Secondary Sources

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 8 8L

i

D

9 5M i Z Y :

RADIOACTIVITY

8Li(β–)

7Li(d,p),E=3.5

[from

deduced inplantation sites of

8Li

and

12N

12N(β+)

MeV];

[from

10B(3He,n),E=3

MeV]; measured β–NMR;

i n Z n S e c r y s t a l . P o l a r i z e d s o u r c e s ,β – N M R t e c h n i q u e . R E P T O U L N S

1994 Annual,P31,Miyake. 9 5On Z Z :

RADIOACTIVITY

8 Li(β – )

[from

MeV]; measured β–NMR; deduced hyperfine field,relaxation time,

7 Li(d,p),E=3.5

atomic dipolar field in ferromagnetic Fe crystal. β–NMR technique. REPT OULNS 1994 Annual,P38,Onishi. 9 5Ya ZZ :

RADIOACTIVITY

8 Li(β – )

[from

MeV]; measured Iβ(θ),β delayed α anisotropy from

7 Li(d,p),E=3.5

8 Be;

deduced

alignment correlation coefficient. β–NMR technique,polarized source. REPT OULNS 1994 Annual,P47, Yamaguchi.

A = 9 9C

D

9 5Ma ZW :

RADIOACTIVITY

[from C( 1 2 C, 9 C),E=67 MeV/nucleon]; measured β–NMR.

9 C(β + )

deduced µ. Polarized source.

9C

REPT RIKEN–94,P40,Matsuta. R

9 5Ma ZW :

NUCLEAR REACTIONS C(12C,9C),E=67 MeV/nucleon; measured β–NMR.

level deduced µ. Projectile

9C

fragmentation. REPT RIKEN–94,P40,Matsuta.

A = 11 1 1C

R

9 5O z Z Z :

NUCLEAR REACTIONS Be,C, 2 7 Al( 1 1 C, 1 1 C),( 1 2 N, 1 2 N),E=730 MeV/nucleon; measured interaction σ; deduced rms 11C,12N

radii and effective deformation parameters.

deduced rms matter radii. Radioactive beams. REPT

RIKEN–94,P35,Ozawa. 1 1N

R

9 5Gu Z Z :

1 4 N( 3 He, 6 He),E=73.4

NUCLEAR REACTIONS

MeV; measured energy spectrum of

1 1 N,σ(θ). 1 1 N

deduced levels,

possible J,π. DWBA. REPT INS 1994 Annual,P3,Guimaraes.

A = 12 1 2B e

R

9 5K o ZU :

NUCLEAR REACTIONS

1 H( 12 Be,p),E=55

MeV/nucleon; measured proton spectra.

12 Be

deduced levels. Radioactive

beams. REPT RIKEN–94,P33,Korsheninnikov. 1 2B

D

9 5M i Z Z :

RADIOACTIVITY

1 2 B(β – )

9 Be( 1 4 N, 1 2 B),E=39.3

[from

MeV/nucleon]; measured source spin polarization. β–NMR

method. REPT OULNS 1994 Annual,P27,Mitsuoka. R

9 5 I c ZZ :

12C(12C,12N),E=135

NUCLEAR REACTIONS

M e V / n u c l e o n ; m e a s u r e d e x c i t a t i o n e n e r g i e s ,σ ( θ ) .

12B

deduced the

structure of spin–dipole resonance. DWBA. REPT RIKEN–94,P48,Ichihara. 1 2C

R

9 5 F u ZV :

1 2 C( 1 6 O, 1 2 C),E(cm)=22.4,29.8,30.1,31.8

NUCLEAR REACTIONS

deduced S matrix elements,intermediate states J,π.

12C

MeV; measured momentum spectra of

1 2 C,σ(θ);

level deduced magnetic substate population. REPT

Kyushu Univ Tandem Acc Lab Rept,1993–1994,P51,Fujita. 1 2N

D

9 5M i Z Y :

RADIOACTIVITY

8Li(β–)

7Li(d,p),E=3.5

[from

deduced inplantation sites of

8Li

and

12N

MeV];

12N(β+)

[from

10B(3He,n),E=3

MeV]; measured β–NMR;

i n Z n S e c r y s t a l . P o l a r i z e d s o u r c e s ,β – N M R t e c h n i q u e . R E P T O U L N S

1994 Annual,P31,Miyake. R

9 5O z Z Z :

NUCLEAR REACTIONS Be,C, 2 7 Al( 1 1 C, 1 1 C),( 1 2 N, 1 2 N),E=730 MeV/nucleon; measured interaction σ; deduced rms radii and effective deformation parameters.

11C,12N

deduced rms matter radii. Radioactive beams. REPT

RIKEN–94,P35,Ozawa.

A = 13 1 3B e

R

9 5K o ZV :

NUCLEAR REACTIONS

2H,C(12Be,p),E=55

MeV/nucleon; measured proton spectra.

13Be

deduced levels.

Radioactive beams. REPT RIKEN–94,P32,Korsheninnikov. 1 3C

R

9 3A t ZZ :

NUCLEAR REACTIONS

1 3 C(α,α),E=54.1,104,155

MeV;

1 3 C, 1 8 O(α,α'),E=54.1,104,155

80.7,104,155 MeV; measured σ(E,θ); deduced model parameters.

MeV;

13C,16,18O

1 6 O(α,α'),(α,α),E=48.7,

levels deduced B(λ).

Coupled–channels analysis. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P26,Atzrott. 1 3N

R

9 5 F u ZU :

NUCLEAR REACTIONS

1 3 C( 3 He,t),E=450

MeV; measur ed tr iton spec tr a,dec ayin g pr oton spec tr a.

13N

deduced

levels,spin–flip dipole resonances. REPT RCNP 1994 Annual,P32,Fujiwara. 1 3O

D

9 5Ma Z Z :

RADIOACTIVITY

1 3 O(β + )

[from

9 Be( 1 6 O, 1 3 O),E=130

MeV/nucleon];

2 3 Mg(β + )

[from

1 9 7 Au( 2 4 Mg, 2 3 Mg),E=100

MeV/

nucleon]; measured β–NMR; deduced relaxation time and Knight shift in Pt crystal. β–NMR technique, polarized sources. REPT OULNS 1994 Annual,P43,Matsuta. 9 5TaZZ :

RADIOACTIVITY constant.

