Cd,133In,l*z,llSSn(63Cu,X)3; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. R A D I O A C T I V I T Y 162,163,164 W,166,167,168,169Re,I ST,168,169,17°Os,168,169,17°,171,172,173I r , 1 7 5 , 1 7 6 p t ; measured Ea. Standard alZBi,~lZPo s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 1 - 0 7 , D e l l a Negra.

270

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A leVEr

D

79ArZU:

=

ONLY)

167

167Tm

D

tCTRe

D 81DeZA:

RADIOACTIVITY leTTm [ f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d I ( c e ) , A u g e r s p e c t r a , lSTEr transitions deduced ICC,d,7-multipolarity,B(M2),hindranee factors. CONE R i g a , P l l 4 , Artamonova. NUCLEAR REACTIONS 1 6 7 E r ( n , n ' 7 ) , E = f a s t ; measured ET. lSTEr d e d u c e d levels,J,~r, configurations. CONE R i g a , P l l 3 , B o n d a r e n k o . RADIOACTIVITY le7Tm [ f r o m T a ( p , X ) , E = 6 6 0 MeV]; m e a s u r e d I ( e e ) , A u g e r s p e c t r a . 167Er transitions deduced ICC,d,7-multipolarity,B(M2),hindrance factors. CONE R i g a , P l l 4 , Artamonova. RADIOACTIVITY ts2.163,164W,166,ts7,168 169Re,167,168,169,1700s,t68,is9 17o,17o 172,173ir,!75 178pt

81DeZL:

[from l°~,t°gAg,~°~,~oCd,~aaIn,~ta,~tSSn(~3Cu,X)]; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della N e g r a . RADIOACTIVITY 162,163,184W,166,167,168,169Re,16?,168,169,17°Os,t68,169 17°,lTl,172,1731r,t75,t76pt ;

R 79BoZG:

iS~Os

79ArZU:

D 81DeZA:

81DeZL:

measured Ea. S t a n d a r d ~tZBi,atapo s o u r c e c a l i b r a t i o n . REPT ] P N O - R C - 8 1 - 0 7 , D e l I a N e g r a . RADIOACTIVITY 162,163,164 W,166,167,t68,169R e,167,168,169,17°0s,168,169,170 170,172 1731 r,I75,176p t [from lsT,l°OAg,1°a,il°Cd,iaaIn,it2,ttSSn(SaCu,X)J; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Delia N e g r a . R A D I O A C T I V I T Y ~62 163,te4W,~66,167,168,169Re,167,168 169,1700s,lSs,leg,lV0,171,172,t~air,175,176pt ; measured

Ea. S t a n d a r d

2t2Bi,~laPo

A tSaTm

D 8~YoZZ:

168Hf

R 82PeZS:

teSRe

D 81DeZA:

8IDeZL:

1680s

D 81DeZA:

8:LDeZL:

~eSir

D

82DeZA:

8J.D e Z L :

169Lu

D 79BaYH 79BuZL

t6aHf

R 8EPeZS

169Re

D 81DeZA

81DeZL

~SeOs

D

81DeZA

81DeZL: ISOlr

D 81DeZA:

REPT I P N 0 - R C - 8 1 - 0 7 , D e l l a

Negra.

168

Della Negra. R A D I O A C T I V I T Y 162,163,164w,tSe,167,t68,169Re,ley,168,169,1700s,168,169,170

171,172,173Ir,175 17apt;

measured Ec~. S t a n d a r d 212Bi,a12Po s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 1 - 0 7 , D e I l a N e g r a . R A D I O A C T I V I T Y 162,t63,164 w,166,167,168,169Re,i 67,168,169,17°0s,168,169,170,17° 172,173 Ir,175 176p~ [from l°?,t°QAg,l°8,11°Cd,1331n,l12,116Sn(63Cu,X)~; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della N e g r a . R A D I O A C T I V I T Y t62,163,164W,166,167,168,169Re,167,168 169,1700s 168 169 170 171 172 1731r,175 176pt; measured Ea. S t a n d a r d 212Bi,212Po s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 ! - O 7 , D e l l a N e g r a . RADIOACTIVITY 162,163,t64w,166,167,168,169Re,167,168,169,17°Os,168 169 170,170,172 173Ir,175,176pt [from l°7,1°gAg,lOs,ll°Cd,133In,lla,l16Sn(63Cu,X)~; m e a s u r e d E~. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. R A D I O A C T I V I T Y 162,163,164 W,166,167,168,169Re,167,168,169,1700s,188 169,170,17t,172,1731 r,175 176p t ;

Ea. S t a n d a r d

212Bi,Zlapo s o u r c e

A D 79BaYH 79BuZL

calibration.

R A D I O A C T I V I T Y ~SSe(EC),lz5Sb(fl-),133Ba(EC),tS°Tb(fl-),lSSTm(EC); m e a s u r e d E T , r e l a t i v e I7. REPT N E A N D C ( J ) - 8 3 / U , P 9 , Y o s h i z a wa. NUCLEAR REACTIONS 16°Gd(160,xn),E=5-9 M e V / n u c l e o n ; m e a s u r e d E T , I T , 7 - m u l t i p l i c i t i e s . 168169 17o t71,172}]f d e d u c e d s p i n a v e r a g e s . REPT J 1 N R - P T - 8 2 - 1 5 , P e t r o v . RADIOACTIVITY 162,163,164w,lS6,167,168,169Re,t67,168 169 1700s,168,169 170,170 I72,1731r 175,!76pt 107 , 109 Ag, 108 , 110Cd, 133 I n , 112 , 116S n ( 63 C u , X ) ] ; m e a s u r e d [from Ea. REPT IPN 1981 A n n u a l , P R 5 ,

measured

tsgyb

=

source

=

calibration.

REPT I P N O - R C - 8 1 - 0 7 , D e l l a

Negra.

169

RADIOACTIVITY 169Lu; measured 7ee-eoin. t69yb deduced levels,J,~. CONE Riga,Pl16,Batsev. RADIOACTIVITY 169Lu [ f r o m Ta(p,X),E=660 MeV]; measured 77(0); deduced A2,A4. 169Yb levels deduced j,d. M a s s - s e p a r a t o r . CONF Riga,Pl15,Budzynski. RADIOACTIVITY ~69Lu; measured 7ce-coin. tsgYb deduced levels,J,n. CONE Riga,P116,Batsev. RADIOACTIVITY 169Lu [ f r o m Ta(p,X),E=660 MeV]; measured 77(0); deduced A2,A4. 169yb levels deduced j,d. Mass-separator. CONF Riga,P115,Budzynski. NUCLEAR REACTIONS IS°Gd('60,xn),E=5-9 MeV/nucleon; measured ET,17,7-multiplicities. 168169 17°,i71,t~eHf deduced s p i n averages. REPT JINR-P7-82-15,Petrov. R A D I O A C T I V I T Y lea 163 164 W les 167 168 169Ret67tsa,1691700s,16s,t69170iTo,173,173ir,i75176p t [from ioT,lOgAg tfla, ,iI°Cd'1331n'l~ " ,, ,~IfSn(63'Cu ,X)3 , measured E~. REPT IPN 1981 Annual,PR5, Della N e g r a . R A D I O A C T I V I T Y ~6a~1~3~64W~66~67,~68~l69Re~67~68~169~I7~168 ~69~l7~17~t7a~73Ir~l75~6~t; m e a s u r e d Ea. S t a n d a r d alaBi,elaPo s o u r c e c a l i b r a t i o n . REPT I P N O - R C - B I - 0 7 , D e I I a N e g r a . R A D I O A C T I V I T Y 162,163,164W,166 167 168,169Re,167 168 169,170Os 168 169 i?0 170 172 1731r,175 176pt [from i°7,1°9Ag,i°8,11°Cd,t33In,t12,116Sn(63Cu,X)]; m e a s u r e d E~. REPT IPN 1981 A n n u a l , P R 5 , Delia N e g r a . RADIOACTIVITY

162,163,164W,166,167,168,169Re,167,168,169 t7°Os168,169170171,172,1731r175,176pt ;

m e a s u r e d Ea. Standard 212Bi,212Po source calibration. REPT IPNO-RC-81-07,DeIIa Negra. R A D I O A C T I V I T Y t62 i63 164W 166,167,168,169Re 167 168 169,1700s,168169170170172173ir175176p t [from lo~,lOgAg,lOa,itoCd,'133in,tla,llSSn(63Cu,X)]., m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della N e g r a .

271

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A ~69ir

D 81DeZL:

RADIOACTIVITY measured

Ea.

D 79BuZH: R 82BeZJ:

17OLu

D 796uZH:

17OHf

R 8~PeZR: 8~PeZS:

170 w

R 82AaZV:

*TO0s

D 81DeZA:

81DeZL: iTOlr

D 81DeZA:

81DeZL:

2~26i,21~Po

171yb

D 79BaYG:

171Lu

D 79BaYG:

171Hf

R 83PeZS:

1711r

D 81DeZL:

*71pt

D 81DeZB:

Ea.

Standard

212Bi,2iaPo

REPT

IPN

1981

R 82BuZW: 176Lu

D 79BuZH:

172Hf

R 82PeZS:

17air

D 81DeZA:

81DeZL: t72pt

D 81DeZB:

Os 168 169 170 171 172 173 I r , 1 7 5 , ~76 Pt," .

REPT

.

.

.

.

.

1PNO-RC-81-07,Della

Negra.

170

=

source

calibration.

REPT

IPNO-RC-81-07,Della

Negra.

171

Annual,PR5,Della

A D 79BuZH:

calibration.

N U C L E A R R E A C T I O N S 17°Er(iSO,isO),E=120 MeV; m e a s u r e d 1 5 0 7 - c o i n . *TIEr d e d u c e d 1 3 / 2 + l e v e l s . Intrinsic Ge d e t e c t o r , Q 3 D spectrometer. Quasiparticle plus rotor model. B A P S A 2 6 1116, AD4,Bond. R A D I O A C T I V I T Y 171Lu [ f r o m T a ( p , X ) , E = 6 6 0 MeVS; m e a s u r e d 7ce-coin. 171Yb d e d u c e d levels. Mass-separator. CONF R i g a , P l l 7 , B a t s e v . R A D I O A C T I V I T Y 171Lu [ f r o m Ta(p,X),E=660 MeV]; measured 7ce-coin. 171yb d e d u c e d levels. Mass-separator. CONF R i g a , P l l T , B a t s e v . NUCLEAR REACTIONS lS°Gd(160,xn),E=5-9 MeV/nucleon; measured ET,IT,7-multiplicities. 168,169 17°,171,I72Hf d e d u c e d spin averages. REPT JINR-PT-82-15,Petrov. 167 168 169 R e . 167 168 169 170 Os . 168. 169 170 171. 172 173 I t , 175 , 176 P t ; R A D I O A C T I V I T Y 162 , 163 , 184 W . 166 . . . . . . . . . measured Ea. Standard 212Bi,212P0 s o u r c e calibration. REPT IPNO-RC-81-07,Della Negra. R A D I O A C T I V I T Y 171,172,173,174pt [ f r o m l12Sn,l13In(S3Cu,X)]; measured Ea,Tl/2. Helium jet collection.

*72yb

=

source

measured Ea. Standard ~laBi,2t2Po source calibration. REPT IPNO-RC-81-07,Della Negra. R A D I O A C T I V I T Y ~62 3~ {. 1 . 164. W .166 . 167. 168. 1 6.9 R e . 167 . 168 169 1 7 0 0 s . 168. 169 . . i~0. 17o . ire 176ir,~75,17Spt [from l°7,109Ag,l°8,1I°Cd,1331n,llZ,llSSn(63Cu,X)]; measured E a . R E P T IPN 1981 A n n u a l , P R S , Delia Negra. R A D I O A C T I V I T Y 16a, 163,164 W . 166 . .167. 168 169 R e . 167 . 168 . . 169 1 7 0 0 s . 168. 169 . 170 . . 171 . 172 173 I r , 1 7 5 , 1 7 6 p t ;

A R 81BoZ0:

continued

R A D I O A C T I V I T Y iS°Ho,iT°,i72Lu,iSaTa; m e a s u r e d I(ce). 16°Dy,17°,iTeYb,162W t r a n s i t i o n s deduced subshell intensity ratios. Double focusing spectrometer. CONF R i g a , P 2 3 8 , B u l g a k o v . NUCLEAR REACTIONS l5~Gd~64'~eEr,~76Yb'176~1~Hf~'1~4W'1~7'1~1e~1~'192~s'~4'~Pt(~2C~F)'E 68-106 MeV; m e a s u r e d a(fragment 0),fission a ( E ) . J T ° Y b , 1 7 6 , * e O w , i a l R e , l S s , l S e O s , l S T I r , 186, iSaPt,194,iS6Hg,lS9,a°°,a°l,2°a,204pb,206,al°Po,a°9At deduced fission barrier. Statistical theory. REPT JINR-P7-82-402,Bejzin. RADIOACTIVITY 16°Ho,17o,172Lu,la2Ta; m e a s u r e d I(ce). i6°Dy,17°,lTaYb,iaaW t r a n s i t i o n s deduced subshell intensity ratios. Double focusing spectrometer. CONF R i g a , P 2 3 8 , B u l g a k o v . NUCLEAR REACTIONS iS°Gd(iSO,xn),(160,6n),E=l10,120,129,134 MeV; m e a s u r e d 7-multiplicity. 17°Hf d e d u c e d high-spin moment of inertia. Statistical m o d e l . REPT J I N R - P 7 - 8 2 - 3 2 1 , P e t r o v . NUCLEAR REACTIONS 16°Gd(iSO,xn),E=5-9 MeV/nucleon; measured ET,17,7-multiplicities. 168169, 17°,171,172Hf d e d u c e d spin averages. REPT JINR-P7-82-15,Petrov. N U C L E A R R E A C T I O N S l S S G d ( a ° N e , x n ) , E = l l 0 MeV; m e a s u r e d 7 7 ( 0 ) . *TOw d e d u c e d yrast band, backbending. R E P T KVI 1981 A n n , P 4 9 , A a r t s . i67 16s 169 R e . 16~ *se i69 i~0 Os . 168. ~69 i70 ~70. ,~2 * ~ I r , 17~ , ~76 P t R A D I O A C T I V I T Y 162 , 163 , 164 W . 166 . . . . . . . . . [from I°7,109Ag,l°8,11oCd,1331n,l12,116Sn(63Cu,X)]; measured E a . R E P T IPN 1981 A n n u a l , P R 5 , Della Negra. R A D I O A C T I V I T Y 162,163,164 W . 1 6.6 1. 6 7. 168 169Re . 167 . 168 . . 160 170Os . 188. 169 . . 170. 171 . 172 173 I r , 1 7 5 , 1 7 6 p t ;

measured

1TiEr

169

162,163,164W,166,167,168,169Re,167,168,169,170

Standard

A 17oyb

=

ONLY)

-

Negra.

172

RADIOACTIVITY 16°Ho,17°,i72Lu,lS2Ta; m e a s u r e d I(ce). J6°Dy,iT°,i72Yb,lsZW transitions deduced subshell intensity ratios. D o u b l e focusing spectrometer. C O N F Riga,P238,Bulgakov. NUCLEAR R E A C T I O N S 17SLu(p,a) E=I7 MeV; measured cr(e),cr(Ea). 17aYb deduced rotational bands, Nilsson configuration,d(E~/M1),band mixing. PHCAA 38 41,FA5,Burke. R A D I O A C T I V I T Y lS°Ho,*7°,lVeLu,lSeTa; m e a s u r e d l ( c e ) . 16°Dy,iT°,172Yb,ls2W t r a n s i t i o n s deduced subshell intensity ratios. Double focusing spectrometer. CONF R i g a , P 2 3 8 , B u l g a k o v . NUCLEAR REACTIONS lS°Gd(lSO,xn),E=5-9 MeV/nucleon; measured ET,IT,7-multiplicities. 166169 17°,171,172Hf d e d u c e d spin averages. REPT JINR-PT-82-15,Petrov. R A D I O A C T I V I T Y 186,163,164 W,166,167,168,169Re,167,168,169,17°0s,168,169,17°,17°,172,173I r , 1 7 5 , 1 7 S p t [from l°7,1°9Ag,l°s,n°Cd,133In,lla,llSSn(SSCu,X)]; measured E a . R E P T IPN 1981 A n n u a l , P R 5 , Della Negra. RADIOACTIVITY

162,163,164 w , l S 6 , 1 6 7 , 1 6 8 , 1 6 9 R e , 1 6 7 , 1 6 8 , 1 6 9 , 1 7 ° O s , 1 6 8 , 1 6 9 , 1 7 ° , 1 7 1 , 1 7 z , 1 7 3 I r , 1 7 5 , 1 7 6 P t ;

measured Ea. Standard alaBi,21aPo source calibration. R A D I O A C T I V I T Y 171,176,173,~74Pt [ f r o m n2Sn,n3In(S3Cu,X)]; collection. R E P T IPN 1981 A n n u a l , P R S , D e l l a Negra.

272

REPT IPNO-RC-81-07,Della Negra. measured E~,Ti/2. Helium jet

SECONDARY

SOURCES

(Reports,Abs[racks,etc.