13O

1 3 O(β + )

[from

9 Be( 1 6 O, 1 3 O),E=67

MeV/nucleon]; measured β–NMR; deduced quadrupole coupling

level deduced µ,quadrupole moment. β–NMR technique,polarized source. REPT OULNS 1994

Annual,P41,Tanigaki.

997

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 14 1 4B e

D

9 5Ao ZZ :

1 4B

D

9 5Ao ZZ :

14Be(β–n)

RADIOACTIVITY deduced log ft.

14 B

14Be(β–n)

RADIOACTIVITY deduced log ft.

14 B

[from Be(18O,14Be),E=100 MeV/nucleon]; measured tof of β–delayed neutron,Eγ;

deduced level. REPT RIKEN–94,P38,Aoi. [from Be(18O,14Be),E=100 MeV/nucleon]; measured tof of β–delayed neutron,Eγ;

deduced level. REPT RIKEN–94,P38,Aoi.

A = 16 1 6N

D

9 5FuZZ :

1 6O

D

9 5FuZZ : 9 3A t ZZ :

state. state.

16 O

[from

15N(d,p),E=2.3

MeV]; measured Eβ,Iβ(t),γ time spectra,T1/2,β decay rate of

levels deduced β–branching. REPT OULNS 1994 Annual,P34,Fukuda.

16 O

16N(β–)

RADIOACTIVITY 16 N(0 – )

R

16N(β–)

RADIOACTIVITY 16 N(0 – )

[from

15N(d,p),E=2.3

MeV]; measured Eβ,Iβ(t),γ time spectra,T1/2,β decay rate of

levels deduced β–branching. REPT OULNS 1994 Annual,P34,Fukuda.

NUCLEAR REACTIONS

1 3 C(α,α),E=54.1,104,155

MeV;

1 3 C, 1 8 O(α,α'),E=54.1,104,155

80.7,104,155 MeV; measured σ(E,θ); deduced model parameters.

MeV;

13C,16,18O

1 6 O(α,α'),(α,α),E=48.7,

levels deduced B(λ).

Coupled–channels analysis. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P26,Atzrott.

A = 17 1 7B

D

9 5U e Z Z :

17B(β–)

RADIOACTIVITY

[from

93Nb(22Ne,17B),E=110

MeV/nucleon]; measured β–NMR.

17B

level deduced µ.

Polarized source. REPT RIKEN–94,P41,Ueno. R

9 5U e Z Z :

NUCLEAR REACTIONS

93 Nb( 22 Ne, 17 B),E=110

MeV/nucleon; measured β–NMR following ejectile β–decay.

17 B

level

deduced µ. Projectile fragmentation. REPT RIKEN–94,P41,Ueno. 1 7N

J

9 5U e Z Y :

NUCLEAR MOMENTS

17 N

[from

93 Nb( 18 O, 17 N),E=70

MeV/nucleon]; measured β–NMR.

17 N

level deduced µ. Polarized

source. REPT RIKEN–94,P42,Ueno. R

9 5U e Z Y :

NUCLEAR REACTIONS

9 3 Nb( 1 8 O, 1 7 N),E=70

MeV/nucleon; measured β–NMR following ejectile β–decay.

17N

level

deduced µ. Projectile fragmentation. REPT RIKEN–94,P42,Ueno.

A = 18 1 8N

D

9 5O z Z Y :

RADIOACTIVITY

19C(β–n);

measured tof of β–delayed neutron,T1/2,Eγ.

18,19N

deduced levels. Projectile

fragmentation. REPT RIKEN–94,P39,Ozawa. 1 8O

R

9 3A t ZZ :

NUCLEAR REACTIONS

1 3 C(α,α),E=54.1,104,155

MeV;

1 3 C, 1 8 O(α,α'),E=54.1,104,155

80.7,104,155 MeV; measured σ(E,θ); deduced model parameters.

MeV;

13C,16,18O

1 6 O(α,α'),(α,α),E=48.7,

levels deduced B(λ).

Coupled–channels analysis. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P26,Atzrott.

A = 19 1 9C

D

9 5O z Z Y :

RADIOACTIVITY

19C(β–n);

measured tof of β–delayed neutron,T1/2,Eγ.

18,19N

deduced levels. Projectile

18,19N

deduced levels. Projectile

fragmentation. REPT RIKEN–94,P39,Ozawa. 1 9N

D

9 5O z Z Y :

RADIOACTIVITY

19C(β–n);

measured tof of β–delayed neutron,T1/2,Eγ.

fragmentation. REPT RIKEN–94,P39,Ozawa.

A = 20 2 0N e

R

9 5FuZT :

NUCLEAR REACTIONS 20 Ne

2 0 Na

R

9 5 S u ZV :

18 O( 3 He,n),E=30

MeV; measured σ(θ); deduced two–nucleon transfer reaction mechanism.

deduced levels,J,π. Tof. DWBA. REPT CYRIC 1994 Annual,P1,Fujii.

NUCLEAR REACTIONS C(20Na,X),(32Na,X),E=900 MeV/nucleon; measured interaction σ for these,other Na isotope projectiles.

20,32Na

deduced rms radii,thick neutron skin for these,other Na isotopes.

Radioactive beams. REPT RIKEN–94,P36,Suzuki.

A = 23 2 3Mg

D

9 5Ma ZV :

RADIOACTIVITY

23 Mg(β + )

[from

197 Au( 24 Mg, 23 Mg),E=91

MeV/nucleon]; measured β–NMR; deduced β–ray asymmetry

parameter. Polarized source. REPT RIKEN–94,P43,Matsuta. 9 5Ma Z Z :

RADIOACTIVITY

1 3 O(β + )

[from

9 Be( 1 6 O, 1 3 O),E=130

MeV/nucleon];

2 3 Mg(β + )

[from

1 9 7 Au( 2 4 Mg, 2 3 Mg),E=100

MeV/

nucleon]; measured β–NMR; deduced relaxation time and Knight shift in Pt crystal. β–NMR technique, polarized sources. REPT OULNS 1994 Annual,P43,Matsuta.

998

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 25 2 5A

l

D

9 3Mo Z P :

RADIOACTIVITY

25Si(β+p)

[from

24Mg(3He,2n),E=35

MeV];

29S(β+p)

β–delayed E(p),βp–,γp–coin,T1/2; deduced GT strength functions.

[from

25Al,29P

28Si(3He,2n),E=35

MeV]; measured

deduced levels. Silicon detector,

β–counter telescope. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P69,Morinobu. 25S

i

D

9 3Mo Z P :

RADIOACTIVITY

25Si(β+p)

[from

24Mg(3He,2n),E=35

MeV];

29S(β+p)

β–delayed E(p),βp–,γp–coin,T1/2; deduced GT strength functions.

[from

25Al,29P

28Si(3He,2n),E=35

MeV]; measured

deduced levels. Silicon detector,

β–counter telescope. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P69,Morinobu.

A = 26 2 6 Na

R

9 5N i Z T :

2 6 Mg, 2 7 Al, 2 8 Si(d,X),E=270

NUCLEAR REACTIONS 27 Mg, 26 Na, 28 P

MeV; measured excitation energies following

2 He

emission.

2 He

emission.

deduced Gamow–Teller strength distributions. REPT RIKEN–94,P47,Niizeki.

A = 27 2 7Mg

R

9 5N i Z T : 9 5N i ZU :

2 6 Mg, 2 7 Al, 2 8 Si(d,X),E=270

NUCLEAR REACTIONS 27 Mg, 26 Na, 28 P

MeV; measured excitation energies following

deduced Gamow–Teller strength distributions. REPT RIKEN–94,P47,Niizeki.

NUCLEAR REACTIONS

2 7 Al(d,X),E=270

MeV; measured excitation energy following

2 He

emission.

2 7 Mg

deduced

Gamow–Teller transition strength distribution. REPT RIKEN–94,P46,Niizeki.

A = 28 28P

R

9 5N i Z T :

2 6 Mg, 2 7 Al, 2 8 Si(d,X),E=270

NUCLEAR REACTIONS 27 Mg, 26 Na, 28 P

MeV; measured excitation energies following

2 He

emission.

deduced Gamow–Teller strength distributions. REPT RIKEN–94,P47,Niizeki.

A = 29 29P

D

9 3Mo Z P :

RADIOACTIVITY

25Si(β+p)

[from

24Mg(3He,2n),E=35

MeV];

29S(β+p)

β–delayed E(p),βp–,γp–coin,T1/2; deduced GT strength functions.

[from

25Al,29P

28Si(3He,2n),E=35

MeV]; measured

deduced levels. Silicon detector,

β–counter telescope. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P69,Morinobu. 29S

D

9 3Mo Z P :

RADIOACTIVITY

25Si(β+p)

[from

24Mg(3He,2n),E=35

MeV];

29S(β+p)

β–delayed E(p),βp–,γp–coin,T1/2; deduced GT strength functions.

[from

25Al,29P

28Si(3He,2n),E=35

MeV]; measured

deduced levels. Silicon detector,

β–counter telescope. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P69,Morinobu.

A = 32 3 2 Na

R

9 5 S u ZV :

NUCLEAR REACTIONS C(20Na,X),(32Na,X),E=900 MeV/nucleon; measured interaction σ for these,other Na isotope projectiles.

20,32Na

deduced rms radii,thick neutron skin for these,other Na isotopes.

Radioactive beams. REPT RIKEN–94,P36,Suzuki. 3 2Mg

R

9 5Mo Z Y :

208Pb(32Mg,32Mg'),E=49.2

NUCLEAR REACTIONS effective σ.

32 Mg

MeV/nucleon; measured Eγ following Coulomb excitation,

deduced deformation parameter,B(E2). Radioactive beams. REPT RIKEN–94,P37,Motobayashi.

A = 39 3 9Ca

D

9 5 T a ZY :

RADIOACTIVITY

39Ca(β+)

[from Ta(40Ca,39Ca),E ≈ 10 MeV/nucleon]; measured β–NMR; deduced polarization.

REPT OULNS 1994 Annual,P46,Tanigaki.

A = 40 4 0Ca

R

9 4Vo ZT :

NUCLEAR REACTIONS

40Ca(e,e'p),(e,e'α),E=183.5

α–spectra; deduced E1,(E2+E0) strength functions.

40Ca(p,2p),(p,p'α),E=99.4

MeV; 40Ca

MeV; measured σ(θ),p–,

deduced electric giant resonance fragmentations.

CONF Dubna(Selected Topics Nucl Struct) Proc,P76,Von Neumann–Cosel. 40S c

R

9 5 I t ZZ :

NUCLEAR REACTIONS

4 0 Ca(p,n),E=35

MeV; measured σ(θ).

REPT CYRIC 1994 Annual,P17,Itoh.

999

4 0 Sc

deduced levels,J,π. NE213 scintillator. DWBA.

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 44 44T

i

R

9 5Ya ZX :

4 0 Ca( 6 Li,d),E=37

NUCLEAR REACTIONS

MeV; measured σ(θ); deduced reaction mechanism.

4 4 Ti

levels deduced

possible configuration. DWBA. REPT INS 1994 Annual,P8,Yamaya.

A = 45 45S c

J

9 5 S a ZY :

45Sc;

NUCLEAR MOMENTS stable

45 Sc

measured NMR; deduced electric field gradient in TiO2 single crystal. Dilute

atoms embedded in TiO 2 . REPT OULNS 1994 Annual,P56,Sato.

A = 46 46T

i

J

9 4Ga Z Z :

NUCLEAR MOMENTS

4 6 , 4 7 , 4 8 , 4 9 , 5 0 Ti;

measured hfs,isotope shifts; deduced charge rms radius differences. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P44,Gangrsky. R

9 4 I s ZS :

4 6 Ti(γ,γ'),E=6.6

NUCLEAR REACTIONS

MeV bremsstrahlung; measured γ–spectra.