A

173yb

D 79MuZZ:

173Lu

D 79MuZZ:

t73ir

D 81DeZA:

81DeZL: 173pt

D 81DeZB:

R 82NaZV:

174pt

D 81DeZB:

D 81DeZA:

81DeZL:

R

79BoZF 82AdZY

82PeZQ:

176 W

R 82BaZQ 82BeZJ

176pt

D 81DeZA

81DeZL

D 79EfZY 82KuZP:

177Hf

D 79EfZY: 82KuZP:

=

175

=

176

NUCLEAR REACTIONS 1 7 6 H f ( n , n ' 7 ) , E = f a s t ; m e a s u r e d E%I7. 176Hf d e d u c e d levels,J,Tr. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r . CONF R i g a , P 1 2 1 , B o n d a r e n k o . NUCLEAR REACTIONS 1 7 4 y b ( ~ , 2 n ) , E = 2 4 , 4 7 MeV; m e a s u r e d I(ce),7(t),7(0). 176Hf d e d u c e d high-spin level 7-multipolarity,6(M1/E2),(g(k)-g(R))/(quadrupole moment). REPT RCNP Osaka,1981 Ann,P131,Adachi. NUCLEAR REACTIONS 1 6 ° G d ( 1 8 0 , n ) , ( 1 6 0 , 2 n ) , ( 1 6 0 , 3 n ) , ( 1 6 0 , 4 n ) , ( 1 6 0 , S n ) , ( 1 6 0 , 7 n ) , ( 1 6 0 , 8 n ) , ( 1 8 0 , 9 n ) , (160,10n),E=80-134 MeV; m e a s u r e d 7 - m u l t i p l i c i t y ; deduced limiting angular momentum for c h a n n e l s . 176Hf d e d u c e d h i g h - s p i n state spin distribution p a r a m e t e r s . REPT J I N R - P T - 8 2 - 3 3 2 , Petrov. NUCLEAR REACTIONS 154Sm(ZdMg,4n),E=l17 MeV; m e a s u r e d 7 - m u l t i p l i c i t y , E % I 7 . 17SW d e d u c e d high-spin state transitions. B A P S A 27 7 0 5 , B C 6 , B a k t a s h . NUCLEAR REACTIONS 158Gd~64~6~Er~i76Yb~76~1~Hf~1~a~1~4W~7~8~189~19~192~s194~9~Pt(12C~F)'E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . 17°Yb,176,16°W,lalRe,lad,lSSOs,167Ir,laa, 192pt,194,196Hg,199,a°6,2°l,a°2,a°4pb,z66,a16po,2°gAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y 162,163,164W,166,i67,168,169Re,167,168169,1700s168,169170170,172,173ir,175176p~ [from l°7,1°gAg,166,n°Cd,1331n,UZ,UdSn(63Cu,X)]; m e a s u r e d E~. REPT IPN 1981 A n n u a t , P R 5 , Della Negra. R A D I O A C T I V I T Y ~62~l63~64~166~67~1~8~69Re~67~16~169~7~S~68169~7~ ~7~72,~73Ir175176Pt; measured Ea. S t a n d a r d 2~aBi,a~2Po s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 1 - 0 7 , D e l l a Negra.

A

'~77Lu

174

R A D I O A C T I V I T Y 162, , 1164W,166 6 3 167,168 169Re167168,16917OOs168,169,17OiTO172,1731rt75,176pt [from l°7,1°gAg,l°8,11°Cd,'133In,i12,lJaSn(63Cu,X)]; m e a s u r e d Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. RADIOACTIVITY 162,163,164 W,166,167,168,169Re,167,168,i 69,17°0s,168,169,17°,i 71,172,1731r,i 75,176p ~; measured Ea. S t a n d a r d 212Bi,z12Po s o u r c e c a l i b r a t i o n . REPT I P N O - R C - 8 1 - O 7 , D e l l a Negra.

A

176Hf

=

NUCLEAR REACTIONS 1 7 4 y b ( ~ , 4 n ) , E = 5 0 MeV; m e a s u r e d E T , I T , I ( c e ) , c e ( 0 ). 174Hf d e d u c e d high-spin transition 7-multipolarity. K-band deexcitation model,continuum s p e c t r a . REPT RCNP O s a k a , 1 9 8 1 A n n , P 1 2 7 , N a k a y a m a . R A D I O A C T I V I T Y l~l,t72,a73,174Pt [ f r o m n2Sn,U3In(63Cu,X)]; measured Ea,T1/2. H e l i u m j e t c o l l e c t i o n . REPT IPN 1981 A n n u a l , P R 5 , D e l l a Negra.

A

175pt

173

R A D I O A C T I V I T Y 173Lu; m e a s u r e d 7V(0); d e d u c e d Ae,A 4. 173yb t r a n s i t i o n s deduced 7-multipolarity,& CONF R i g a , P l l 8 , M u m i n o v . R A D I O A C T I V I T Y 173Lu; m e a s u r e d 77(0); deduced Aa,A 4. 17aYb t r a n s i t i o n s deduced 7-multipolarity,& CONF R i g a , P l l 8 , M u m i n o v . R A D I O A C T I V I T Y 162,1sa,164 W,166,167,168,169Re,167,166,169,17°0s,i 68,I 69,17°,170,172,1731 r,175,176p t [from l°7,1°gAg,l°8,ll°Cd,133In,lla,i16Sn(63Cu,X)]; measured Ea. REPT IPN 1981 A n n u a l , P R 5 , Della Negra. R A D I O A C T I V I T Y •62••63••64•••66••67••68••69Re••67••68••69••7•••••6•••69••7•••7•••72••73Ir••75••76Pt; measured Ea. S t a n d a r d ~IZBi,zt2Po s o u r c e c a l i b r a t i o n . REPT IPNO-RC-81-O7,Della N e g r a . R A D I O A C T I V I T Y 171,17a,173,174pt [ f r o m llaSn,ii31n(63Cu,X)~; measured E~,T~/2. H e l i u m j e t c o l l e c t i o n . REPT IPN 1981 Annual,PR5,Della N e g r a .

A

174Hf

=

ONLY)

=

177

R A D I O A C T I V I T Y 177mLu; m e a s u r e d I f l - , I ( e e ) . 177Hf,177Lu intensity ratios,-y-multipolarity. CONF R i g a , P 1 2 3 , E f r e m o v a . R A D I O A C T I V I T Y 177Lu(fl-); m e a s u r e d E v , I v , v T - c o i n . 177Hf ( g ( k ) - g ( R ) ) e / Q o a. REPT INS T o k y o 1981 A n n , P 3 1 , K u r i h a r a . R A D I O A C T I V I T Y 177mLu; m e a s u r e d I f l - , I ( c e ) . l~7Hf,t77Lu intensity ratios,~-multipolarity. CONF R i g a , P 1 2 3 , E f r e m o v a . R A D I O A C T I V I T Y 177Lu(fl-); m e a s u r e d E v , I v , v T - c o i n . 177Hf ( g ( k ) - g ( R ) ) e / Q o 2. REPT INS T o k y o 1981 A n n , P 3 1 , K u r i h a r a .

273

transitions deduced

transition

transitions deduced

deduced

intensities,

deduced

transition

subshell

subshell

intensities,

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A = *TaHf

R 79BoZE:

D 82KeZZ: R 79BoZD: 82NeZX:

8RVaZU:

~80Ta

R 81NoZX: 82DeZW:

1so w

R 80KoZK 81KoZU 82BeZJ

ISOOs

R 82NeZW

D 79ZaZW

lSlTa

D 79ZaZW: 82GuZZ:

~6~W

D 79SeZU: 8RGuZZ:

iS'Re

R 82BeZJ:

D 79BuZH: 81YoZX: R 82TsZZ:

102 W

D 79BuZH: R 81EoZU:

18aOs

D 81LiZT:

180

=

181

RADIOACTIVITY 181Hf; m e a s u r e d 77(0,T). lSlTa d e d u c e d e l e c t r i c f i e l d g r a d i e n t . S o u r c e i n HfO~. CONF R i g a , P 4 5 6 , Z a l y u b o v s k i j . RADIOACTIVITY lSlHf; m e a s u r e d 77(0,T). lSlTa d e d u c e d e l e c t r i c f i e l d g r a d i e n t . S o u r c e i n HfO 2. CONF R i g a , P 4 5 6 , Z a l y u b o v s k i j . RADIOACTIVITY iS'W; m e a s u r e d (K X - r a y ) ( K X - r a y ) - , 7 ( K X - r a y ) - c o i n . 'S'Ta l e v e l s d e d u c e d K-capture f e e d i n g p r o b a b i l i t i e s . BAPSA 27 5 2 2 , E Y a 7 , G u i m a . RADIOACTIVITY IS'W; m e a s u r e d I(K X - r a y ) , I T ; d e d u c e d Ifl+,log ft. Ge(Li) d e t e c t o r s . CONF Riga,P128,Sergienko. RADIOACTIVITY lSlW; m e a s u r e d (K X - r a y ) ( K X - r a y ) - , 7 ( K X - r a y ) - c o i n . 'SlTa l e v e l s d e d u c e d K-capture feeding probabilities. BAPSA 27 5 2 2 , E Y a 7 , G u i m a . NUCLEAR REACTIONS i~Gd~64~i88Er~i7sYb~17~1s0Hf~1~1~4W~1~7~i~8~'~9~'9~19~s~'94~19~Pt(1~C~F)'E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n or(E). 17°yb,176,1S°W,iaiRe,lSs,lSe0s,iOTIr,18s, 192Pt,194,196Hg,l~%~°°,~°l,~°~,~°4Pb,~°~,~°Po,~°~At deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n .

A lS2Ta

=

levels,J,zr. E n r i c h e d

RADIOACTIVITY 's°mHf(fl-); m e a s u r e d f l - d e c a y b r a n c h u p p e r l i m i t . A n t i c o i n c i d e n c e t e c h n i q u e . BAPSA 27 705,BC7,Kellogg. NUCLEAR REACTIONS l S ° H f ( n , n ' 7 ) , E = f a s t ; m e a s u r e d E%I% 'a°Hf d e d u c e d levels,J,~r. E n r i c h e d t a r g e t s , G e ( L i ) d e t e c t o r . CONF R i g a , P 1 2 6 , B o n d a r e n k o . NUCLEAR REACTIONS 's6,1~°Gd,lS~,lS~Dy,iS°Hf(4°Ar,~°Ar'),E n o t g i v e n ; m e a s u r e d ~(E); d e d u c e d ion-ion potential contours,radial,angular l o c a l i z a t i o n e f f e c t s . ~a°Hf d e d u c e d q u a d r u p o l e , hexadecapole moments. DABBB 42 3737,Neese. NUCLEAR REACTIONS 'S~W,~3~Th(d,~Li),E=45 MeV; m e a s u r e d a(E(SLi)), la°Hf d e d u c e d g r o u n d s t a t e r o t a t i o n a l b a n d . ~ S R a d e d u c e d p o s s i b l e m u l t i p l e t . REPT KVI 1981 A n n , P 2 0 , v a n d e n Berg. NUCLEAR REACTIONS 1 8 ° H f ( p , n ) , E = 8 - 9 MeV; m e a s u r e d ET,IT,77(t). lS°Ta d e d u c e d levels,T~/~. BAPSA 26 l l l S , A D 5 , N o r m a n . NUCLEAR REACTIONS 'SlTa(d,t),E n o t g i v e n ; m e a s u r e d a(O). lS°Ta d e d u c e d l e v e l s , r o t a t i o n a l bands,J,~r,Nilsson assignments,Gallagher-Moszkowski e n e r g y s p l i t t i n g . BAPSA 27 523,EYag, Dewberry. NUCLEAR REACTIONS ~S°W(SSKr,S~Kr'),E=340 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , T - d e c a y . 'SOW deduced yrast levels,J,rr,transition probabilities. REPT IPN 1980 A n n u a l , P N 2 5 , K o u k i o u . NUCLEAR REACTIONS ls°,lsa,'O4W(S~Kr,SSKr'),E=340 MeV; m e a s u r e d E T , I T , T S S K r - c o i n , C o u l o m b e x c i t a t i o n . 's°,la~,lS4W d e d u c e d r o t a t i o n a l b a n d s , B ( E 2 ) . REPT I P N O - T - 8 0 - 0 6 , K o u k i o u . NUCLEAR REACTIONS 1 ~ G d ~ 1 ~ 4 ~ s s E r ~ ' ~ s Y b ~ i 7 6 ~ ' ~ H f ' ~ 4 ~ 1 ~ 7 ~ i ~ s ~ ' ~ 9 ~ i 9 ~ s ~ 4 ~ 9 ~ P t ( ' ~ C ~ F ) ~ E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a(E). ~Toyb,l~s,1SOw,iS'Re,ia6,1aSOs,iSTIr,iSa, l~Pt,'~,l~SHg,~99,~°°,~°l,a°~,a°~Pb,~OS,~l°Po,~°9At deduced fission barrier. Statistical t h e o r y . REPT J I N R - P T - 8 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS 168Er('60,4n),E=83 MeV; m e a s u r e d I(ce). la°Os d e d u c e d l e v e l s , y r a s t b a n d , J , z ~ , K , I C C , c o n f i g u r a t i o n , g ( K ) . REPT J U L - S p e z - 1 4 6 , P 6 1 , N e s k a k i s .

A

ISiHf

178

NUCLEAR REACTIONS 17aHf(n,n'7),E=fast; m e a s u r e d E7,17. i~SHf d e d u c e d t a r g e t s , G e ( L i ) d e t e c t o r . CONE R i g a , P 1 2 4 , B o n d a r e n k o .

A teOHf

ONLY)

=

182

RADIOACTIVITY lS°Ho,17°,17aLu,lSZTa; m e a s u r e d I(ce). 16°Dy,17°,172yb,18ZW t r a n s i t i o n s d e d u c e d subshell intensity ratios. Double focusing spectrometer. CONF R i g a , P 2 3 8 , B u l g a k o v . RADIOACTIVITY lz4Sb,166mHo,182Ta; m e a s u r e d E T , r e l a t i v e I7. REPT N E A N D C ( J ) - 7 5 / U , P 2 1 , Yoshizawa. NUCLEAR REACTIONS 181Ta,Z38U(n,n),E=0.024-1 MeV; m e a s u r e d a ( t o t a l ) vs E. mZTa,239U d e d u c e d s-,p-,d-wave average resonance parameters. REPT N E A N D C ( J ) - 8 3 / U , P 1 4 , T s u b o n e . RADIOACTIVITY 16°Ho,17°,172Lu,lS2Ta; m e a s u r e d I(ce). 16°Dy,17°,lTZyb,isZW t r a n s i t i o n s d e d u c e d subshell intensity ratios. Double focusing spectrometer. CONF R i g a , P 2 3 8 , B u l g a k o v . NUCLEAR REACTIONS 18°,'8z,184W(SSKr,SSKr'),E=340 MeV; m e a s u r e d E T , I T , ~ S 6 K r - c o i n , C o u l o m b e x c i t a t i o n , i°°,Isa,lS4W d e d u c e d r o t a t i o n a l b a n d s , B ( E 2 ) . REPT I P N O - T - 8 0 - 0 6 , K o u k i o u . RADIOACTIVITY lSZOs [ f r o m lSOEr(laO,4n),(160,En),E=80 MeV]; m e a s u r e d 7 7 - c o i n , I ( c e ) , 7 ( 0 ) ; deduced levels,J,w,6,two-quasiparticle bands,backbending f r e q u e n c i e s . REPT J U L - S p e z 99, P56,Lieder.