4 6 Ti

deduced levels,( Γ 0 ) 2 /Γ,

B(λ). CONF Dubna(Selected Topics Nucl Structure) Contrib,P53,Ishkhanov.

A = 47 47T

i

J

9 4Ga Z Z :

NUCLEAR MOMENTS

4 6 , 4 7 , 4 8 , 4 9 , 5 0 Ti;

measured hfs,isotope shifts; deduced charge rms radius differences. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P44,Gangrsky.

A = 48 48T

i

J

9 4Ga Z Z :

NUCLEAR MOMENTS

4 6 , 4 7 , 4 8 , 4 9 , 5 0 Ti;

measured hfs,isotope shifts; deduced charge rms radius differences. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P44,Gangrsky. R

9 4A l ZX :

48Ti(γ,γ'),E=6.6

NUCLEAR REACTIONS

MeV bremsstrahlung; measured γ–spectra.

48Ti

levels deduced B(M1).

CONF Dubna(Selected Topics Nucl Structure) Contrib,P16,Alimov. 4 8C r

R

9 3ZuZZ :

20Ne(28Si,24Mg),(28Si,28Si),(28Si,16O),E=11,20

NUCLEAR REACTIONS

MeV; measured σ(θ) vs E.

48Cr

deduced

resonance structure. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P387,Zurmuhle.

A = 49 4 9Ca

R

9 5H i Z Z :

48 Ca(d,p),E=25

NUCLEAR REACTIONS

MeV; measured σ(θ).

49 Ca

levels deduced J,π,C 2 S. DWBA. REPT INS 1994

Annual,P4,Hino. 49T

i

J

9 4Ga Z Z :

NUCLEAR MOMENTS

4 6 , 4 7 , 4 8 , 4 9 , 5 0 Ti;

measured hfs,isotope shifts; deduced charge rms radius differences. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P44,Gangrsky.

A = 50 50T

i

J

9 4Ga Z Z :

NUCLEAR MOMENTS

4 6 , 4 7 , 4 8 , 4 9 , 5 0 Ti;

measured hfs,isotope shifts; deduced charge rms radius differences. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P44,Gangrsky.

A = 56 56F e

R

9 4 I s ZR :

NUCLEAR REACTIONS

5 6 Fe(γ,γ'),E=6.6

MeV bremsstrahlung; measured γ–spectra.

5 6 Fe

deduced levels,(Γ 0 ) 2 /Γ,

B(λ). CONF Dubna(Selected Topics Nucl Structure) Contrib,P54,Ishkhanov.

A = 57 5 7N i

D

9 5Oh Z Z :

RADIOACTIVITY

57Ni(β+)

[from

58Ni(α,3n2p),E=50

MeV]; measured NMR,β asymmetry.

57Ni

deduced µ.

Recoil–implantation,low–temperature nuclear orientation. REPT INS 1994 Annual,P5,Ohtsubo.

A = 58 5 8 Cu

R

9 5Ak ZY :

NUCLEAR REACTIONS

58Ni(3He,t),E=450

MeV; measured momentum spectra of t.

strength of Gamow–Teller resonance states. REPT OULNS 1994 Annual,P91,Akimune.

1000

58Cu

deduced transition

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 71 7 1G e

R

9 5Da Z Z :

7 1 Ga( 3 He,t),E=450

NUCLEAR REACTIONS

MeV; measured triton spectra.

7 1 Ge

deduced Gamow–Teller transition

strength,solar neutrino capture rates. REPT RCNP 1994 Annual,P23,Daito. 7 1A s

R

9 3K o ZM :

70Ge(polarized

NUCLEAR REACTIONS

p , p ) , E = 4 . 9 4 – 5 . 1 8 M e V ; m e a s u r e d σ ( E ) , a n a l y z i n g p o w e r A ( z ) (θ , E ) .

71As

deduced parity nonconservation effect,IAR excitation. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992, P27,Kouda. 9 3O c Z Z :

70Ge(polarized

NUCLEAR REACTIONS

p , p ) , E = 4 . 9 4 – 5 . 1 6 M e V ; m e a s u r e d σ ( E ) , a n a l y z i n g p o w e r A ( z ) (θ , E ) .

71As

deduced IAR parameters,parity nonconserving matrix element. REPT Kyushu Univ Tandem Acc Lab Rept, 1991–1992,P25,Ochiishi.

A = 78 7 8Rb

D

9 5Mu Z T :

RADIOACTIVITY

7 8 Rb(β + )

[from

5 4 Fe( 2 8 Si,n3p),E=110

MeV]; measured Eγ,K X–rays,γγ–coin; deduced levels,J,π,

T 1/2 . REPT UTTAC 1994 Annual,P24,Mukai,UTTAC–62. R

9 5Mu Z T :

MeV; measured Eγ,Iγ,γγ(particles)–coin.

54Fe(28Si,n3p),E=110

NUCLEAR REACTIONS

78Rb

deduced high–spin

levels,J,π,T 1/2 ,band structure. REPT UTTAC 1994 Annual,P24,Mukai,UTTAC–62.

A = 79 79S r

R

9 3 SuZT :

NUCLEAR REACTIONS properties.

79Sr

5 8 Ni( 2 8 Si,n2pα),E=128

MeV; measured Eγ,Iγ,γ(θ),γγ–coin,T 1 / 2 ; deduced band structure and

d e d u c e d h i g h – s p i n l e v e l s , J ,π . N O R D B A L L s p e c t r o m e t e r . R E P T K y u s h u U n i v T a n d e m A c c L a b

Rept,1991–1992,P72,Suematsu.

A = 80 80S r

D

9 5 S h ZX :

RADIOACTIVITY MeV]; 80 Sr

8 0Y

D

9 5 S h ZX :

[from

[from

58Ni(32S,np),E=100,102

54Fe(28Si,np),E=88

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata.

RADIOACTIVITY MeV]; 80 Sr

88Tc(β+),(EC)

80Y(β+),(EC)

88Tc(β+),(EC)

80Y(β+),(EC)

[from

[from

58Ni(32S,np),E=100,102

54Fe(28Si,np),E=88

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata.

A = 81 8 1Rb

R

9 3 L i ZR :

NUCLEAR REACTIONS bands features.