274

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A ~BeOs

R 80LiZP:

NUCLEAR rotational

R 82MaZS:

IB3Au

D 81BoZL:

R 81KoZU: 82DaZU: 8aMaZS:

la4tr

D 80AbZQ:

R 81FIZW:

185 W

R 80BeYV: 83MaZS:

185Au

D 80AbZQ: 81BeYX: 81BoZJ: 82BoZY:

iOSHg

D

81BoZJ: 81BoZK: 83BoZY:

R 82BeZJ:

18OAu

D 80AbZQ: 81AbZT:

deduced

levels,

183

=

184

=

185

NUCLEAR REACTIONS 70Zn, 104 Ru, 110Pd, 154S m , 158, 160Gd, 186W, 196,198Pt, 202,204 Hg, 244 P u ( p o l a r l z e d t , a ) , 1 9 O P t , z 4 4 p u , T S G e ( p o l a r i z e d t , p ) , E = 1 7 MeV; 8 a , S ° S e , i ° ° M o , i a a , i a 4 S n ( p o l a r i z e d t,3He),E=23-25 MeV; m e a s u r e d a(0),analyzing p o w e r v s O,cr(Ea),a(Ep),a(aHe). 69Cu,l°3Tc,l°aRh,153pm,157,159Eu, la5Ta,lOS,197Ir,a°l,a°aAu,243Np,2°°Pt,a46pu,78Ge,B°,SaAs,i°°Nb,la2,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . NUCLEAR REACTIONS l°4W(n,T),E=5-a00 keV; m e a s u r e d a(E). l°Sw d e d u c e d r e s o n a n c e p a r a m e t e r s , average level spacing,effective nuclear r a d i u s . REPT K f K - 3 0 6 8 , P 1 6 , B e e r . NUCLEAR REACTIONS lsa,183,184,tOSW(n,v),E=3.6-2000 ke V ; m e a s u r e d G ( c a p t u r e ) v s E. l s 3 i s 4 1 s s , 187W d e d u c e d resonanees,Jjr,FT,resonance parameters. REPT L A - 9 2 0 0 - M S , M a c k l i n . R A D I O A C T I V I T Y 18s,18°,laSAu,ta41r; m e a s u r e d I(ee). O n - l i n e 180 o s p e c t r o g r a p h . REPT IPN 1980 Annual,PN38,Abreu. R A D I O A C T I V I T Y l°SAu E f r o m 185m,mSHg d e c a y ] ; m e a s u r e d Tl/a; d e d u c e d M1 t r a n s i t i o n h i n d r a n c e , intraband E2 t r a n s i t i o n strength. REPT IPN 1981 A n n u a l , P 4 2 , B e r g . R A D I O A C T I V I T Y 1BSm,lSSHg; m e a s u r e d l(ce),vT(t), taSAu deduced transitions,d,shape coexistence. REPT IPN 1981 A n n u a l , P N 4 1 , B o u r g e o i s . R A D I O A C T I V I T Y 185m,185Hg ~ f r o m Au(p,xn),E=300 MeV]; measured E-/,I~,I(ce),v-y-, 7(X-ray)-coin. '85mHg d e d u c e d IT b r a n c h i n g , lSSHg d e d u c e d l e v e l s , lSSAu d e d u c e d l e v e l s , J j r , ICC,-/-multipolarities. Ge(Li),hyperpure Ge,Si-Li detectors,magnetic spectrograph. REPT IPNO-DRE-82-09,Bourgeois. R A D I O A C T I V I T Y l°5m,lOSHg; m e a s u r e d I(ce),Tv(t). 185Au d e d u c e d transitions,8,shape coexistence. REPT IPN 1981 A n n u a l , P N 4 1 , B o u r g e o i s . R A D I O A C T I V I T Y 185mHg; m e a s u r e d I(ee); d e d u c e d i s o m e r d e c a y c h a r a c t e r i s t i c s , T - b r a n c h i n g , 7-multipolarity,6,possible Jjr,rotational b a n d . REPT IPN 1981 A n n u a l , P N 3 9 , B o u r g e o i s . RADIOACTIVITY l°5m,lsSHg [from Au(p,xn),E=200 MeV]; measured EV,I-/,I(ce),vT-, T(X-ray)-coin. 185mHg d e d u c e d IT b r a n c h i n g . ~85Hg d e d u c e d l e v e l s . ~SSAu d e d u c e d levels,J,~r, ICC,T-multipolarities. Ge(Li),hyperpure Ge,Si-Li detectors,magnetic spectrograph. REPT IPNO-DRE-82-09,Bourgeois.

A 1860s

=

~aaOs

NUCLEAR REACTIONS l°°,18a,la4W(86Kr,SSKr'),E=340 MeV; m e a s u r e d Ev,I%vSSKr-coin,Coulomb excitation, ls°,ls2,1S4W d e d u c e d r o t a t i o n a l b a n d s , B ( E 2 ) . REPT I P N O - T - 8 0 - 0 6 , K o u k i o u . NUCLEAR REACTIONS t a a W ( n , ~ ) , E = t h e r m a l ; m e a s u r e d ET,I T. ~S~W d e d u c e d l e v e l s , 7 - b r a n c h i n g , B(E2),band structure. Curved-crystal spectrometer. REPT J U L - S p e z - 1 4 6 , P 6 8 , D a v i d s o n . NUCLEAR REACTIONS ~sa,~s3,1s4,1S~W(n,T),E=2.6-20O0 ke V ; m e a s u r e d c ~ ( c a p t u r e ) v s E. ~03~o¢1s5 ~aTW d e d u c e d resonances,Jjr,FT,resonance parameters. REPT L A - 9 3 0 O - M S , M a e k l i n . R A D I O A C T I V I T Y le5,is~,lSSAu,lS4Ir; m e a s u r e d I(ce). O n - l i n e 1800 s p e c t r o g r a p h . REPT IPN 1980 Annual,PN38,Abreu.

A i85Ta

continued

NUCLEAR REACTIONS 182,183,184,186W(n,'y),E=2.6-~000 k e Y ; m e a s u r e d a ( c a p t u r e ) v s E. i s a i a h - ~ 5 l°7W d e d u c e d r e s o n a n c e s , J , ~ r , F v , r e s o n a n c e parameters. REPT L A - 9 2 0 0 - M S , M a e k l i n . R A D I O A C T I V I T Y 'SaAu [ f r o m Pt(p,xn),E=~00 MeV]; m e a s u r e d E%I% REPT IPN 1981 Annual,PN38, Bourgeois.

A t84 W

182

REACTIONS l ~ S E r ( ~ ° O , 4 n ) , E = 8 1 MeV; m e a s u r e d ~T-coin. b a n d s . NaI,Ge d e t e c t o r s . REPT J U L - S p e z - T a , P 4 8 , L i e d e r .

A is3 W

=

ONLY)

=

186

NUCLEAR REACTIONS 158 Gd, 164 , 168 Er, 176 Yb, 176 , 180 Hf, 182 , 184 W . 187. 188 . .1 8 9. 190 192 Os, 194 , 198 P t ( 13C,F),E 6 8 - 1 0 6 MeV; m e a s u r e d g(fragment 0 ) , f i s s i o n a ( E ) . 17°yb,17s,ls°W,iSlRe,lSs,lUSOs,iaTIr,la8, 192pt,lo4,1OOHg,ioo,z°°,2°i,a°a,a°4pb,a°o,al°Po,a°OAt deduced fission barrier. Statistical theory. REPT J I N R - P 7 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y la5,1a6,1°8Au,iS41r; m e a s u r e d I(ce). O n - l i n e 1800 s p e c t r o g r a p h . REPT IPN 1980 Annual,PN38,Abreu. R A D I O A C T I V I T Y laSHg; m e a s u r e d ( c e ) ( c e ) ( t ) , ( c e ) ( X - r a y ) ( t ) . 186Au l e v e l s d e d u c e d TI/a,B(X),6. REPT IPN 1981 A n n u a l , P N 4 5 , A b r e u .

275

SECONDARY

SOURCES

(Reports,Abstracts,e~c.

A iO6Au

D 81BoZI:

186Hg

D 81AbZT: 81BoZI:

R 82MaZS:

lSTlr

R 82BeZJ:

~S~Pt

D 81GnZZ:

i87Au

D 81BrZX: 81GnZZ:

R 81KaZH: 82BeZJ:

82CaZX:

~08pt

R 82BeZJ:

ISaAu

D 80AbZP: 80AbZQ: 82NeZU:

tSSHg

D 80AbZP:

D 81BeYW:

189Au

D 81BeYW:

R 79FuZN:

19OAu

D 80AbZP:

187

=

188

=

189

R A D I O A C T I V I T Y 189m,189Au; m e a s u r e d 1981 A n n u a l , P N 4 6 , B e r g . R A D I O A C T I V I T Y 189m,189Au; m e a s u r e d 1981 A n n u a l , P N 4 6 , B e r g .

A tOOpt

=

NUCLEAR REACTIONS l e T O s , 1 9 5 p t ( n , e ) , ( n , 7 ) , E = t h e r m a l ; measured a ( E ( e ) , E T , I T ) . 180Os,196Pt deduced 0+ states,E0 transitions. Interacting b o s o n m o d e l . B A P S A 26 l l l 7 , A D 8 , K a n e . NUCLEAR REACTIONS 158Gd~4~16~Er~176Yb~17~i~Hf~1~2~i~4W~7~i~1~9~t9~192~s~i94~i9~Pt(12C~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . 17°yb,170,l°°W,lelRe,lSS,lSBOs)SVIr, 188, 192Pt,i94,196Hg,~99,2°o,a°l,2°2,2°4pb,2°6,21°Po,a°gAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - O 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS l S T 0 s ( n , X ) , E = 0 . 0 0 2 7 - 2 0 0 k e V ; m e a s u r e d a ( t o t a l ) v s E. leSOs d e d u c e d resonances,resonance parameters,s-wave strength function,level spacing. Tof,enriched t a r g e t . B A P S A 27 5 4 3 , G Y a 8 , C a r l t o n . NUCLEAR REACTIONS ~58Gd~1~4~t6~Er~76Yb~17s~1e~Hf~2~184W~87~8~89~9~'19a~s~94~19~Pt(12C~F)~E 6 8 - 1 0 8 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . 17°yb,i76,18ow,181Re,lS~,1aSOs,lSTIr,iSs, 19apt,194,196Hg,199,a°°,2°t,2°a,a°4pb,206,21°po,2°gAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y 180,lg°Hg [ f r o m A u ( p , x n ) , E = 2 O 0 MeV]; m e a s u r e d ( c e ) ( c e ) - , ( c e ) ~ / - c o i n . lss,19°Au l e v e l s d e d u c e d TI/a,M1,E2 t r a n s i t i o n hindrance f a c t o r s . REPT IPN 1980 A n n u a l , P N 3 9 , A b r e u . R A D I O A C T I V I T Y ~s5,~8~,~aSAu,la4Ir; m e a s u r e d I(ce). 0 n - l i n e 1800 s p e c t r o g r a p h . REPT IPN 1980 Annual,PN38,Abreu. R A D I O A C T I V I T Y ~SeAu [ f r o m ~ 9 ~ I r ( a , T n ) , E = 9 0 MeV]; d e d u c e d levels,~/-branching,band configurations. E n r i c h e d Ir t a r g e t , i n - b e a m s p e c t r o s c o p y . REPT J U L - S p e z - 1 4 6 , P 6 7 , N e s k a k i s . R A D I O A C T I V I T Y ~as,l°°Hg [ f r o m A u ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d (ce)(ee)-,(ce)3~-coin. 18a,i~6Au l e v e l s d e d u c e d T~/2,M1,E2 t r a n s i t i o n hindrance f a c t o r s . REPT IPN 1980 A n n u a l , P N 3 9 , A b r e u .

A

189pt

continued

NUCLEAR REACTIONS ls~,ls3,184,186W(n,7),E=2.6-2000 keV; m e a s u r e d c r ( c a p t u r e ) v s E. 1~3~4 ~85 ~STW d e d u c e d r e s o n a n e e s , J , r r , F T , r e s o n a n c e parameters. REPT L A - 9 2 0 O - M S , M a c k l i n . NUCLEAR REACTIONS ~ 5 ~ G d ~ i ~ 4 ~ 1 6 ~ E r ~ 7 ~ Y b ~ 7 ~ e ~ H f ~ i ~ a ~ i 8 4 ~ i ~ 8 ~ i ~ i ~ a ~ s ~ i 9 4 ~ i 9 8 P t ( ~ a C ~ F ) ~ E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . 17°Yb,~,~8°W,lS~Re,iS~,~SSOs,tSVIr,lSS, ~°apt,104,~96Hg,i99,2°o,2°~,a°~,~°4pb,~°6,21°Po,a°9At deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y 1BTAu [ f r o m T a ( ~ C , X ) , E = 1 0 0 MeV; Hf(14N,X),E=103 MeV]; m e a s u r e d 3'7(t), ce-/(t). ~ÜTpt d e d u c e d l e v e l s . B A P S A 26 1 1 1 6 , A D 6 , G n a d e . RADIOACTIVITY 187mAu [ f r o m H f ( ~ N , 5 n ) ] ; m e a s u r e d T~/a. Digitized t i m e p u l s e e n e r g y e v e n t coincidence. B A P S A 26 1 1 1 7 , A D 7 , B r a g a . R A D I O A C T I V I T Y laTAu [ - f r o m Ta(laC,X),E=100 MeV; Hf(14N,X),E=103 MeV]; m e a s u r e d 77(t), ce-/(t). ~S~Pt d e d u c e d l e v e l s . B A P S A 26 1 1 1 6 , A D 6 , G n a d e .

A

~O0s

186

R A D I O A C T I V I T Y 'aSHg; m e a s u r e d ~/-,7(X-ray)-coin,~-~(t),7(X-ray)(t),(ce)(ce)(t),(ee)~/(t). ~8~Au d e d u c e d levels,J,~,shape coexistence,prolate,oblate deformations. REPT IPN 1981 Annual,PN44,Bourgeois. R A D I O A C T I V I T Y 10SHg; m e a s u r e d ( c e ) ( c e ) ( t ) , ( c e ) ( X - r a y ) ( t ) . ~°SAu l e v e l s d e d u c e d Ti/a,B(X),6. REPT IPN 1981 A n n u a l , P N 4 5 , A b r e u . R A D I O A C T I V I T Y laSHg; m e a s u r e d ~/7-,7(X-ray)-coin,~/(t),7(X-ray)(t),(ce)(ee)(t),(ee)~/(t). 18~Au d e d u c e d levels,Jjr,shape coexistence,prolate,oblate deformations. REPT IPN 1981 Annual,PN44,Bourgeois.

A 187 W

=

ONLY)

=

I(ce). 189pt d e d u c e d

levels,band

structure.

REPT IPN

I(ce). 189Pt d e d u c e d

levels,band

structure.

REPT IPN

190

NUCLEAR REACTIONS 188,19°,1°aOs(a,2n),E=27 MeV; m e a s u r e d E3,,I7,7(0). 19°,l°a,194pt l e v e l s . d e d u c e d ~,B(E2) r a t i o s . REPT Z F K - 3 8 5 , P 5 2 , F u n k e . R A D I O A C T I V I T Y tss,19°Hg [ f r o m A u ( p , x n ) , E = 2 0 0 MeV]; m e a s u r e d ( c e ) ( c e ) - , ( c e ) ~ / - e o i n . 18s,19°Au l e v e l s d e d u c e d TI/a,MI,E2 t r a n s i t i o n hindrance f a c t o r s . REPT IPN 1980 A n n u a l , P N 3 9 , A b r e u .

276

SECONDARY

SOURCES

(Reports,Abskraets,ekc.

A 16OHg

D

80AbZP:

D 82LiZV:

191Hg

D 82LiZV

R 79FuZN 82BeZJ

D 82LiZV

=

191

=

192

NUCLEAR REACTIONS 1 2 6 , 1 9 0 , 1 9 2 0 s ( a , 2 n ) , E - 2 7 MeV; m e a s u r e d EV,I-/,~/(0). 190,192,194pt l e v e l s d e d u c e d 6,B(E2) r a t i o s . REPT Z F K - 3 8 5 , P 5 2 , F u n k e . NUCLEAR REACTIONS 15~Gd~4~08Er,17~Yb~170,18~Hf~s~184W~1~7~1s~,169~19~,19~s~1~4~1~6Pt(1~C~F),E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n or(E). 170Yb,170,lS°W,101Re,126,12BOs,tSVlr,188, 16aPt,194,19°Hg,la9,zo°,2°l,a°2,a64pb,a°6,al°Po,2°6At deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n .

A 193Au

continued

RADIOACTIVITY 197,195,193,161Hg [ f r o m 1 6 4 p t ( a , x n ) ] ; m e a s u r e d NMR o n o r i e n t e d n u c l e i . 197195 193,191Au l e v e l d e d u c e d /*. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t . R A D I O A C T I V I T Y 1°7,195,199,1mHg [ f r o m 1 6 4 p t ( a , x n ) ] ; m e a s u r e d NMR on o r i e n t e d n u c l e i . 197,190 199,191Au l e v e l d e d u c e d /*. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t .

A 16apt

190

R A D I O A C T I V I T Y lss,16°Hg [ f r o m A u ( p , x n ) , E = a 0 O MeV]; m e a s u r e d ( c e ) ( e e ) - , ( c e ) - / - c o i n . las,19°Au l e v e l s d e d u c e d TI/2,M1,EE t r a n s i t i o n hindrance f a c t o r s . REPT IPN 1980 A n n u a l , P N 3 9 , A b r e u .

A

191Au

=

ONLY)

=

193

197,195,193,191Hg [ f r o m 1 9 4 p t ( a , x n ) ] ; m e a s u r e d NMR on o r i e n t e d n u c l e i . 167 165 l e v e l d e d u c e d N. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t . R A D I O A C T I V I T Y 16~,195,193,1mHg [ f r o m 104P t (a ,xn)3; m e a s u r e d NMR o n o r i e n t e d n u c l e i . 197165 193,191Au l e v e l d e d u c e d /~. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t . NUCLEAR REACTIONS l s 4 , 1 8 Z W ( 1 0 0 , 5 n ) , ( l ° O , 4 n ) , ( 1 0 0 , 6 n ) , E = 1 0 3 MeV; m e a s u r e d 77(t), `/(X-ray)-coin. 195,193pb d e d u c e d l e v e l s , d e c a y c h a r a c t e r i s t i c s . 194pb d e d u c e d l e v e l s , d e c a y characteristics,T1/2. REPT IPN 1981 A n n u a l , P N 5 5 , A l b o u y . NUCLEAR REACTIONS 10a,124W(160,4n),(lOO,5n),E=100 MeV; le4W(100,6n),E=t00 MeV; 122W(100,6n), ( 1 2 0 , 5 n ) , E = 1 0 5 MeV; m e a s u r e d E%I`/,`/`/(0),I(ce),E(X-ray),I(X-ray),`/`/-,`/(X-ray)-coin. 105pb deduced levels,T-branching,T-multipolarity,J,vr,d,T~/2. 194pb d e d u c e d levels,Tl/a,J,Tr, -/-branching. lgapb deduced levels,J,~rF/-multipolarity,~/-branching. REPT I P N O - T - 8 2 - 0 1 , Albin. RADIOACTIVITY

163,161Au

iSaHg

D 82LiZV

193pb

R 81AIZP

82AIZY

A 164pt

R 79FuZN 80BeYT: 81VeZZ:

82B1ZX

194Hg

R 82BeZJ

194pb

R 81A1ZP

82A1ZY

82VaZT

=

194

NUCLEAR REACTIONS l s s , t s ° , l S Z O s ( a , 2 n ) , E = 2 7 MeV; m e a s u r e d E%I`/,`/(0). 190 19a,104pt l e v e l s d e d u c e d d,B(E2) r a t i o s . REPT Z F K - 3 8 5 , P 5 2 , F u n k e . NUCLEAR REACTIONS 193Ir(aHe,d),E=36 MeV; m e a s u r e d cr(Ed),~(0), lg4Pt l e v e l s d e d u c e d S. DWBA a n a l y s i s . REPT IPN 1980 A n n u a l , P N 1 7 , B e r r i e r - R o n s i n . NUCLEAR REACTIONS 193Ir(SHe,d),E=25.5,36 MeV; ' 9 3 I r ( a , t ) , E = 2 7 MeV; m e a s u r e d cT(Ed),cr(Et). 194Pt l e v e l s d e d u c e d s u p e r s y m m e t r y s e l e c t i o n r u l e b r e a k d o w n . REPT IPN 1981 A n n u a l , P N 3 2 , Vergnes. NUCLEAR REACTIONS l°31r(d,aHe),(3He,d),E=40 MeV; m e a s u r e d ~(O); d e d u c e d s u p e r s y m m e t r y s c h e m e v a l i d i t y . 194pt d e d u c e d l e v e l , L , p o s s i b l e J,rr. DWBA a n a l y s i s . REPT KVI 1981 A n n , P 2 3 , Blasi. NUCLEAR REACTIONS 15s Gd, 164 , 168 Er, 176 Yb, 176 , 180 Hf, 182 , 104 W . ls7. i06 . .las. 19o lg~ Os, 164 , i66 P t ( 12C,F),E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n cr(E). 170yb,170,180W,101Re,laa,1260s,107ir,188, 192 P t , 194 , 196 Hg . 199. e00 . .a01. 202 804 P b , 206 , 210 P o, 206 A t d e d u c e d fission barrier. Statistical theory. REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS l e 4 , 1 0 2 W ( 1 6 0 , 5 n ) , ( 1 0 0 , 4 n ) , ( 1 0 0 , 6 n ) , E = 1 0 3 MeV; m e a s u r e d ~/T(t), "/(X-ray)-coin. 195,193pb d e d u c e d l e v e l s , d e c a y c h a r a c t e r i s t i c s . 194Pb d e d u c e d l e v e l s , d e c a y characteristics,T1/2. REPT IPN 1981 A n n u a l , P N 5 5 , A l b o u y . NUCLEAR REACTIONS 10a,lS4W(160,4n),(160,5n),E=100 MeV; 184W(100,6n),E=100 MeV; 122W(160,6n), ( 1 0 0 , 5 n ) , E = 1 0 5 MeV; m e a s u r e d ET,I`/,`/`/(0),I(ce),E(X-ray),I(X-ray),`/`/-,v(X-ray)-eoin. 165Pb deduced levels,`/-branehing,`/-multipolarity,J,rr,6,T1/2. 194pb d e d u c e d levels,Tl/a,JDr, `/-branching. 190pb d e d u c e d l e v e l s , J , ~ r , ` / - m u l t i p o l a r i t y , ` / - b r a n e h i n g . REPT I P N O - T - 8 2 - 0 1 , Albin. NUCLEAR REACTIONS 102Os(12C,xn),E=75,100 MeV; m e a s u r e d E ` / , I % ` / ` / - e o i n , - / ( 0 ) , I ( c e ) . 194,19°Pb deduced yrast levels,J,isomer TI/2. REPT KVI 1981 A n n , P 4 8 , v a n Nes.

277

SECONDARY

SOURCES ( R e p o r t s , A b s t r a c t s , e t c .

A ~95ir

R 81F1ZW:

t95Au

D 82LiZV:

~gSHg

D 82LiZV:

195pb

D 80A1ZS R 81A1ZP

82AIZY

=

R 81KaZR: 81VeZY:

t96Hg

R 82BeZJ:

196pb

R 82VaZT:

tSSTa,lOs,lSTlr,2Sl,2°3Au,243Np,Z°°Pt,a46Pu,VSGe,S°,82As,t°SNb,122,~24In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . RADIOACTIVITY 197,195,193,tmHg [ f r o m 194Pt(a,xn)]; m e a s u r e d NMR o n o r i e n t e d n u c l e i . 197195 193,19iAu l e v e l d e d u c e d /~. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t . RADIOACTIVITY 197,195,193,1mHg [ f r o m 194pt(a,xn)3; m e a s u r e d NMR o n o r i e n t e d n u c l e i . 197195 193,191Au l e v e l d e d u c e d /~. Recoil i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t . RADIOACTIVITY 195pb [ f r o m 185W(lsO,5n)3; m e a s u r e d 7 - / ( X - r a y ) - c o i n , r e c o i l . REPT IPN 1980 Annual,PN25,Albouy. NUCLEAR REACTIONS l s 4 , i a e w ( l S O , 5 n ) , ( 1 6 0 , 4 n ) , ( l S O , 6 n ) , E = 1 0 3 MeV; m e a s u r e d ~/7(t), 7(X-ray)-coin. t9s,193pb d e d u c e d l e v e l s , d e c a y c h a r a c t e r i s t i c s . 194Pb d e d u c e d l e v e l s , d e c a y characteristics,Tl/2. REPT IPN 1981 A n n u a l , P N 5 5 , A l b o u y . NUCLEAR REACTIONS 182,184W(lsO,4n),(160,5n),E=100 MeV; 184W(/sO,6n),E=100 MeV; 182W(160,6n), (lSO,5n),E=105 MeV; m e a s u r e d E%I%-/7(0),I(ce),E(X-ray),I(X-ray),7-y-,-/(X-ray)-coin. tgSPb deduced levels,7-branching,7-multipolarity,J,rr,6,T1/2. 194pb d e d u c e d levels,Tl/a,J,~r, v-branching. 193pb d e d u c e d l e v e l s , J , T r , v - m u l t i p o l a r i t y , 7 - b r a n c h i n g . REPT I P N O - T - 8 2 - 0 1 , Albin.

R 81FIZW:

196

NUCLEAR REACTIONS l S T O s , l O 5 p t ( n , e ) , ( n , 7 ) , E = t h e r m a l ; m e a s u r e d a ( E ( e ) , E T , I T ) . 1880s,196pt deduced 0 + states,E0 transitions. Interacting b o s o n m o d e l . BAPSA 26 l l l 7 , A D S , K a n e . NUCLEAR REACTIONS 197Au(d,aHe),E=108 MeV; m e a s u r e d ff(E(3He)). 196pt l e v e l s d e d u c e d CaS, supersymmetry s e l e c t i o n r u l e v a l i d i t y . REPT IPN 1981 A n n u a l , P N 3 3 , V e r g n e s . NUCLEAR REACTIONS ~58Gd~164~168E~176Yb~7~8~Hf~182~84~187~188~9~t9~192~194~19~P~(~2C~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d ~(fragment 0 ) , f i s s i o n a ( E ) . tv°Yb,176,1SSw,lelRe,la6,1880s,laTIr,iS8, 192pt,la4,tO6Hg,199,2°°,a°l,2°2,a°aPb,2°%alSpo,2°9At deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS 1aaOs(12C,xn),E=75,100 MeV; m e a s u r e d ET,IT,~/7-coin,7(0),l(ce). 194,lasPb d e d u c e d y r a s t l e v e l s , J , i s o m e r TI/2. REPT KVI 1981 A n n , P 4 8 , v a n Nes.

A 197ir

195

N U C L E A R R E A C T I O N S 7°Zn,l°4Ru,u°pd,154Sm,iSs,lS°Gd,lsSW,tgs,lOSPt,2°2,2°4Hg,244pu(polarized t,a), 198Pt,244Pu,TSGe(polarized t,p),E=17 MeV; 82,8°Se,l°°Mo,122,124Sn(polarized t,SHe),E=22-25 MeV; m e a s u r e d a(0),analyzing power vs 0,a(Ea),a(Ep),~(3He). SSCu,t°aTc,1°gRh,lS3pm,lST,iSgEu,

A =

196pt

ONLY)

=

197

N U C L E A R R E A C T I O N S 7°Zn 1°4Ru u°pd t54Sm 15s 160Gd 186 w 196 t9Spt 202 aO4Hg 244pu(polarized t,a), ~gSpt,244pu,VSGe(polarized t,p),E=17 MeV; s2,SOSe,i°°Mo,122,124Sn(polarized t,aHe),E=22-25 MeV; m e a s u r e d a(0),analyzing power vs 0,a(Ea),a(Ep),a(3He). SgCu,tO3Tc,i°gRh,153Pm,lST,159Eu, lS5Ta,195,/97ir,aOl,2OaAu,24aNp,aOOpt,246pu,78Ge,SO,SaAs,lOONb,122,124in

197Au

D 82LiZV: R 80LeZK:

81DjZT:

I97Hg

D 82LiZV:

A 198Au

D 82WhZY:

198Hg

R 82B1ZY:

deduced

mass

e x c e s s . CONF

H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . RADIOACTIVITY 197,195,193,191Hg [ f r o m 194pt(a,xn)]; m e a s u r e d NMR o n o r i e n t e d n u c l e i . 197 195 193,191Au l e v e l d e d u c e d p . R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 l , L i g t h a r t . NUCLEAR REACTIONS 6°Ni, 90 Zr, 115 I n , 120 S n , 144 S i n , 165 Ho, 197 A u , 208 P b ( 3 He, 3 H e ' ) , E = 1 0 8 . 5 MeV; m e a s u r e d ff(E(3He)),ff(0). 6°Ni d e d u c e d GQR,F. 9OZr,U5In,12°Sn,144Sm,lSSHo,197Au d e d u c e d GQR, g i a n t m o n o p o l e r e s o n a n c e , F . REPT ISN 8 0 - 0 1 , P 4 2 , L e b r u n . NUCLEAR REACTIONS 2 ° s P b , l O T A u , l a ° S n ( p , p ' ) , E = 2 0 1 MeV; m e a s u r e d a ( E p ' ) , G ( 0 ) . 197Au,la°Sn d e d u c e d g i a n t r e s o n a n c e F. 2°8Pb d e d u c e d g i a n t r e s o n a n c e , F , T , v - m u l t i p o l a r i t y . REPT IPN 1981 A n n u a l , P N 5 8 , D j a l a l i . RADIOACTIVITY 197,195,193,1mHg [ f r o m l ° 4 p t ( a , x n ) 3 ; m e a s u r e d NMR on o r i e n t e d n u c l e i . ,97,195 193,191Au l e v e l d e d u c e d /~. R e c o i l i m p l a n t a t i o n i n Fe. REPT KVI 1981 A n n , P 6 1 , L i g t h a r t .

=

198

RADIOACTIVITY 198Au(fl-); m e a s u r e d d e c a y r a t e v s s o u r c e a c c e l e r a t i o n ; d e d u c e d p o s s i b l e gravitation,nuclear p r o c e s s d i r e c t c o u p l i n g e v i d e n c e . REPT L A - 9 3 8 8 - M S , W h i t a k e r . NUCLEAR REACTIONS ~9~Au(3He,d),E=50 MeV; m e a s u r e d a ( E d ) , a ( 0 ) ; d e d u c e d s u p e r s y m m e t r y scheme nonvalidity. 19aHg l e v e l s d e d u c e d L. REPT KVI 1981 A n n , P 2 2 , B l a s i .

278

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A i99pb

R 82BeZJ:

199Bi

D 82PiZZ:

R 81FIZW:

aoOpb

R 82BeZJ:

R 81F1ZW

2OiT1

R 82BUZZ

aolpb

R 82BeZJ

aOiBi

D 81BeYV 82PiZZ

R 82BUZZ

aoapb

R 82BeZJ

aoaBi

D 8OKIZX: R 80ThZZ:

SeaT1

R 81F1ZW:

R 82BUZZ:

=

201

=

203

NUCLEAR REACTIONS a ° T p b ( ~ - , x n ) , E at r e s t ; m e a s u r e d n e u t r o n m u l t i p l i c i t y . 2oi,aoa,zo3,2e4,zos, a°s,aO7T1 d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,eoaxial lithium drifted Ge d e t e c t o r s . B A P S A 27 5 2 9 , G E 1 , B u d i e k . NUCLEAR REACTIONS i5~Gd~i54~168Er~17~Yb~176~8~Hf~1sa~1~4~7~isa~189~19~i9a~s~i~4~i9~Pt(12C~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . l~°Yb,176,18°W,iSlRe,lSs,i880s,iS~Ir,188, 19apt,194,196Hg,199,2°°,a°l,2°a,a°4pb,a°s,2i°po,2°SAt d e d u c e d fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y a°a,a°4Bi [ f r o m a°3Tl(a,5n),E=65 MeV; Z°STl(c~,3n),E=40.4 MeV]; m e a s u r e d ET,IT, 7 ( H , t ) . 2°2,2°~Bi l e v e l s d e d u c e d g. E n r i c h e d t a r g e t . REPT J U L - S p e z - 7 2 , P 6 1 , K l e i n r a h m . NUCLEAR REACTIONS Z ° 3 T l ( a , 5 n ) , E - 6 6 MeV; m e a s u r e d a(ET),T(0),TT(t),Ta(t),I(ce), a°eBi deduced levels,J,~,T1/a,7-multipolarity. REPT J U L - S p e z - 7 2 , P 6 O , T h i r u m a l a Rao.

A 2OaAu

200

NUCLEAR REACTIONS 7°Zn,i°4Ru,u°Pd,154Sm,15s,16OGd,186W,las,laSpt,a°a,2°4Hg,a44pu(poiarized t,a), 198pt,Z44pu,76Ge(polarized t , p ) , E = 1 7 MeV; s z , S ° S e , i ° ° M o , t a a , l a 4 S n ( p o l a r i z e d t,SHe),E=22-25 MeV; m e a s u r e d a(0),analyzing p o w e r v s 0 , a ( E a ) , a ( E p ) , a ( a H e ) . 69Cu,l°aTc,i°SRh,153pm,15~,lSSEu, lS5Ta,195,197Ir,a°l,a°3Au,a43Np,Z°°Pt,a46pu,TaGe,8°,SaAs,l°°Nb,*aa,ia4In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V e i l P107, CERN 8 1 - 0 9 . NUCLEAR REACTIONS a°~Pb(~t-,xn),E a t r e s t ; m e a s u r e d n e u t r o n m u l t i p l i c i t y , zm,20a,aoa,ao~,a05 a°6,~e7T1 d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,coaxial lithium drifted Ge d e t e c t o r s . B A P S A 27 5 2 9 , G E i , B u d i c k . NUCLEAR REACTIONS i ~ 8 G d ~ i ~ 4 ~ 6 s E r ~ i 7 ~ Y b ~ 7 6 ~ 8 ~ H f ~ 8 a ~ i 8 4 W ~ 7 ~ i ~ i ~ 9 z ~ s ~ i ~ 4 ~ i 9 8 P t ( i a C ~ F ) ' E 6 8 - 1 0 6 MeV; m e a s u r e d ~(fragment 0 ) , f i s s i o n a ( E ) . l~°yb,~s,~SOw,~8*Re,18~,lSSOs,~S~Ir,188, 19apt,194,~S~Hg,i99,a°°,z°i,a°~,Zo4pb,z°~,~*OPo,~°SAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P T - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y z°7,~°5,z°3,a°lBi [ f r o m Po d e c a y ] ; m e a s u r e d (ce)(ce)-,(ce)7-eoin. 2o7 zo5 ~o3 2°iBi l e v e l s d e d u c e d T w a , v - m u l t i p o l a r i t y , B ( X ) . REPT IPN 1981 A n n u a l , P N 4 7 , B e r g . R A D I O A C T I V I T Y 199,Z°lBi [ f r o m i94,196pt(~°B,5n)]; m e a s u r e d isomer TWa,V(0,H,T). iS~Bi deduced i s o m e r g. B A P S A 27 522 E Y a 8 , P i e l .

A SeaT1

=

NUCLEAR REACTIONS V°Zn,~°4Ru,u°Pd,*54Sm,~58,~6°Gd,18~W,lS6,19Spt,Z°a,a°4Hg,a44pu(polarized t,a), ~96pt,a44pu,76Ge(polarized t , p ) , E = 1 7 MeV; s z , S ° S e , ~ ° ° M o , l a a , l Z 4 S n ( p o l a r i z e d t,3He),E=22-25 MeV; m e a s u r e d a(0),analyzing p o w e r v s O,cr(E~),a(Ep),cr(SHe). 69Cu,*°STc,i°SRh,~53pm,157,15SEu, lSSTa,iSs,ls7Ir,ao*,a°SAu,a43Np,2°°Pt,a46pu,7SGe,8°,8~As,l°°Nb,iaa,iZ4In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P I 0 7 , CERN 81 09. NUCLEAR REACTIONS *58Gd'*64'~68Er'i7~Yb~i76~8~Hf'i8a~84w~i87'i8s~i89~i9~9~Os~i94~s~t(i~C'F)~E 6 8 - 1 0 6 MeV; m e a s u r e d or(fragment 0 ) , f i s s i o n ~(E). ~°Yb,~Ts,~8°W,iSlRe,186,~SSOs,*S7Ir,~Ss, 19~pt,184,~S6Hg,*99,a°°,z°i,aoa,a°4Pb,Z°~,Zl°Po,Z°SAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n .