81S r

R

9 3 L i ZR :

R

9 3M i Z P :

81 Sr

5 3 Cr( 3 1 P,n2p),( 3 1 P,2np),E=97

MeV; measured Eγ,Iγ,γγ–coin.

8 1 Rb

deduced J,π,rotational

deduced high–spin levels. REPT McMaster Univ,1992–1993,Annual,P59,Liden.

NUCLEAR REACTIONS bands features.

8 1Y

81 Sr

5 3 Cr( 3 1 P,n2p),( 3 1 P,2np),E=97

MeV; measured Eγ,Iγ,γγ–coin.

8 1 Rb

deduced J,π,rotational

deduced high–spin levels. REPT McMaster Univ,1992–1993,Annual,P59,Liden.

NUCLEAR REACTIONS

58 Ni( 28 Si,pα),E=100

MeV;

58 Ni( 32 S,p2α),E=120,125

MeV; measured Eγ,Iγ,γ(θ).

81 Y

deduced

high–spin levels,J,π. NORDBALL spectrometer,n–,γ–multiplicity filter. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P75,Mitarai.

A = 82 82S r

R

9 3N i ZW :

NUCLEAR REACTIONS

63 Cu( 19 F,X),E=50,54.4,68.2

MeV;

66 Zn( 16 O,X),E=50,65

MeV; measured Eγ.

82 Sr

deduced GDR

widths. BaF 2 scintillator. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P62,Niiya. 8 2Y

R

9 3Mu ZW :

NUCLEAR REACTIONS

58 Ni( 28 Si,n3p),E=100,102,128

MeV; measured Eγ,Iγ,γγ–coin.

82 Y

deduced high–spin levels,

J,π. NORDBALL spectrometer. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P78,Mukai. 82Z r

R

9 3M i ZO :

NUCLEAR REACTIONS

5 8 Ni( 2 8 Si,2n2p),E=128

MeV; measured Eγ,Iγ,γγ–coin.

8 2 Zr

deduced high–spin levels,J,π.

NORDBALL spectrometer,n–,γ–multiplicity filter. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P82, Mitarai.

A = 83 8 3Rb

D

9 3G o Z L :

RADIOACTIVITY

83Rb(EC);

measured Eγ,E(ce). Electrostatic spectrometer. Precise measurements,comparison

with other data. CONF Dubna,P181,Gorozhankin.

1001

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 84 84Z r

D

9 5 S h ZX :

80 Sr 8 4 Nb

D

9 5 S h ZX :

88Tc(β+),(EC)

RADIOACTIVITY MeV];

80Y(β+),(EC)

[from

58Ni(32S,np),E=100,102

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata. 88Tc(β+),(EC)

RADIOACTIVITY MeV]; 80 Sr

[from

54Fe(28Si,np),E=88

80Y(β+),(EC)

[from

[from

58Ni(32S,np),E=100,102

54Fe(28Si,np),E=88

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata.

A = 85 8 5 Nb

R

9 3 T o ZV :

NUCLEAR REACTIONS

5 8 Ni( 3 2 S,pα),E=110,125

MeV; measured Eγ,Iγ,γγ–coin.

8 5 Nb

deduced high–spin levels,J,π.

NORDBALL spectrometer,n–,γ–multiplicity filter. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P86, Tomura.

A = 86 8 6 Nb

D

9 3 ShZT :

86Mo(β+)

RADIOACTIVITY

[from

54Fe(35Cl,2np),E=103

M e V ] ; m e a s u r e d Eγ , E β , β γ ( t ) , T 1 / 2 ; d e d u c e d Q ( E C ) .

86Nb

deduced levels,J,π,T1/2 for isomer,multipolarities. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P88, Shizuma. 8 6Mo

D

9 3 ShZT :

86Mo(β+)

RADIOACTIVITY

[from

54Fe(35Cl,2np),E=103

M e V ] ; m e a s u r e d Eγ , E β , β γ ( t ) , T 1 / 2 ; d e d u c e d Q ( E C ) .

86Nb

deduced levels,J,π,T1/2 for isomer,multipolarities. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P88, Shizuma.

A = 87 8 7 Nb

R

9 6LaZZ :

NUCLEAR REACTIONS

58Ni(32S,3p),E

not given; measured γγ–coin.

87Nb

deduced high–spin levels,J,π,

superdeformed band. CONF Argonne(Nuclear Structure at the Limits) Contrib,P23,LaFosse. 8 7Mo

R

9 3 I d ZY :

NUCLEAR REACTIONS

58 Ni( 32 S,2pn),E=110–125

MeV; measured Eγ,Iγ,γγ–coin.

87 Mo

deduced high–spin levels,J,π.

NORDBALL spectrometer,n–,γ–multiplicity filter. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P91, Ideguchi.

A = 88 8 8Mo

D

9 3Od Z Y :

RADIOACTIVITY 88 Mo

9 5 S h ZX :

80 Sr

D

9 3Od Z Y : 9 5 S h ZX :

80Y(β+),(EC)

MeV]; measured E β,Eγ,βγ–,γγ–coin,T 1 / 2 ; deduced Q(EC).

[from

[from

58Ni(32S,np),E=100,102

54Fe(28Si,np),E=88

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

8 8 Tc(β + )

[from

5 8 Ni( 3 2 S,np),E=96–105

MeV]; measured E β,Eγ,βγ–,γγ–coin,T 1 / 2 ; deduced Q(EC).

deduced levels,J,π. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P95,Odahara.

RADIOACTIVITY MeV]; 80 Sr

5 8 Ni( 3 2 S,np),E=96–105

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata.

RADIOACTIVITY 88 Mo

[from

88Tc(β+),(EC)

RADIOACTIVITY MeV];

88T c

8 8 Tc(β + )

deduced levels,J,π. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P95,Odahara.

80Y(β+),(EC)

88Tc(β+),(EC)

[from

[from

58Ni(32S,np),E=100,102

54Fe(28Si,np),E=88

MeV];

84Nb(β+),(EC)

[from

58Ni(28Si,np),E=88

MeV]; measured Eγ,Eβ,γγ–coin; deduced Qβ+,Q(EC).