A aOlAu

199

NUCLEAR REACTIONS ~ 5 8 G d ~ 6 4 ~ i ~ 8 E r ~ 7 6 Y b ~ i 7 a ~ i ~ H f ~ i 8 a ~ s 4 W ~ s 7 ~ 1 ~ 8 ~ i 9 ~ 9 z ~ s ~ i 9 4 ~ 9 8 P t ( 1 ~ C ~ F ) ~ E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n or(E), iT°yb,i7s,iaOw,181Re,iS~,~SSOs,187Ir, ~ss, 19apt,i94,~9~Hg,isa,z°°,a°l,a°e,ao~pb,a°~,a~Opo,a°SAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . R A D I O A C T I V I T Y ~99,~°*Bi [ f r o m ~94,196Pt(~°B,5n)3; m e a s u r e d isomer T I / ~ , 7 ( 0 , H , T ) . t"SBi d e d u c e d i s o m e r g. B A P S A 27 522 E Y a 8 , P i e l .

A ZOOpt

=

ONLY)

=

203

NUCLEAR REACTIONS 7°Zn,l°4Ru,u°pd,lS4Sm,15a,16°Gd,186w,i96,iSSpt,a°a,a°4Hg,a44pu(polarized t,a), 19SPt,z44pu,76Ge(polarized t,p),E-17 MeV; s a , S ° S e , l ° ° M o , l Z a , 1 2 4 S n ( p o l a r i z e d t , 3 H e ) , E = 2 3 25 MeV; measured a(0),analyzing power vs 0,~;(Ea),G(Ep),a(aHe). 69Cu,l°aTc,l°9Rh,153pm,i57,159Eu, 185Ta,~95,1971r,a°l,a°3Au,Z43Np,2°°Pt,a46pu,78Ge,a°,aZAs,i°°Nb,122,la41n deduced mass excess. CONF Helsingor Voll PI07, CERN 81-09. NUCLEAR REACTIONS a°TPb(~-,xn),E at rest; measured neutron multiplicity, am,aoa,203,ao4,205 a°s,a°TTl deduced transitions. In-beam gamma spectroscopy,intrinsic Ge,coaxial lithium drifted Ge detectors. BAPSA 27 529,GEI,Budiek.

279

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A a63Bi

D 81BeYV:

aO3po

D 82SeZY:

aO3At

D 82SeZY:

R 82BUZZ:

~o4pb

D 79DzZY:

R 81BeZN: 81BoZQ: 81StZQ: 82BeZJ:

82LuZZ: 83PaZU: a64Bi

D 79DzZY: 80KIZX:

a04po

D 79VaZY:

D 81BeZI: R 82BUZZ:

2oSpb

R 81HoZK:

~OSBi

D 81BeYV:

2O5po

D 82KuZV: 82KuZW:

aOSAt

D 82KuZV: 82KuZW:

D 81UsZZ:

aOST1

R 82AnZX:

=

304

=

305

R A D I O A C T I V I T Y a°ST1 [ f r o m a°4Hg(t,2n),E=16 MeV]; m e a s u r e d 7(0,H,t). 2°5T1 l e v e l d e d u c e d J j r , T1/a,g,configuration. B A P S A 26 l l l 7 , A D 1 0 , B e e k e r . NUCLEAR REACTIONS a°7pb(lz-,xn),E at r e s t ; m e a s u r e d n e u t r o n m u l t i p l i c i t y , aol,ao2,ao3,ao4,2os, a°6,a°7T1 d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,coaxial lithium drifted Ge d e t e c t o r s . B A P S A 27 5 2 9 , G E t , B u d i c k . NUCLEAR REACTIONS 2°4Pb(n,X),E < 1O0 keV; m e a s u r e d t r a n s m i s s i o n . 2°spb d e d u c e d l e v e l s , level density,s-wave strength function. Particle-core d o o r w a y m o d e l . BAPSA 26 1139,CEI0, Horen. R A D I O A C T I V I T Y a°7,a°5,2°3,a°lBi [ f r o m Po d e c a y ] ; m e a s u r e d (ce)(ce)-,(ce)v-coin. 2o~ 2o5,~o3, a°lBi l e v e l s d e d u c e d T 1 / 2 , 7 - m u l t i p o l a r i t y , B ( ) ~ ) . REPT IPN 1981 A n n u a l , P N 4 7 , B e r g . R A D I O A C T I V I T Y 2°SAt; m e a s u r e d E T , I T , 7 7 - , ( c e ) v - c o i n . 2°5Po d e d u c e d l e v e l s , J , v r , 7 - b r a n c h i n g , 7-multipolarity,& REPT J I N R - P 6 - 8 2 - 1 3 3 , K u z n e t s o v a . R A D I O A C T I V I T Y a°SAt; m e a s u r e d Ev;Iv,I(ce),TV-,v(ce)-coin. 2°SPo d e d u c e d transitions, 7-multipolarity,& REPT J I N R - P 6 - 8 2 - 8 8 , K u z n e t s o v a . R A D I O A C T I V I T Y a°SAt; m e a s u r e d E v , I v , v ~ - , ( e e ) v - e o i n . 2°5Po d e d u c e d l e v e l s , J , ~ r , v - b r a n e h i n g , 7-multipolarity,6. REPT J I N R - P 6 - 8 2 - 1 2 3 , K u z n e t s o v a . R A D I O A C T I V I T Y 2°SAt; m e a s u r e d ET,IT,I(ce),TV-,7(ce)-coin. 2°5Po d e d u c e d transitions, 7-multipolarity,6. REPT J I N R - P 6 - 8 2 - 8 8 , K u z n e t s o v a .

A 2O6Hg

continued

NUCLEAR REACTIONS a°Tpb(/z-,xn),E at r e s t ; m e a s u r e d n e u t r o n m u l t i p l i c i t y , aoi,2oa,aoa,ao4,2os, a°6,2°TT1 d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,coaxial lithium drifted Ge d e t e c t o r s . B A P S A 27 5 2 9 , G E 1 , B u d i c k . R A D I O A C T I V I T Y a64Bi; m e a s u r e d Ev,IT,I(ce). a°4Pb t r a n s i t i o n s deduced ICC,7-multipolarity. Ge(Li) d e t e c t o r s , t o r o i d spectrometer. CONF R i g a , P 1 3 1 , D z h e l e p o v . NUCLEAR REACTIONS a64pb(a,a'),E=104 MeV; m e a s u r e d a(Ea), a64pb d e d u c e d h e x a d e c a p o l e state. High resolution magnetic spectrometer. REPT J U L - S p e z - 9 9 , P 4 1 , B e r g . NUCLEAR REACTIONS a64,a66,2°7,2°sPb(X,X),E n o t g i v e n ; m e a s u r e d K X - r a y i s o t o p e s h i f t s . 268 2o7,a86,264pb d e d u c e d r m s c h a r g e r a d i i . REPT J U L - S p e z - 9 9 , P 4 6 , B o r c h e r t . NUCLEAR REACTIONS a°4pb(a,a'),E=104 MeV; m e a s u r e d a(0). a64pb deduced hexadecapole transition characteristics. REPT ISN 8 1 - O l , P 6 4 , S t a c h . NUCLEAR REACTIONS i56Gd~i64~j68Er~i76Yb~i76~1~Hf~i62~4~i87~1~8~1~g~i~i~a~s~i~4~1~Pt(1aC~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . 176Yb,~76,166W,161Re,la6,1860s,167Ir,16s, 19apt,lo4,196Hg,169,2o6,2ol,2°a,a°4pb,a°s,~°Po,a°gAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS a ° S T l ( p , 2 n ) , E = 1 4 MeV; m e a s u r e d ET,Iv,vT-coin,l(ce). a64pb deduced transitions,Tl/~,E2,E0 transition strength. REPT J Y F L 1981 A n n , P 7 7 , L u o n t a m a . NUCLEAR REACTIONS ~64,Z°6Pb(e,e'); m e a s u r e d n o t g i v e n , uoa,~66Pb d e d u c e d t r a n s i t i o n c h a r g e d e n s i t i e s . B A P S A 27 7 O 6 , B C 1 3 , P a p a n i c o l a s . R A D I O A C T I V I T Y a6~Bi; m e a s u r e d Ev,IT,I(ce). a°aPb t r a n s i t i o n s deduced ICC,7-multipolarity. Ge(Li) d e t e c t o r s , t o r o i d spectrometer. CONF R i g a , P 1 3 1 , D z h e l e p o v . R A D I O A C T I V I T Y a°~,a64Bi [ f r o m 2°3Tl(a,5n),E=65 MeV; e°3Tl(~,3n),E=40.4 MeV]; m e a s u r e d EV,I7, 7 ( H , t ) . aoa,a64Bi l e v e l s d e d u c e d g. E n r i c h e d t a r g e t . REPT J U L - S p e z - 7 2 , P 6 1 , K l e i n r a h m . R A D I O A C T I V I T Y a°4Po; m e a s u r e d 7 c e - c o i n , E T , 1 7 . T o r o i d s p e c t r o m e t e r , G e ( L i ) d e t e c t o r . CONF Riga,P132,Vasharosh.

A 2O5T1

303

R A D I O A C T I V I T Y a67,a°5,a°a,a°~Bi [ f r o m Po d e c a y ] ; m e a s u r e d (ce)(ce)-,(ce)v-coin. a07,aosao3, e6iBi l e v e l s d e d u c e d T i / a , v - m u l t i p o l a r i t y , B ( ~ ). REPT IPN 1981 A n n u a l , P N 4 7 , B e r g . R A D I O A C T I V I T Y Z°3At [ f r o m I r ( 1 6 0 , x n ) , E = 1 2 5 M e V , m a s s s e p a r a t i o n ] ; measured 7 7 ( t ) . a°3po d e d u c e d l e v e l s . B A P S A 27 7 0 5 , B C 1 0 , S e m m e s . R A D I O A C T I V I T Y U°3At [ f r o m Ir(160,×n),E=135 M e V , m a s s s e p a r a t i o n ] ; measured 7 7 ( t ) . a°3po d e d u c e d l e v e l s . B A P S A 27 7 0 5 , B C 1 0 , S e m m e s .

A a64TI

=

ONLY)

=

206

R A D I O A C T I V I T Y 2°°Hg [ f r o m a°4Hg(t,p),E=16 MeV]; measured 7(t); deduced J,Tr,g,Tl/a, configuration. B A P S A 26 l l l T , A D l l , U s s e r y . NUCLEAR REACTIONS a°Tpb(l~-,n),E a t r e s t ; m e a s u r e d E%I7,7(t); d e d u c e d r e a c t i o n m e c h a n i s m . "2°6T1 d e d u c e d l e v e l s , J , v r , c o n f i g u r a t i o n s . B A P S A 27 5 2 9 , G E 2 , A n i g s t e i n .

280

SECONDARY

SOURCES

(Reporks,Abstracts,ekc.

A 2O6T1

R

ao6pb

R 80GaZO:

82BUZZ:

80TaZM: 81BoZQ: 81DuZU: 82BIZW: 82KuZO: 82KuZR: 82PaZU: 2O6po

R 82BeZJ:

82RaZW:

D 81JoZW:

2O7T1

D 81JoZW:

R

81GeZT: 82BeZM: 82BUZZ:

2o7pb

D 81TaZE: R 81BoZQ: 81DiZX:

2O7Bi

D 81BeYV: 81TaZQ:

81TaZR: 2OXpo

R 82RaZV:

R 79BeYP:

continued

=

207

RADIOACTIVITY Z°7Hg [ f r o m Z°spb(n,2p)]; m e a s u r e d T1/2,ET,IT,flT-,77-eoin; d e d u c e d Q,log ft. Z°TTl d e d u c e d l e v e l s , J , r r , 7 - b r a n c h i n g , 7 - m u l t i p o l a r i t y . CONF H e l s i n g o r Vo12 P640, CERN 81-09. RADIOACTIVITY a°THg [ f r o m a°sPb(n,2p)]; m e a s u r e d T1/2,E%I%flV-,VV-coin; d e d u c e d Q,log ft. 2°7TI d e d u c e d l e v e l s , J , T r , v - b r a n c h i n g , v - m u l t i p o l a r i t y . CONF H e l s i n g o r Vol2 P640, CERN 81-09. NUCLEAR REACTIONS a°sPb(d,SHe),E=108 MeV; m e a s u r e d cr(E(aHe)). 2°7TI d e d u c e d l e v e i , J , ~ , configuration. REPT IPN 1981 A n n u a l , P N 6 6 , G e r l i c . NUCLEAR REACTIONS a°sPb,2°gBi(d,SHe),E=45 MeV; m e a s u r e d (7(0); d e d u c e d e f f e c t i v e r e s i d u a l interaction, a°TTI,2°spb l e v e l s d e d u c e d c o n f i g u r a t i o n . REPT J U L - S p e z - 1 4 6 , P 1 1 , B e r g . NUCLEAR REACTIONS 2°TPb(/z-,xn),E at rest; m e a s u r e d n e u t r o n m u l t i p l i c i t y , zm,2o2,2osao42o5 2°6,a°TTl d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,coaxial lithium d r i f t e d Ge d e t e c t o r s . BAPSA 27 5 2 9 , G E i , B u d i c k . R A D I O A C T I V I T Y 2°7Bi; m e a s u r e d E(L X - r a y ) , v V ( t ) ; d e d u c e d Q(EC). a°Tpb l e v e l d e d u c e d n o K-capture,L2/L1 capture probability r a t i o . BAPSA 26 1 2 3 6 , H E I 7 , T a n . NUCLEAR REACTIONS 2°4,2°6,a°7,a°sPb(X,X),E n o t g i v e n ; m e a s u r e d K X - r a y i s o t o p e s h i f t s . 208 2°7,2°6,2°¢Pb d e d u c e d r m s c h a r g e r a d i i . REPT J U L - S p e z - 9 9 , P 4 6 , B o r c h e r t . NUCLEAR REACTIONS ~08Pb(p,d),E=26.3 MeV; m e a s u r e d a(0). a°TPb l e v e l s d e d u c e d S. Z e r o - , finite-range DWBA a n a l y s e s . BAPSA 26 1117,AD12,Dickey. R A D I O A C T I V I T Y 2°7,a°5,2°3,2°IBi [ f r o m Po d e c a y ] ; m e a s u r e d ( c e ) ( e e ) - , ( c e ) v - c o i n . 2o7 ~.o52o3 a°iBi l e v e l s d e d u c e d T i / a , v - m u l t i p o l a r i t y , B ( X ). REPT IPN 1981 A n n u a l , P N 4 7 , B e r g . RADIOACTIVITY 2°7Bi; m e a s u r e d (X-ray)(X-ray)(t),(X-ray)(ce)(t),I(ce),E(X-ray),l(X-ray); deduced L-shell branching ratios,fluorescence yields,Coster-Kronig transition probabilities. BAPSA 26 1235,HE13,Tan. R A D I O A C T I V I T Y 2°7Bi; m e a s u r e d E(L X - r a y ) , - y T ( t ) ; d e d u c e d Q(EC). 2°Tpb l e v e l d e d u c e d n o K-eapture,L2/L1 capture probability r a t i o . BAPSA 26 1236,HE17,Tan. NUCLEAR REACTIONS 2°aPb(a,5n),2°dPb((~,3n),a°Tpb(sHe,3n),E n o t given; m e a s u r e d 7 - d e c a y . 2°7Po deduced levels,J,rr,configurations,v-branching,isomer decay characteristics. In-beam s p e c t r o s c o p y . REPT JYFL 1981 A n n , P 8 2 , R a h k o n e n .