88Mo,84Zr,

deduced levels. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P63,Shibata.

A = 89 89Z r

D

9 5Oh Z Y :

RADIOACTIVITY

89Zr(β+)

[from

89Y(α,4n),E=50

MeV]; measured NMR,β asymmetry.

89Zr

deduced µ.

Recoil–implantation,low–temperature nuclear orientation. REPT INS 1994 Annual,P7,Ohtsubo.

A = 90 90Z r

R

9 5 Fu ZY :

NUCLEAR REACTIONS 92,94,96Zr

90 , 92 , 94 , 96 Zr(p,p'),E=65

MeV;

90 , 92 , 94 , 96 Zr(α,α'),E=70

MeV; measured momentum spectra.

90 ,

deduced strengths of isovector components for low–lying states. REPT OULNS 1994 Annual,P92,

Fujita.

1002

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 91 91Z r

R

9 4Fo ZZ :

9 0 Zr, 2 0 8 Pb(α, 3 HeX),E=120

NUCLEAR REACTIONS

MeV; measured E( 3 He),( 3 He)n–coin,nn(θ).

9 1 Zr, 2 0 9 Pb

deduced

n–decay branching ratios for high–spin states. CONF Dubna(Selected Topics Nucl Struct) Proc,P269, Fortier.

A = 92 92Z r

R

9 5 Fu ZY :

NUCLEAR REACTIONS 92,94,96Zr

90 , 92 , 94 , 96 Zr(p,p'),E=65

MeV;

90 , 92 , 94 , 96 Zr(α,α'),E=70

MeV; measured momentum spectra.

90 ,

deduced strengths of isovector components for low–lying states. REPT OULNS 1994 Annual,P92,

Fujita.

A = 94 94Z r

R

9 5 Fu ZY :

NUCLEAR REACTIONS 92,94,96Zr

90 , 92 , 94 , 96 Zr(p,p'),E=65

MeV;

90 , 92 , 94 , 96 Zr(α,α'),E=70

MeV; measured momentum spectra.

90 ,

deduced strengths of isovector components for low–lying states. REPT OULNS 1994 Annual,P92,

Fujita.

A = 96 96Z r

R

9 5 Fu ZY :

NUCLEAR REACTIONS 92,94,96Zr

90 , 92 , 94 , 96 Zr(p,p'),E=65

MeV;

90 , 92 , 94 , 96 Zr(α,α'),E=70

MeV; measured momentum spectra.

90 ,

deduced strengths of isovector components for low–lying states. REPT OULNS 1994 Annual,P92,

Fujita.

A = 100 1 0 0Mo

D

9 5E j ZY :

RADIOACTIVITY

116Cd,100Mo(2β);

measured E(2β) following 2β–decay; deduced lower limits of T1/2 for

2ν–accompanied 2–β–decay and 0ν–accompanied 2–β–decays,matrix elements. Ultra–low background, high–sensitivity counter ELEGANT V. REPT RCNP 1994 Annual,P49,Ejiri. 9 5E j ZZ :

RADIOACTIVITY

1 1 6 Cd(2β); 1 0 0 Mo(2β);

measured sum of Eβ's following 0ν–,2ν–accompanied 2β–decay; deduced

nuclear matrix elements,lower limits of T1/2. Ultra–low background high–sensitivity detector ELEGANT V. REPT OULNS 1994 Annual,P23,Ejiri. 1 0 0 Ru

D

9 5K e Z Z :

RADIOACTIVITY

100Rh(β+),(EC);

meaasured Eγ,Iγ,γγ–coin,T1/2.

100Ru

deduced levels,J,π,Iβ,δ,γ

multipolarity. Interacting boson model interpretation,algebraic SU(5) limit. THESIS G Kenchian, Univ de Sao Paulo. 1 0 0 Rh

D

9 5K e Z Z :

RADIOACTIVITY

100Rh(β+),(EC);

meaasured Eγ,Iγ,γγ–coin,T1/2.

100Ru

deduced levels,J,π,Iβ,δ,γ

multipolarity. Interacting boson model interpretation,algebraic SU(5) limit. THESIS G Kenchian, Univ de Sao Paulo. 100Sn

D

9 5S c ZZ :

RADIOACTIVITY

102,100Sn(β+),104Sb(β+); 108Te(β+),(α)

[from

9Be(124Xe,X),E=1.095

GeV/nucleon]; measured

decay characteristics. REPT GSI–94–1,P26,Schneider. R

9 4Pe ZZ :

NUCLEAR REACTIONS,ICPND Ni( 112 Sn,X) 100 Sn,E not given; measured yields; deduced evidence for

100 Sn.

CONF

Dubna(Selected Topics Nucl Struct) Proc,P255,Penionzhkevich.

A = 101 1 0 1Y

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren. 101Sn

D

9 5 J aZZ :

RADIOACTIVITY

1 0 1 Sn(β + p)

[from

5 0 Cr( 5 8 Ni,X)];

measured β–delayed Ep,Ip; deduced T 1 / 2 . REPT GSI–94–1,P27,

Janas.

A = 102 1 0 2Y

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren. 102Sn

D

9 5S c ZZ :

RADIOACTIVITY

102,100Sn(β+),104Sb(β+); 108Te(β+),(α)

decay characteristics. REPT GSI–94–1,P26,Schneider.

1003

[from

9Be(124Xe,X),E=1.095

GeV/nucleon]; measured

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 103 1 0 3Y

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren.

A = 104 104Sb

D

9 5S c ZZ :

RADIOACTIVITY

102,100Sn(β+),104Sb(β+); 108Te(β+),(α)

[from

9Be(124Xe,X),E=1.095

GeV/nucleon]; measured

decay characteristics. REPT GSI–94–1,P26,Schneider.

A = 105 1 0 5 Nb

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren.

A = 106 1 0 6 Nb

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren. 106Sn

D

9 5 I s ZZ :

RADIOACTIVITY

106,108Sn(β+),(EC)

[from

54Fe(56Fe,X),E=210

MeV]; measured g–factors. Doppler–shift tof.