A

aospb

206

NUCLEAR REACTIONS 2°TPb(p~-,xn),E at rest; m e a s u r e d n e u t r o n m u l t i p l i c i t y . 2ol,2022o32o4,2o5, 2°6,207T1 d e d u c e d t r a n s i t i o n s . In-beam gamma spectroscopy,intrinsic Ge,eoaxial lithium d r i f t e d Ge d e t e c t o r s . BAPSA 27 5 2 9 , G E 1 , B u d i c k . NUCLEAR .REACTIONS 9°Zr,HSSn,2°sPb(c~fiHe),E=218 MeV; m e a s u r e d a(E(dHe)). SSZr,11%n,a°dpb deduced levels,broad structures. REPT IPN 1980 A n n u a l , P N 1 4 , G a l e s . NUCLEAR REACTIONS e°sPb(c~,dHe),E=64.3 MeV; m e a s u r e d a(0). a°dPb l e v e l s d e d u c e d L. E x a c t finite-range DWBA a n a l y s i s . REPT INS T o k y o 1980 A n n , P 4 1 , T a n a k a . NUCLEAR REACTIONS 2°4,2°6,2°7,2°sPb(X,X),E n o t g i v e n ; m e a s u r e d K X - r a y i s o t o p e s h i f t s . 208 z°7,a°6,2°4pb d e d u c e d r m s c h a r g e r a d i i . REPT J U L - S p e z - 9 9 , P 4 6 , B o r c h e r t . NUCLEAR REACTIONS 58Ni,'ldSn,2°sPb(a,dHe),E=218 MeV; m e a s u r e d cr(0),cr(E(6He)). 56Ni,l14Sn, 2 ° s p b d e d u c e d l e v e l s . REPT IPN 1981 A n n u a l , P N T 1 , D u h a m e l . NUCLEAR REACTIONS a ° s P b ( p , t ) , E = 5 0 . 5 MeV; m e a s u r e d a(Et),cr(0), a°dPb l e v e l s d e d u c e d excitation mechanism. DWBA,coupled-channels a n a l y s e s . REPT KVt 1981 A n n , P 2 8 , B l o k . NUCLEAR REACTIONS a°sPb(a,dHe),E=109 MeV; m e a s u r e d cr(0),cr(E(dHe)). 2°dPb d e d u c e d level,J, ~r. Z e r o - r a n g e DWBA. REPT INS T o k y o 1981 A n n , P 3 2 , K u r i h a r a . NUCLEAR REACTIONS a°aPb(c~,dHe),E:109 MeV; m e a s u r e d a(O). 266pb d e d u c e d level,J,Tr. Zero-range DWBA a n a l y s i s . REPT RCNP Osaka,1981 A n n , P 7 6 , K u r i h a r a . NUCLEAR REACTIONS a°4,a°dPb(e,e'); m e a s u r e d n o t g i v e n . 2°4,2°6Pb d e d u c e d t r a n s i t i o n c h a r g e d e n s i t i e s . BAPSA 27 7 0 6 , B C 1 2 , P a p a n i c o l a s . NUCLEAR REACTIONS ~58Gd~64~16aEr~76Yb~76~8~Hf~82~l~4~7~l88~1~%19~9a~s~194~t9~t(~aC~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n or(E). 17oyb,t76,~S°W,~8~Re,~Sd,188Os,~STIr, ~88, tgaPt,~94,t96Hg,t99,2°°,2°l,a°~,2°4pb,a°6,a~°Po,a°gAt deduced fission barrier. Statistical t h e o r y . REPT J I N R - P 7 - 8 2 - 4 0 2 , B e j z i n . NUCLEAR REACTIONS e°dpb(a,4n),2°TPb(a,5n),E n o t given; a°spb(sHe,Sn),E=21-28 MeV; m e a s u r e d 7 ( t ) , c r ( E v ) , v v - e o i n . 2°6Po d e d u c e d levels,T~/a,J,~r,7-multipolarity,v-branching. In-beam, conversion e l e c t r o n s p e c t r o s c o p y . REPT JYFL 1981 A n n , P 7 9 , R a h k o n e n .

A 2O7Hg

=

ONLY)

:

208

NUCLEAR REACTIONS 2°Tpb(n,n),(n,X),E not given; m e a s u r e d w i d t h s . C O N F Riga,P293,Benetskij.

281

(r,total (~. a°sPb d e d u c e d

IAS,

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 2oepb

R 80EyZZ: 80LeZI: 80MoZE: 80MoZF: 80MoZI: 81BoZM: 81BoZQ: 81DjZS:

81DjZT:

81DjZU:

81DjZV: 81DjZW:

81HAZE: 81MoZU: 81YaZV: 82BeZM: 82BoZU: 82DaZV:

82GuZY: 82MoZZ:

82ShZU: 82SjZZ: 82YaZX: aOapo

R 821tZZ:

R 81CaZV: 8IDrZX:

2O9Bi

R 8201ZY:

208

continued

NUCLEAR REACTIONS 2 ° s P b ( a , a ' ) , E n o t g i v e n ; m e a s u r e d a n ( 0 ) . 2°sPb d e d u c e d T = 0 , g i a n t resonance decay characteristics. REPT K f K - 3 0 6 8 , P 4 1 , E y r i c h . NUCLEAR REACTIONS 2osPb(gBe,gBe'),E=243 MeV; m e a s u r e d G(E(gBe)) at g r a z i n g angle; d e d u c e d reaction mechanism. 2°sPb d e d u c e d GQR e x c i t a t i o n . REPT ISN 8 0 - 0 1 , P 5 1 , L e b r u n . NUCLEAR REACTIONS 9°Zr,12°Sn,2OsPb(a,a'),E=100,172 MeV; m e a s u r e d G(Ea'). 9°Zr,12°Sn,~°sPb d e d u c e d G Q R , g i a n t m o n o p o l e r e s o n a n c e s , F . REPT J U L - S p e z - 7 2 , P 8 , M o r s c h . NUCLEAR REACTIONS 2oSpb(a,a'),E=172 MeV; 2°sPb(d,d'),E=86 MeV; m e a s u r e d G(O). 2°sPb d e d u c e d g i a n t r e s o n a n c e s . M i c r o s c o p i c DWBA a n a l y s i s . REPT J U L - S p e z - 7 2 , P 6 , M o r s c h . NUCLEAR REACTIONS e°epb(p,p'),E=45 MeV; m e a s u r e d G(Ep'),a(0). 2°sPb d e d u c e d levels. High resolution magnetic spectrometer. REPT J U L - S p e z - 7 2 , P 2 2 , M o r s c h . NUCLEAR REACTIONS 2°sPb(a,a),(a,a'),E=320,480 MeV; m e a s u r e d a(0). 2°sPb d e d u c e d q u a d r u p o l e , m o n o p o l e r e s o n a n c e . REPT ISN 8 1 - O l , P 4 3 , B o n i n . NUCLEAR REACTIONS 2°4,2°s,2°7,2°spb(X,X),E n o t g i v e n ; m e a s u r e d K X - r a y i s o t o p e s h i f t s . 2oa 2°7,2°6,2°4Pb d e d u c e d r m s c h a r g e r a d i i . REPT J U L - S p e z - 9 9 , P 4 6 , B o r c h e r t . NUCLEAR REACTIONS 2 ° s P b ( p , p ' ) , E = 2 0 1 MeV; m e a s u r e d G(0). 2esPb l e v e l s d e d u c e d B(X). M a c r o s c o p i c , M i c r o s c o p i c m o d e l s , D W B A , D W I A a n a l y s e s , R P A d e n s i t i e s . REPT IPN 1981 A n n u a l , PN60,Djalali. NUCLEAR REACTIONS 2 ° s p b , ' 9 7 A u , ' 2 ° S n ( p , p ' ) , E = 2 0 1 MeV; m e a s u r e d G(Ep'),~(0). i97Au,ia°Sn d e d u c e d g i a n t r e s o n a n c e F. a ° s P b d e d u c e d g i a n t r e s o n a n c e , F , T , - / - m u l t i p o l a r i t y . REPT IPN 1981 A n n u a l , P N 5 8 , D j a l a l i . NUCLEAR REACTIONS 2 ° s P b ( p , p ' ) , E = 2 0 1 MeV; m e a s u r e d G(O). a ° s P b d e d u c e d T=0,GQR fragmentation,T=l GQR,T=0 GDR. M a c r o s c o p i c D W B A , m i c r o s c o p i c DWIA a n a l y s e s . REPT IPNO-PhN-81-21,Djalali. NUCLEAR REACTIONS 2 ° s P b , l ~ T A u ( p , p ' ) , E = 2 0 0 MeV; m e a s u r e d & ( E p ' ) , a ( 0 ) . 2°9Pb d e d u c e d i s o s c a l a r G D R , i s o v e c t o r GQR. REPT I P N O - P h N - 8 1 - i 3 , D j a l a i . NUCLEAR REACTIONS a ° s p b ( p , p ' ) , E = 2 0 1 MeV; e ° s p b ( d , d ' ) , E = 1 0 8 MeV; Z e e P b ( a , a ' ) , E = 2 1 8 MeV; measured a(O,Ep'),o'(O,Ed'),G(O,Ea% e ° s P b d e d u c e d g i a n t r e s o n a n c e s , F , B ( k ) , E W S R f o r GQR. REPT I P N O - T - 8 1 - 0 2 , D ja lali. NUCLEAR REACTIONS 2°SBi(d,3He),E=50 MeV; m e a s u r e d a(O). 2°sPb d e d u c e d p a r t i c l e - h o l e s t a t e strength distributions. REPT RCNP O s a k a , 1 9 8 0 A n n , P 5 7 , H a y a k a w a . NUCLEAR REACTIONS 2 o S p b ( a , a ' ) , E = 1 7 2 MeV; m e a s u r e d G(Ea'),G(O). eesPb d e d u c e d g i a n t m o n o p o l e r e s o n a n c e , C Q R . M i c r o s c o p i c DWBA a n a l y s i s . REPT J U L - S p e z - 9 9 , P g , M o r s c h . NUCLEAR REACTIONS 2°spb(3He,3He'),E=140 MeV; m e a s u r e d a(E(3He)),a(0). 2°spb d e d u c e d levels, L. DWBA a n a l y s i s . REPT RCNP 0 s a k a , 1 9 8 0 A n n , P 4 6 , Y a m a g a t a . NUCLEAR REACTIONS a°sPb,2°gBi(d,3He),E=45 MeV; m e a s u r e d a(0); d e d u c e d e f f e c t i v e r e s i d u a l interaction. 2°TT1,2°sPb l e v e l s d e d u c e d c o n f i g u r a t i o n . REPT J U L - S p e z - 1 4 6 , P l l , B e r g . NUCLEAR REACTIONS 2°sPb(e,e'n),E=56,68,80 MeV; m e a s u r e d e ' n - c o i n ; d e d u c e d a. 2°8Pb d e d u c e d p o s s i b l e g i a n t r e s o n a n c e e x c i t a t i o n . BAPSA 27 7 3 2 , E E 1 2 , B o l m e . NUCLEAR REACTIONS a ° ~ P b ( n , n ) , E = t h e r m a l ; m e a s u r e d I(ce),vV-coin,Ev,Iv. 2°sPb d e d u c e d level, J,Tr,no t w o p h o n o n o c t u p o l e v i b r a t i o n , E 0 , E 3 t r a n s i t i o n s t r e n g t h . REPT I N D C ( A R G ) - 9 / G , P b 4 2 , Davidson. NUCLEAR REACTIONS 54,5eFe,SSNi,~2°Sn,2Oapb(polarized n,n'),E=10 MeV; m e a s u r e d A(0). 54,SSFe, 58Ni,la°Sn,2°epb l e v e l d e d u c e d s p i n - o r b i t deformation p a r a m e t e r s . BAPSA 27 542,GYa2,Guss. NUCLEAR REACTIONS 2 ° s P b ( a , a ' ) , E = 1 7 2 MeV; m e a s u r e d a ( E a ' ) , a ( 0 ) . 2esPb d e d u c e d G D R , g i a n t octupole excitation. Small angle behavior,single-wire,multi-wire proportional counters, magnetic spectrometer. REPT J U L - S p e z - 1 4 6 , P 1 6 , M o r s c h . NUCLEAR REACTIONS a ° a P b ( 7 , n ) , E n o t g i v e n ; m e a s u r e d a ( t o t a l ) . 2°sPb d e d u c e d r e s o n a n c e . PHCAA 38 3 3 , E A 6 , S h e r m a n . NUCLEAR REACTIONS 9°Zr,2°sPb(lsO,lsO'),E=400 MeV; m e a s u r e d or(0). 9°Zr,2OePb d e d u c e d g i a n t r e s o n a n c e s . BAPSA 27 7 3 2 , E E l l , S j o r e e n . NUCLEAR REACTIONS ~ospb(3He,3He'),E=140 MeV; m e a s u r e d &(E(3He')). 2°spb d e d u c e d r e s o n a n c e structure. H i g h r e s o l u t i o n . REPT RCNP Osaka,1981 A n n , P 5 1 , Y a m a g a t a . NUCLEAR REACTIONS 2°4,2°e,2°~pb(3He,F),E=60 MeV; 'g20s(IeO,F),E=90,110,131 MeV; 19Spt(12C,F), E=86,110.5 MeV; m e a s u r e d fission (fragment)(fragment)(0),total k i n e t i c e n e r g y . 208,21°Po deduced excitation,angular momentum r o l e i n f i s s i o n . REPT J I N R - P T - S 2 - 1 9 , I t k i s .

A 2ogpb

=

ONLY)

=

209

NUCLEAR REACTIONS a°gBi(n,p),E-61 MeV; m e a s u r e d a(Ep),cr(0), a°9pb level d e d u c e d p o s s i b l e g i a n t T = I m o n o p o l e r e s o n a n c e . BAPSA 26 l 1 3 9 , C E l l , C a s t a n e d a . NUCLEAR REACTIONS 2°8Pb(n,~/),E=7-20 MeV; m e a s u r e d a s y m m e t r y . 2°~Pb deduced T=I,GQR. REPT LA 9 0 2 6 , D r a k e . NUCLEAR REACTIONS P b , 2 ° g B i ( n , n ) , E = l . 5 - 4 MeV; m e a s u r e d or(E), a°gBi,Pb d e d u c e d GDR characteristics. Tof. REPT N E A N D C ( O R ) - 1 5 7 / U , P 1 2 , 0 1 s s o n .

282

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A ~O9At

R

82BeZJ:

D 81HaZN:

alOpo

R 82BeZJ:

821tZZ:

a~OAt

D 79BaXY:

D 79BaXY:

RADIOACTIVITY

R 80LoZV: 81LoZX:

D 81HaZN:

al4Rn

R 81LoZY:

R

a:eTh

R 81BaZ0:

81LoZY:

D 81HaZN:

218Ra

R 82EnZZ: 82GaZX:

=

211 Auger

spectra.

CONF R i g a , P 2 5 7 , B a b e n k o v .

212

=

214

=

216

NUCLEAR REACTIONS ~ ° s P b ( 1 3 C , 3 n a ) , ( l a C , 5 n ) , E = 7 5 - 9 5 MeV; m e a s u r e d Ev,Iv,v(0),13CT(t),vT(t), a7-coin, at4Rn,a16Ra deduced levels,J,rr,Tl/a,B(X),7-multipolarity,configurations. Ge(Li),Si surface barrier detectors,enriched t a r g e t . REPT JYFL R R - 1 3 / 8 1 , L o n n r o t h . NUCLEAR REACTIONS Z°sPb,ZaSU,z4SCm(tSO,X),(160,F),ls4W,197Au,a°Spb(aas,x),(a2S,F),E n o t g i v e n ; measured or(fragment 0). e a 4 , e i e T h , 2 5 4 F m , a 6 4 1 0 4 , a a g A m , a 4 ° C f d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . B A P S A 36 l l l g , A E 9 , B a c k .

A

alaFr

=

R A D I O A C T I V I T Y ZiSFr; m e a s u r e d Ea,Ia; d e d u c e d T,/2,isomer,(~ b r a n c h i n g , a14At; m e a s u r e d Tl/a, Ec~,Ia; d e d u c e d isomer,J,rr,configuration. 21°Bi l e v e l s deduced a-decay population probability. REPT A E C L - 7 2 3 4 , P 2 1 , H a g b e r g . NUCLEAR REACTIONS 2 ° S P b ( l a C , 3 n e ~ ) , ( l a C , 5 n ) , E = 7 5 - 9 5 MeV; m e a s u r e d ET,IT,7(0),laCT(t),77(t), aT-coin. Z14Rn,a16Ra d e d u c e d levels,J,rr,T1/a,B(X),7-multipolarity,configurations. Ge(Li),Si surface barrier detectors,enriched t a r g e t . REPT JYFL R R - 1 3 / 8 1 , L o n n r o t h .

A a16Ra

210

NUCLEAR REACTIONS a ° 9 B i ( c % n ) , E = 1 8 - 2 1 MeV; m e a s u r e d c r ( E T ) , T ( t ) , v V - c o i n , alZAt d e d u c e d levels,possible J,rr,T-multipolarity. REPT JYFL 1980 A n n , P 7 5 , L o n n r o t h . NUCLEAR REACTIONS 2 ° g B i ( a , n ) , E = 1 8 - 2 0 . 8 MeV; m e a s u r e d E'y,Iv,I(ce),7(0),cr(E'y),VV-, 7(X-ray)-eoin. 2'aAt deduced levels,J,rr,isomer Twa,ICC,d,V-multipolarity,configuration. REPT J Y F L R R - 1 4 / 8 1 , L o n n r o t h .

A al4At

=

al°,211At; m e a s u r e d

A 21aAt

continued

R A D I O A C T I V I T Y alSFr; m e a s u r e d Ea,Ia; d e d u c e d T l / a , i s o m e r , a - b r a n c h i n g . a~4At; m e a s u r e d TI/2, Ea,Icx; d e d u c e d isomer,J,~r,configuration. 21°Bi l e v e l s deduced a-decay population probability. REPT A E C L - 7 2 3 4 , P 2 1 , H a g b e r g . NUCLEAR REACTIONS ~5sGd~164~88Er~76Yb~i76~18~Hf~8~1e4W~s7~8~2~19~z~s~94~i98Pt(~aC~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d (r(fragment 0 ) , f i s s i o n (~(E). 170yb,17~,~8°W,~2~Re,126,182Os,laTIr,188, 1 9 a p t , ~ 9 4 , , 9 6 H g , ~ 9 9 , a o 0 , a o l sea a o 4 p b , a 2 ~ , a ~ O p o , a O g A t d e d u c e d fission barrier. Statistical t h e o r y . REPT J I N R - P Y - 8 3 - 4 0 3 , B e j z i n . NUCLEAR REACTIONS 2°~,a°~,a°TPb(aHe,F),E=60 MeV; ~gaOs(~O,F),E=90,110,131 MeV; ~9~Pt(IzC,F), E=86,110.5 MeV; m e a s u r e d fission (fragment)(fragment)(0),total kinetic energy, a°2,a'°Po deduced excitation,angular momentum r o l e i n f i s s i o n . REPT J I N R - P 7 - 8 2 - 1 9 , I t k i s . RADIOACTIVITY ai°,anAt; measured A u g e r s p e c t r a . CONF R i g a , P 3 5 7 , B a b e n k o v .