REPT JAERI–TV 1994 Annual,P15,Ishii.

A = 107 1 0 7 Nb

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren.

A = 108 1 0 8 Nb

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren. 108Sn

D

9 5 I s ZZ :

RADIOACTIVITY

106,108Sn(β+),(EC)

[from

54Fe(56Fe,X),E=210

MeV]; measured g–factors. Doppler–shift tof.

REPT JAERI–TV 1994 Annual,P15,Ishii. 108T e

D

9 5S c ZZ :

RADIOACTIVITY

102,100Sn(β+),104Sb(β+); 108Te(β+),(α)

[from

9Be(124Xe,X),E=1.095

GeV/nucleon]; measured

decay characteristics. REPT GSI–94–1,P26,Schneider.

A = 109 1 0 9 Nb

D

9 5Me Z Z :

RADIOACTIVITY

1 0 1 , 1 0 2 , 1 0 3 Y, 1 0 5 , 1 0 6 , 1 0 7 , 1 0 8 , 1 0 9 Nb(β – );

measured T 1 / 2 ,β–gated neutron spectra. REPT Univ Mainz,

1994 Annual,P31,Mehren.

A = 112 112Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke. 9 5Mo ZW :

NUCLEAR REACTIONS ratios.

112Sb

8 9 Y( 2 9 Si,2nα),E=108

MeV;

8 8 Sr( 2 8 Si,3np),E=120

MeV; measured Eγ,Iγ,γγp–,γγ–coin,DCO

deduced levels,J,π,high–spin bands. BGO suppressed hyperpure Ge detector. REPT UTTAC 1994

Annual,P36,Moon,UTTAC–62.

A = 114 1 1 4Cd

R

9 4Kh Z X :

NUCLEAR REACTIONS

113Cd(n,γ),E=thermal;

m e a s u r e d Eγ , γ γ – c o i n .

114Cd

deduced levels. Coincidence pulse

amplitude sum method,Ge(Li) detectors. CONF Dubna(Selected Topics Nucl Structure) Contrib,P106,Khitrov. 114Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

1004

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 115 115

In

R

9 4Du Z Y :

NUCLEAR REACTIONS,ICPND

115 In(γ,γ') 115 In/ 115m In,E=3–5

deduced excitation mechanism.

115mIn

MeV bremsstrahlung; measured

115m In

production σ(E);

deduced cluster character. Quasiparticle–phonon model. CONF

Dubna(Selected Topics Nucl Structure) Contrib,P34,Dubensky.

A = 116 1 1 6Cd

D

9 5E j ZY :

RADIOACTIVITY

116Cd,100Mo(2β);

measured E(2β) following 2β–decay; deduced lower limits of T1/2 for

2ν–accompanied 2–β–decay and 0ν–accompanied 2–β–decays,matrix elements. Ultra–low background, high–sensitivity counter ELEGANT V. REPT RCNP 1994 Annual,P49,Ejiri. 9 5E j ZZ :

RADIOACTIVITY

1 1 6 Cd(2β); 1 0 0 Mo(2β);

measured sum of Eβ's following 0ν–,2ν–accompanied 2β–decay; deduced

nuclear matrix elements,lower limits of T1/2. Ultra–low background high–sensitivity detector ELEGANT V. REPT OULNS 1994 Annual,P23,Ejiri. 116Sn

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl. 9 4K r Z Z :

NUCLEAR REACTIONS

116 , 124 Sn, 150 Nd, 208 Pb(α,α'),E=120

(α,α'),E=14–20 MeV; measured σ(θ).

MeV; measured GDR excitation σ(θ),γα–coin.

116,124Sn,150Nd,208Pb

150 Nd(α,α),

deduced proton,neutron density distribution

differences,deformation parameters. DWBA,deformed optical model. CONF Dubna(Selected Topics Nucl Struct) Proc,P86,Krasznahorkay. 116Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

A = 117 117Sb

R

9 3 J aZZ :

NUCLEAR REACTIONS

1 2 , 1 3 , 1 4 C, 1 1 7 , 1 2 0 Sn( 3 He,t),E=200

MeV; measured σ(Et,θ).

1 1 7 , 1 2 0 Sb

deduced Gamow–Teller

strength fragmentation,configuration splitting. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P304, Janecke. 9 3K o Z L :

NUCLEAR REACTIONS

1 1 6 Sn(polar ized

p,p),E=6.8–7.01 MeV; measu r ed σ(E),an alyzing power A(z)(θ ,E).

1 1 7 Sb

deduced parity nonconservation effect,IAR excitation. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992, P29,Kouda. 9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

A = 118 118Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

A = 119 119Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

A = 120 120Sn

R

9 4ThZZ :

NUCLEAR REACTIONS

120 Sn(α,α'γ),E=160,200

MeV;

208 Pb(α,α'γ),E=160

MeV; measured σ(Eα'),αγ–coin.

120 Sn, 208 Pb

deduced GDR width vs excitation energy. CONF Dubna(Selected Topics Nucl Struct) Proc,P224,Thoennessen. 120Sb

R

9 3 J aZZ :

NUCLEAR REACTIONS

1 2 , 1 3 , 1 4 C, 1 1 7 , 1 2 0 Sn( 3 He,t),E=200

MeV; measured σ(Et,θ).

1 1 7 , 1 2 0 Sb

deduced Gamow–Teller

strength fragmentation,configuration splitting. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P304, Janecke. 9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke.

1005

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 122 122Sb

R

9 4 J aZZ :

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

NUCLEAR REACTIONS 120,122,124Sb

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke. 1 2 2C s

R

9 5K o Z T :

NUCLEAR REACTIONS

MeV; measured Eγ,Iγ,γγ–coin,γγ(θ).

111Cd(14N,3n),E=59

deduced levels,J,π,

122Cs

high–spin bands. BGO suppressed hyperpure Ge detector. REPT UTTAC 1994 Annual,P33,Komatsubara,UTTAC–62.

A = 124 124Sn

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl. 9 4K r Z Z :

NUCLEAR REACTIONS

116 , 124 Sn, 150 Nd, 208 Pb(α,α'),E=120

(α,α'),E=14–20 MeV; measured σ(θ).