A ZHAt

209

NUCLEAR REACTIONS i5~Gd~64~i68Er~78Yb~76~8~Hf~t84W~187~i82~i29~i9~iaz~s~4~192Pt(i~C~F)~E 6 8 - 1 0 6 MeV; m e a s u r e d a(fragment 0 ) , f i s s i o n a ( E ) . ~7°yb,~Te,12OW,181Re,~26,~eSOs,iaTIr,iSs, 192pt,194,196Hg,i99,2oo,2ol 2o8 8 o 4 p b , a O 2 2 1 O p o , a O g A t d e d u c e d fission barrier. Statistical t h e o r y . REPT J I N R - P T - 8 2 - 4 0 2 , B e j z i n .

A ZiOBi

=

ONLY)

=

218

R A D I O A C T I V I T Y ZlSFr; m e a s u r e d Ea,l~; d e d u c e d T w a , i s o m e r , a - b r a n c h i n g . e14At; m e a s u r e d TWz, Ec~,la; d e d u c e d isomer,J,~r,configuration. 21°Bi l e v e l s deduced a-decay population probability. REPT A E C L - 7 2 3 4 , P 2 1 , H a g b e r g . NUCLEAR REACTIONS a°e,2°sPb(IzC,3n),E=69 MeV; m e a s u r e d V V - c o i n . 21SRa d e d u c e d l e v e l s , J j r . B A P S A 27 7 1 5 , C D 1 0 , E n n i s . NUCLEAR REACTIONS 2°6,2°sPb(13C,3n),E n o t g i v e n ; m e a s u r e d VV(0)~V(0),G(Ev),Tc~(6),TV- , 7a-coin. Z18Ra d e d u c e d levels,J,rr,B(X),a-clustering. B A P S A 27 533,EYa11,Gai.

283

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A

aa4Ra

D 82BoZT:

ua4Th

R 81BaZ0:

82BaZU

R 82VaZU

aaaTh

D 82VaZQ

R 81BaZ0:

D 81VaZV:

82VaZP: R 79BlZU: 82SiZW:

R 79BrZG:

79DuZQ: 81MeZX:

81MoZV: 81VaZS: 82GaZW: 82ItZY: 82JAZZ:

82TaZR: ~a2pa

R 81P1ZX:

=

229

=

231

RADIOACTIVITY aaSU,aalTh; m e a s u r e d T - e m i s s i o n p r o b a b i l i t y . U - A I a l l o y , U r a n i u m f l o u r i d e , Uranium acetate sources,a-counting,mass spectrometric isotope dilution. REPT INDC(NDS)-126/NE,P13,Vaninbroukx. RADIOACTIVITY ZaSu,aalTh Cin e q u i l i b r i u m w i t h a35U]; m e a s u r e d T - e m i s s i o n p r o b a b i l i t y f o r Z31Th,2alPa t r a n s i t i o n s . REPT N E A N D C ( E ) - 2 3 2 U , V o l I I I , P 5 1 , V a n i n b r o u k x . NUCLEAR REACTIONS Za°Th(n,F),E < 5 MeV; m e a s u r e d a(E). zalTh deduced v i b r a t i o n a l resonance, f i s s i o n c h a n n e l K v a l u e s . REPT N E A N D C ( E ) - 2 0 2 U , V o l I I I , P 6 , B l o n s . NUCLEAR REACTIONS aa°Th(d,pF),E=17 MeV; m e a s u r e d f i s s i o n f r a g m e n t y i e l d vs m a s s . aalTh deduced symmetric fission characteristics. REPT L A - 9 3 8 1 - P R , P 9 3 , S i c r e .

A

aaaTh

228

NUCLEAR REACTIONS 2°spb,2aaU,a4aCm(160,X),(l°0,F),I84W,197Au,2°spb(3aS,X),(32S,F),E n o t g i v e n ; measured c r ( f r a g m e n t 0). 224,216Th,a54Fm,264104,2agAm,a4°Cf d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . BAPSA 26 l l l 9 , A E 9 , B a c k .

A

aalTh

=

NUCLEAR REACTIONS lS4W,232Th(d,6Li),E=45 MeV; m e a s u r e d cr(E(6Li)), lS°Hf d e d u c e d g r o u n d s t a t e r o t a t i o n a l b a n d . a~aRa d e d u c e d p o s s i b l e m u l t i p l e t . REPT KVI 1981 A n n , P 2 0 , v a n d e n Berg. RADIOACTIVITY 228Th [ i n e q u i l i b r i u m w i t h a3ZU3; m e a s u r e d v - e m i s s i o n p r o b a b i l i t i e s f o r 21ZBi, a~2Po,a°sPb,aa°Rn t r a n s i t i o n s . REPT N E A N D C ( E ) - 2 3 2 U , V o l I I I , P 4 9 , V a n i n b r o u k x .

A

229Am

224

RADIOACTIVITY aa4Ra; m e a s u r e d Ea,Ia; deduced a - e m i s s i o n p r o b a b i l i t y . REPT NEANDC(E)-232U, Vol I I I , P 4 9 , B o r t e l s . NUCLEAR REACTIONS aoSpb,eaaU,a4SCm(l~O,X),(~sO,F),~84W,~97Au,a°apb(aeS,X),(aaS,F),E n o t g i v e n ; measured a(fragment 0). aa4,al°Th,a54Fm,a64104,aaOAm,a4°Cf d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . BAPSA ~6 l l l 9 , A E 9 , B a c k . NUCLEAR REACTIONS Z°spb,aaaTh,a3aU(mO,F),E n o t given; m e a s u r e d f i s s i o n a ( f r a g m e n t 0). aa4Th, a4SCf,a54Fm d e d u c e d s a d d l e p o i n t d e f o r m a t i o n . Halpern-Strutinski method,near barrier f u s i o n . BAPSA 27 6 7 5 , G Y c 2 , B a c k .

A

~SRa

=

ONLY)

=

232

NUCLEAR REACTIONS a a 2 T h ( a 4 K r , a 4 K r ' ) , E n o t given; measured ET,IT,77-coin,Coulomb excitation. ~3aTh d e d u c e d levels,rotational band,K,~r,vibrational modes. CONF Argonne(High-Spin Phenomena in Nuclei) Proc,P477,Briancon. NUCLEAR REACTIONS 23aTh(n,n'7),E=3 MeV; m e a s u r e d E% 232Th d e d u c e d t r a n s i t i o n s . Ge(Li) d e t e c t o r s . CONF R i g a , P 5 8 7 , D u s h i n . NUCLEAR REACTIONS a32Th,aa4,aas,23SU(p,p'),E=35.3 MeV; m e a s u r e d a ( 0 ) . aa2Th,aa4,aas,aaSu deduced quadrupole,hexadecapole,multipole moments. Split-pole spectrograph,UF4,ThF 4 targets. Coupled-channels a n a l y s i s . DABBB 42 2 4 2 7 , M e l i n . NUCLEAR REACTIONS aa2Th,23aU(a,a'),E=100,172 MeV; m e a s u r e d a(Ea'),cr(0). 23ZTh,23Su d e d u c e d g i a n t r e s o n a n c e f r a g m e n t a t i o n , L , F , E W S R . REPT J U L - S p e z - 9 9 , P 8 , M o r s c h . NUCLEAR REACTIONS a3aTh(e,F),E=5.9-8 MeV; m e a s u r e d ~ ( f r a g m e n t 0). a3aTh l e v e l d e d u c e d p o s s i b l e J,rr. REPT I N D C ( B Z L ) - 5 / G , P 7 , V a n n u c c i . NUCLEAR REACTIONS 2aSU,aa2Th(T,F),E ~ 4.4-5.05 MeV; m e a s u r e d G. aaSU,2aaTh levels d e d u c e d fission probabilities. REPT J I N R - P 1 5 - 8 2 - 1 8 , G a n g r s k y . NUCLEAR REACTIONS 2 3 a T h ( n , n ' 7 ) , E = l - 2 . 2 MeV; m e a s u r e d ET,IT; d e d u c e d a. aaaTh d e d u c e d l e v e l s . REPT N E A N D C ( J ) - 8 3 / U , P S 5 , 1 t a g a k i . NUCLEAR REACTIONS aaaTh(p,p'F),E=30 MeV; m e a s u r e d a ( E p ' ) , ~ ( f r a g m e n t 0); d e d u c e d f i s s i o n probability v s e x c i t a t i o n , a3aTh d e d u c e d f i s s i o n b a r r i e r c h a r a c t e r i s t i c s . REPT KVI 1981 Ann,P39,Janszen. NUCLEAR REACTIONS e a a T h ( n , n ' 7 ) , E = l - 2 . 2 MeV; m e a s u r e d E T , I T , a ( E T , E ) , a ( 0 n ) . 232Th l e v e l s deduced excitation probability. REPT N E T U - 4 0 , P 1 4 , T a k a h a s h i . NUCLEAR REACTIONS a a I P a ( n , F ) , E = 0 . 4 - 1 0 0 e V , 0 . 1 2 - 0 . 4 2 MeV; m e a s u r e d ~7(E). aa2Pa d e d u c e d r e s o n a n c e s , K , l r , f i s s i o n b a r r i e r p a r a m e t e r s . S t a t i t i s t i c a l m o d e l . REPT N E A N D C ( E ) - 2 1 1 - L , P 4 3 , Plattard.

284

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 232 U

R 81JaZT

R 79CoZF 80IwZV

81AuZX

81TaZP 233 U

D 79GeZR 81AhZV R 81VaZT

D

80VaZO:

R 81ArZU: 81ArZV:

81MeZX:

82VaZS:

D 79ZhZV 79ZhZW 81VaZV

82VaZP R 80DeZI:

R 79VoZY: 81ArZU: 81ArZV:

8tMaZB: 8IMeZX:

233

=

234

=

235

RADIOACTIVITY 235mu; m e a s u r e d Ey. CONF R i g a , P 5 6 4 , Z h u d o v . RADIOACTIVITY aaSrnu; m e a s u r e d I ( c e ) ( t ) ; d e d u c e d Tt/~. CONF R i g a , P 5 6 3 , Z h u d o v . RADIOACTIVITY aaSu,zalTh; m e a s u r e d y - e m i s s i o n p r o b a b i l i t y . U-A1 a l l o y , U r a n i u m f l o u r i d e , Uranium acetate sources,a-counting,mass spectrometric isotope dilution. REPT INDC(NDS)-126/NE,P13,Vaninbroukx. RADIOACTIVITY aaSu,2aITh Ein e q u i l i b r i u m w i t h 235U3; m e a s u r e d y - e m i s s i o n p r o b a b i l i t y f o r aalTh,231Pa t r a n s i t i o n s . REPT N E A N D C ( E ) - 2 3 2 U , V o l I I I , P 5 1 , V a n i n b r o u k x . NUCLEAR REACTIONS 235U(84Kr,S4Kr'),E=370,450 MeV; m e a s u r e d C o u l o m b e x c i t a t i o n , E % I y , y y ( t ) , y(84Kr)-coin, aaSu d e d u c e d rotational bands,J,rr. Rotor plus quasiparticle model, Hartree-Fock o r b i t a l s . REPT ISN 8 0 - 0 1 , P 3 9 , d e B e t t e n c o u r t .

A 236 U

=

RADIOACTIVITY e38pu; m e a s u r e d Ey,I%E(L X - r a y ) , I ( L X - r a y ) follwing a-decay. 234U transition d e d u c e d ICC. REPT NEANDC(E)-21EU,Vol I I I , P 3 2 , V a n i n b r o u k x . NUCLEAR REACTIONS aa4,a3s,a38U(e,F),E=5.5-8 MeV; m e a s u r e d g ( f r a g m e n t 0). 234,aas,aaSu d e d u c e d levels,J,rr,T,E2 transition s t r e n g t h , E W S R . REPT I N D C ( B Z L ) - 5 / G , P 9 , A r r u d a Neto. NUCLEAR REACTIONS 234,236,aaSU(e,F),E=5.5-25 MeV; m e a s u r e d a b s o l u t e G ( f i s s i o n ) . 234,236,aaSU d e d u c e d GQR d e c a y , E 2 s t r e n g t h function,fission probabilities. REPT I N D C ( B Z L ) - 5 / G , P 8 , Arruda Nero. NUCLEAR REACTIONS 2aaTh,234,236,238U(p,p'),E=35.3 MeV; m e a s u r e d (r(0). aSeTh,ea4,zae,2aSu deduced quadrupole,hexadecapole,multipole moments. Split-pole spectrograph,UF4,ThF 4 targets. Coupled-channels a n a l y s i s . DABBB 42 2 4 2 7 , M e l i n . NUCLEAR REACTIONS aaaTh(a,2n),E n o t g i v e n ; m e a s u r e d Ey,I%I(ce). e34U d e d u c e d levels,J,rr, B(E0)/B(E2),E0 e n h anc e m e nt,rota tiona l b a n d s . REPT KVI 1981 A n n , P S l , v a n K l i n k e n .

A aa5 U

continued

NUCLEAR REACTIONS eaZTh(n,y),E=20-2200 eV; m e a s u r e d a(Ey). 23aTh deduced r e s o n a n c e s , p - w a v e assignment,neutron r e d u c e d w i d t h s . REPT N E A N D C ( E ) - 2 0 g U , V o l I I 1 , P 1 6 , C o r u i . NUCLEAR REACTIONS 2a2Th(n,F),E=I.5 MeV; m e a s u r e d ( ~ ( E n ) , p r o m p t f i s s i o n , aaaTh d e d u c e d temperature. Maxwellian distribution,least-square fitting. REPT N E A N D C ( J ) - 6 7 / U , P 6 9 , Iwasaki. NUCLEAR REACTIONS aU2Th(n,F),E=0.7-9 MeV; m e a s u r e d a(fission,E). 233Th d e d u c e d s t r u c t u r e , rotational band character,K,relative f i s s i o n s t r e n g t h s . REPT L A - 8 6 7 1 , A u c h a m p a u g h . NUCLEAR REACTIONS 232Th(n,F),E=l.6 MeV; m e a s u r e d ~ ( E n ) , p r o m p t n e u t r o n s . 2aaTh d e d u c e d Maxwellian temperature. REPT N E A N D C ( J ) - 7 5 / U , P 6 3 , T a m u r a . R A D I O A C T I V I T Y a33U; m e a s u r e d T1/2. CONF R i g a , P 5 4 8 , G e j d e l m a n . R A D I O A C T I V I T Y 233U,239pu; m e a s u r e d E a , r e l a t i v e I s . REPT I N D C ( N D S ) - I E 6 / N E , P 2 8 , A h m a d . NUCLEAR REACTIONS 233U(e,F),E=5.5-31 MeV; m e a s u r e d a b s o l u t e a ( f i s s i o n ) , a33U d e d u c e d GQR. Photofission d a t a i n p u t . REPT I N D C ( B Z L ) - 5 / G , P S , V a n n u c c i .

A 234 U

232

NUCLEAR REACTIONS a a a T h ( a , 4 n ) , E = 4 0 MeV; m e a s u r e d I ( c e ) , ( c e ) ( c e ) - , y ( e e ) - e o i n . 2aZu d e d u c e d levels,a,~r,interband transitions. REPT KVI 1980 A n n , P 8 9 , a a n s e n .

A Z33Th

=

ONLY)

=

236

NUCLEAR REACTIONS 235U(n,F),E=0.23-5.0 MeV; m e a s u r e d s h a d o w effect, a3eU d e d u c e d TI/2 vs e x c i t a t i o n . CONF R i g a , P 6 0 4 , V o r o t n i k o v . NUCLEAR REACTIONS za4,z3e,a38U(e,F),E=5.5-8 MeV; m e a s u r e d a ( f r a g m e n t e). 2a4,2as,ZaSU d e d u c e d tevels,J,rr,T,E2 transition s t r e n g t h , E W S R . REPT I N D C ( B Z L ) - 5 / G , P 9 , A r r u d a Nero. NUCLEAR REACTIONS z34,aae,ZaSU(e,F),E=5.5-25 MeV; m e a s u r e d a b s o l u t e a ( f i s s i o n ) . ~a4,zas,aaau d e d u c e d GQR d e c a y , E 2 s t r e n g t h function,fission probabilities. REPT I N D C ( B Z L ) - 5 / G , P 8 , Arruda Neto. NUCLEAR REACTIONS 235U(d,pf),E=15 MeV; m e a s u r e d p ( f r a g m e n t ) - c o i n . 2aau d e d u c e d f r a g m e n t charge distribution v s e x c i t a t i o n . REPT ISN 8 1 - 0 1 , P 6 5 , M a r i o l o p o u l o s . NUCLEAR REACTIONS ZS2Th,234,2ae,2aaU(p,p'),E=35.3 MeV; m e a s u r e d (~(8). eSaTh,a34,zas,238U deduced quadrupole,hexadecapole,multipole moments. Split-pole spectrograph,UF4,ThF 4 targets. Coupled-channels a n a l y s i s . DABBB 42 2 4 2 7 , M e l i n .

285

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A 236U

R 82ChZS:

=

D 81AIZV:

=

R A D I O A C T I V I T Y a37Pu(SF) [ f r o m AE15,Alonso-Arias.

A 238 U

D 80PoZX:

R 81ArZU: 81ArZV:

81DoZZ:

81MeZX:

81MoZT: 81MoZV: 82GaZW: 82MoZY:

82VaZY: a38Np

D 79BaYF:

238pu

D 80AhZV: 80VaZ0:

R 82McZY:

82TsZZ: 239p U

D 79VaZG: 80RyZX: 81AhZV 81UmZZ

239Am

R 82RaZT

D 79BuZC 80AhZV:

235U(a,2n),E=25 MeV]; m e a s u r e d

=

isomer

T1/2. BAPSA 26 1120,

238

=

239

NUCLEAR REACTIONS 165Ho,a3SU(n,v),E=7-15 MeV; m e a s u r e d EV,Iv; d e d u c e d a(0) v s E , r e a c t i o n mechanism. 239U,'66Ho t r a n s i t i o n s deduced inital,final state Nilsson assignments. Direct-semidireet m o d e l . REPT L A - 9 0 9 3 - M S , M c D a n i e l s . NUCLEAR REACTIONS 181Ta,a38U(n,n),E=0.024-1 MeV; m e a s u r e d a ( t o t a l ) v s E. '82Ta,~39U d e d u c e d s-,p-,d-wave average resonance parameters. REPT N E A N D C ( J ) - 8 3 / U , P I 4 , T s u b o n e . R A D I O A C T I V I T Y 239pu; m e a s u r e d a-decay T1/2. S p e c i f i c a c t i v i t y measurement. REPT NEANDC(E)-202U,Vol III,P26,Vaninbroukx. R A D I O A C T I V I T Y 239pu; m e a s u r e d Ea. A b s o l u t e measurement,spectrograph. CONF E a s t Lansing(Atomic Masses,Fund Constants) P249,Rytz. R A D I O A C T I V I T Y a33U,a39pu; m e a s u r e d Ea,relative I a . REPT I N D C ( N D S ) - l R 6 / N E , P 2 8 , A h m a d . R A D I O A C T I V I T Y 239pu; m e a s u r e d Ev,relative IV. Ge(Li) d e t e c t o r , h i g h precision. REPT INDC(NDS)-126 /NE,P38,Umeza wa. NUCLEAR REACTIONS a37Np(a,2n),E=25 MeV; m e a s u r e d 7(0,H). a39Am d e d u c e d f i s s i o n i s o m e r g, configuration. B A P S A 27 7 0 6 , B C l l , R a f a i l o v i c h .

A 24Opu

237

R A D I O A C T I V I T Y a38U(SF); m e a s u r e d n n - e o i n , n e u t r o n m u l t i p l i c i t y ; d e d u c e d TI/a. P r o p o r t i o n a l counter detection. REPT J I N R - E 1 5 - 8 0 - 2 7 6 , P o p e k o . NUCLEAR R E A C T I O N S 234,aa6,eaaU(e,P),E=5.5-8 MeV; m e a s u r e d o r ( f r a g m e n t 0). 234,236,a38U d e d u c e d levels,J,Tr,T,E2 transition s t r e n g t h , E W S R . REPT I N D C ( B Z L ) - 5 / G , P 9 , A r r u d a Nero. NUCLEAR REACTIONS 234,23°,a3aU(e,F),E=5.5-25 MeV; m e a s u r e d a b s o l u t e a ( f i s s i o n ) , aa4236,aa8 U deduced GQR d e c a y , E 2 s t r e n g t h function,fission probahilities. REPT I N D C ( B Z L ) - 5 / G , P 8 , Arruda Nero. NUCLEAR REACTIONS a 3 a U ( e , e ' F ) , E = 6 7 . 1 1 , 5 6 . 9 1 , 4 6 . 4 9 MeV; m e a s u r e d e(fragment)(0),form f a c t o r s . ZaaU d e d u c e d multipole contribution to fission decay. Plastic scintillators,UF 4 t a r g e t . DABBB 42 6 7 3 , D o w e l l . NUCLEAR REACTIONS a a a T h , a 3 4 , a a 6 , 2 3 a U ( p , p ' ) , E = 3 5 . 3 MeV; m e a s u r e d a ( 0 ) . 232Th,a34,aa6,aaSU deduced quadrupole,hexadecapole,multipole moments. Split-pole spectrograph,UF4,ThF 4 targets. Coupled-channels a n a l y s i s . DABBB 42 2 4 2 7 , M e l i n . NUCLEAR REACTIONS a3SU(a,a'F),E=172 MeV; m e a s u r e d a ( f r a g m e n t ) - c o i n , a38u d e d u c e d g i a n t resonance e v i d e n c e . REPT J U L - S p e z - 9 9 , P 1 2 , M o r s c h . NUCLEAR REACTIONS 232Th,e3aU(~,a'),E=100,172 MeV; m e a s u r e d cr(Ea'),~r(O). 232Th,238U d e d u c e d giant resonance fragmentation,L,F,EWSR. REPT J U L - S p e z - 9 9 , P 8 , M o r s c h . NUCLEAR REACTIONS a3eU,a32Th(7,F),E ~ 4 . 4 - 5 . 0 5 MeV; m e a s u r e d a. a38U,a32Th l e v e l s d e d u c e d fission probabilities. REPT J I N R - P 1 5 - 8 2 - 1 8 , G a n g r s k y . NUCLEAR REACTIONS 2 3 S U ( a , a ' F ) , ( a , a ' ) , E = 1 7 2 MeV; m e a s u r e d a(Ea'),a(fragment)-coin,a(Oa, fragment O). a38U d e d u c e d T=0,giant resonance fission decay characteristics. REPT JUL-Spez- 146,P17,Morsch. NUCLEAR REACTIONS a38U(e,e'F),E=80.3,118.4 MeV; m e a s u r e d ( f r a g m e n t ) e - c o i n . a38U d e d u c e d E 2 / E0 t r a n s i t i o n strength distribution. B A P S A 27 4 5 9 , A Y a 6 , V a n B i b b e r . R A D I O A C T I V I T Y 242mAre; m e a s u r e d E a , I a , E 7. aaeNp d e d u c e d l e v e l s , J , ~ r , K . CONF R i g a , P 1 3 4 , Baranov. R A D I O A C T I V I T Y a38,a4°Pu; m e a s u r e d relative I a . REPT I N D C ( N D S ) - l l 8 / N E , P 4 0 , A h m a d . R A D I O A C T I V I T Y a38pu; m e a s u r e d ET,Iv,E(L X - r a y ) , I ( L X-ray) follwing a-decay, a34U transition d e d u c e d ICC. REPT N E A N D C ( E ) - 2 1 2 U , V o l I I I , P 3 R , V a n i n b r o u k x .

A 230 U

continued

NUCLEAR REACTIONSIa3aTh,a36U(laC,SBe),E n o t g i v e n ; m e a s u r e d a a ( f r a g m e n t ) - c o i n following fission, a36U,z4°pu d e d u c e d fission probability vs excitation. REPT L A - 9 3 8 1 - P R , P g 0 , Cheifetz.

A

237pu

236

ONLY)

=

R A D I O A C T I V I T Y a4°pu(SF); m e a s u r e d measured

RADIOACTIVITY 238,24°pu;

286

240 Tt/a. REPT NEANDC(E)-202U,Vol I I I , P 9 , B u d t z d o r g e n s e n . r e l a t i v e I a . REPT INDC(NDS)-ilB/NE,P40,Ahmad.

SECONDARY

SOURCES

(Reports,Abstracts,etc.

A a40pu

R

a4Ocf

R 81BaZO:

82ChZS:

D 79VaZF: 82DeZP:

D 82A1ZW:

24aAm

D 79BaYF: 81VaZQ: R 79KnZ0: 80WiZN:

242Cm

D 80UsZZ:

R 81FIZW:

D 81BoZN:

246Fm

R 81FIZW:

D 81BoZN:

R 82BaZU:

242

=

243

=

244

=

246

NUCLEAR REACTIONS 7°Zn,l°4Ru,n°Pd,154Sm,158,16°Gd,~sSW,196,198pt,2°a,2°4Hg,z44pu(polarized t,a), 198Pt,a44pu,76Ge(polarized t,p),E=17 MeV; 82,8°Se,1°°Mo,12a,la4Sn(polarized t,aHe),E=22-25 MeV; m e a s u r e d a ( 0 ) , a n a l y z i n g p o w e r v s 0,cr(Ea),o~(Ep),a(3He). 89Cu,'°aTc,'°gRh,15apm,157,159Eu, 185Ta,195,1971r,2Ol,a°aAu,a43Np,a°°Pt,e4SPu,78Ge,8°,82As,lO°Nb,lZe,124In d e d u c e d m a s s e x c e s s . CONF H e l s i n g o r V o l l P107, CERN 8 1 - 0 9 . R A D I O A C T I V I T Y 244,246Fm(SF); m e a s u r e d fragment average total kinetic energy,average neutron number,mass asymmetry. Multi-parametric ionization chambers. REPT JINR P 1 5 - 8 1 - 7 0 6 , B o g d a n o v .

A 248Cf

=

R A D I O A C T I V I T Y a44,246Fm(SF); m e a s u r e d fragment average total kinetic energy,average neutron number,mass asymmetry. Multi-parametric ionization chambers. REPT JINR-Pl5-81-706,Bogdanov.

A 246pu

241

NUCLEAR REACTIONS 7°Zn,lO4Ru,n°Pd,154Sm,158,1S°Gd,186W,196,198pt,2°~,a°4Hg,244pu(polarized t,a), 19°pt,244pu,76Ge(polarized t , p ) , E = 1 7 MeV; 8 a , 8 ° S e , l ° ° M o , l ~ a , l a 4 S n ( p o l a r i z e d t , 3 H e ) , E = 2 2 - 2 5 MeV; m e a s u r e d ( r ( 0 ) , a n a t y z i n g p o w e r v s 0,(r(Ea),~(Ep),a(3He). 69Cu,l°3Tc,l°gRh,153prn,157,159Eu, lS5Ta,195,197Ir,a°l,a°3Au,243Np,2°°Pt,a46pu,78Ge,e°,82As,l°°Nb,laa,'241n d e d u c e d m a s s e x c e s s . CONF H e t s i n g o r V o l l P107, CERN 8 1 - 0 9 .

A a44Fm

=

RADIOACTIVITY 24Zpu(SF); m e a s u r e d f i s s i o n f r a g m e n t y i e l d v s m a s s , t o t a l k i n e t i c e n e r g i e s ; deduced difference from n-induced f i s s i o n i n ~41Pu. REPT N E A N D C ( E ) - 2 3 2 U , V o l I I I , P 4 , Allaert. RADIOACTIVITY 24amAm; m e a s u r e d Ea,Ic~,E-y. ~3SNp d e d u c e d l e v e l s , J j r , K . CONF Riga,P134, Baranov. RADIOACTIVITY 242Arn(SF) [ - f r o m 2 4 3 A m ( a O M g , X ) , E = l I 0 - 1 4 0 MeV3; m e a s u r e d TI/a. KEPT JINR-P7-81-863,Vasko. NUCLEAR REACTIONS 241Am(n,F),E=l eV-5.3 MeV; m e a s u r e d a(E). 24aArn deduced resonances,Ff. Fission fragment d e t e c t i o n . REPT N E A N D C ( E ) - 2 0 2 U , V o l I I I , P 1 0 , K n i t t e r . NUCLEAR REACTIONS 241Arn(n,7),E=14.75 meV,30 keV; m e a s u r e d o r ( c a p t u r e ) , a42Arn d e d u c e d i s o m e r i c r a t i o . REPT K f K - 3 0 6 8 , P 2 1 , W i s s h a k . R A D I O A C T I V I T Y 24aCre; m e a s u r e d T,/2. REPT N E A N D C ( J ) - 6 7 / U , P 6 , U s u d a .

A Z43Np

continued

R A D I O A C T I V I T Y 241pu; m e a s u r e d c~-decay TW2. Mass spectrornetric,a41Am i n g r o w t h t e c h n i q u e s . KEPT N E A N D C ( E ) - 2 0 2 U , V o l I I I , P 2 6 , V a n i n b r o u k x . R A D I O A C T I V I T Y a41Pu; m e a s u r e d TI/~. Mass s p e c t r o m e t r y , d i r e c t decay. REPT NEANDC(E)-232U, Vol I I I , P 5 4 , D e B i e v r e .

A a42pu

240

NUCLEAR REACTIONS 232Th,23Su(12C,SBe),E not g i v e n ; m e a s u r e d a a ( f r a g r n e n t ) - c o i n f o l l o w i n g f i s s i o n . 236U,24Opu d e d u c e d fission probability vs excitation. REPT L A - 9 3 8 1 - P R , P 9 0 , Cheifetz. NUCLEAR REACTIONS 2°sPb,23~U,a~SCm(~SO,X),(I~O,F),I84W,~97Au,~°spb(32S,X),(3aS,F),E n o t g i v e n ; measured a(fragrnent 0). 2a4,at6Th,a54Frn,2~4104,a~gArn,a4°Cf d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . BAPSA 26 l l l g , A E 9 , B a c k .

A Z4lpu

=

ONLY)

=

248

NUCLEAR REACTIONS a°spb,a32Th,a38U(160,F),E n o t given; m e a s u r e d f i s s i o n o r ( f r a g m e n t 0). 224Th, 24SCf,254Frn d e d u c e d s a d d l e p o i n t d e f o r m a t i o n . Halpern-Strutinski method,near barrier f u s i o n . BAPSA 27 675,GYcE,Baek.

287

SECONDARY

(Reports,Abstracts,etc.

SOURCES

A

aSOBk

D 82KoZZ:

D 79BoZA: 82WeZV:

D 79SeZV:

a54Es

D 82KoZZ:

254Fm

R 81BaZ0:

82BaZU:

R 81BaZO:

R 81BoZH:

=

254

Gr e n o b l e ( N u c l . S p c c t r o s c . F i s s i o n P r o d u c t s ) , P 3 1 6 , S e l i c . RADIOACTIVITY a54Es; m e a s u r e d E t x , I a , E 7 , I T , I ( c e ) , a T - , ( c e ) 7 - c o i n . aS°Bk d e d u c e d levels, rotational bands,configurations. BAPSA 27 5 2 3 , E Y a 1 3 , K o e n i g . NUCLEAR REACTIONS 2°sPb,23aU,a¢aCm(180,X),(160,F),la4W,laTAu,2°apb(3aS,X),(3aS,F),E n o t g i v e n ; measured a(fragment 0). 224,218Th,254Fm,264104,aagAm,Z4Ocf d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . BAPSA 36 l l l g , A E 9 , B a c k . NUCLEAR REACTIONS a°aPb,232Th,Z3aU(lSO,F),E n o t given; m e a s u r e d f i s s i o n a ( f r a g m e n t 0). 2Z4Th, 242Cf,a54Fm d e d u c e d s a d d l e p o i n t d e f o r m a t i o n . Halpern-Strutinski method,near barrier f u s i o n . BAPSA 37 675,GYe3,Back.

=

~64

NUCLEAR REACTIONS Z°8Pb,23aU,e4SCm(160,X),(160,F),lS4W,197Au,ZOSpb(a2S,X),(32S,F),E n o t g i v e n ; measured a(fragment O). 224,216Th,a54Fm,264104,229Am,24°Cf d e d u c e d f i s s i o n s a d d l e p o i n t deformation. F i s s i o n f o l l o w i n g f u s i o n . BAPSA 26 l l l g , A E 9 , B a c k .

A 278110

252

RADIOACTIVITY 254Cf(SF); m e a s u r e d E % I % 7 ( f r a g m e n t ) - c o i n ; d e d u c e d i n d e p e n d e n t y i e l d s f o r 9 8 S r 10o 1o2 lO4Zr 1o4 106 lOaMo 108 l10,112Ru,14o,142Xe,142,144 146 148Ba,146,148,15OCe ' CONF

A 264104

=

aS°Bk deduced levels,

RADIOACTIVITY 252Cf(SF); m e a s u r e d lfi + u p p e r l i m i t . CONF R i g a , P 5 6 5 , B o r o v o j . RADIOACTIVITY ~SaCf(SF); m e a s u r e d f r a g m e n t y i e l d , a v e r a g e t o t a l k i n e t i c e n e r g y , v a r i a n c e vs f r a g m e n t m a s s . C o m p a r i s o n w i t h t r i t o n i n d u c e d f i s s i o n i n 258Cf t a r g e t . REPT L A - 9 3 8 1 - P R , P92,Weber.

A

254Cf

250

RADIOACTIVITY 254Es; m e a s u r e d Ea,Ia,ET,IT,I(ce),(~7-,(ce)7-coin. rotational bands,configurations. BAPSA 27 5 2 3 , E Y a 1 3 , K o e n i g .

A

~SaCf

=

ONLY)

=

378

NUCLEAR REACTIONS 2aaU(4°Ar,F),E=209 MeV; m e a s u r e d a ( f r a g m e n t ) v s m a s s ; d e d u c e d f a s t f i s s i o n e v i d e n c e . 278110 d e d u c e d f i s s i o n b a r r i e r . REPT IPN 1981 A n n u a l , P R 1 3 , B o r d e r i e .

288