MeV; measured GDR excitation σ(θ),γα–coin.

116,124Sn,150Nd,208Pb

150 Nd(α,α),

deduced proton,neutron density distribution

differences,deformation parameters. DWBA,deformed optical model. CONF Dubna(Selected Topics Nucl Struct) Proc,P86,Krasznahorkay. 124Sb

R

9 4 J aZZ :

NUCLEAR REACTIONS 120,122,124Sb

112 , 114 , 116 , 117 , 118 , 119 , 120 , 122 , 124 Sn( 3 He,t),E=200

MeV; measured σ(θ).

112 , 114 , 116 , 117 , 118 , 119 ,

deduced Gamow–Teller resonances,Γ,fragmentations. Enriched targets. CONF Dubna(Selected

Topics Nucl Struct) Proc,P29,Janecke. 124T e

R

9 4Kh Z Y :

123Te(n,γ),E=thermal;

NUCLEAR REACTIONS

measured Eγ,γγ–coin.

124Te

deduced levels. Coincidence pulse

amplitude sum method,Ge(Li) detectors. CONF Dubna(Selected Topics Nucl Structure) Contrib,P105,Khitrov.

A = 125 125La

D

9 4A s ZY :

RADIOACTIVITY

1 2 5 Ce(β + )

measured Eγ,γγ–coin,βγ(t). 1 2 5C e

D

9 4A s ZY :

RADIOACTIVITY

1 2 5 Ce(β + )

measured Eγ,γγ–coin,βγ(t). 9 5O s ZY :

RADIOACTIVITY 125 , 126 Ce

125P r

D

9 5O s Z Y :

9 2 Mo( 3 6 Ar,n2p),E=195

[from

9 2 Mo( 3 6 Ar,n2p),E=195

125 , 126 La

MeV];

1 2 6 Ce(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,2n2p),E=195

MeV];

deduced levels. REPT JAERI–TIARA 1993 Annual,P171,Asai. MeV];

1 2 6 Ce(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,2n2p),E=195

MeV];

deduced levels. REPT JAERI–TIARA 1993 Annual,P171,Asai.

1 2 5 , 1 2 6 Pr(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,xnp),E=5.4

MeV/nucleon]; measured Eγ,Iγ,βγ–,γγ–coin,T 1 / 2 .

deduced levels,J,π,B(E2) ratio. ISOL. REPT JAERI–TIARA 1994 Annual,P181,Osa.

RADIOACTIVITY 125 , 126 Ce

[from

125 , 126 La

1 2 5 , 1 2 6 Pr(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,xnp),E=5.4

MeV/nucleon]; measured Eγ,Iγ,βγ–,γγ–coin,T 1 / 2 .

deduced levels,J,π,B(E2) ratio. ISOL. REPT JAERI–TIARA 1994 Annual,P181,Osa.

A = 126 1 2 6Ba

D

9 5A s ZZ :

RADIOACTIVITY 152 Gd, 126 Ba

126La

D

9 4A s ZY :

1 5 2 Eu(β – ),(β + ),(EC); 1 2 6 La(β + ),(EC)

RADIOACTIVITY

1 2 5 Ce(β + )

measured Eγ,γγ–coin,βγ(t). 9 5A s ZZ :

RADIOACTIVITY 152 Gd, 126 Ba

1 2 6C e

D

9 4A s ZY :

RADIOACTIVITY RADIOACTIVITY 125 , 126 Ce

126P r

D

9 5O s Z Y :

MeV]; measured γγ(θ).

1 5 2 Sm,

[from

9 2 Mo( 3 6 Ar,n2p),E=195

125 , 126 La

MeV];

1 2 6 Ce(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,2n2p),E=195

MeV];

deduced levels. REPT JAERI–TIARA 1993 Annual,P171,Asai.

1 5 2 Eu(β – ),(β + ),(EC); 1 2 6 La(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,n3p),E=195

MeV]; measured γγ(θ).

1 5 2 Sm,

1 2 5 Ce(β + )

[from

9 2 Mo( 3 6 Ar,n2p),E=195

125 , 126 La

MeV];

1 2 6 Ce(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,2n2p),E=195

MeV];

deduced levels. REPT JAERI–TIARA 1993 Annual,P171,Asai.

1 2 5 , 1 2 6 Pr(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,xnp),E=5.4

MeV/nucleon]; measured Eγ,Iγ,βγ–,γγ–coin,T 1 / 2 .

deduced levels,J,π,B(E2) ratio. ISOL. REPT JAERI–TIARA 1994 Annual,P181,Osa.

RADIOACTIVITY 125 , 126 Ce

9 4 Mo( 3 6 Ar,n3p),E=195

deduced A 2 ,A 4 for γγ(θ). ISOL. REPT JAERI–TIARA 1994 Annual,P184,Asai.

measured Eγ,γγ–coin,βγ(t). 9 5O s ZY :

[from

deduced A 2 ,A 4 for γγ(θ). ISOL. REPT JAERI–TIARA 1994 Annual,P184,Asai.

1 2 5 , 1 2 6 Pr(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,xnp),E=5.4

MeV/nucleon]; measured Eγ,Iγ,βγ–,γγ–coin,T 1 / 2 .

deduced levels,J,π,B(E2) ratio. ISOL. REPT JAERI–TIARA 1994 Annual,P181,Osa.

A = 127 1 2 7C e

D

9 4 S e ZY :

RADIOACTIVITY T 1/2 ; deduced T 1/2 .

127P r

D

9 4 S e ZY :

RADIOACTIVITY T 1/2 ; deduced T 1/2 .

1 2 7 Pr(β + ),(EC) 127 Ce

1 2 7 Pr(β + ),(EC) 127 Ce

[from

9 4 Mo( 3 6 Ar,2np),E=5.4

MeV/nucleon]; measured E β,Eγ,X–rays,βγ–,γγ–coin,

deduced levels,J, π. REPT JAERI–TIARA 1993 Annual,P166,Sekine. [from

9 4 Mo( 3 6 Ar,2np),E=5.4

MeV/nucleon]; measured E β,Eγ,X–rays,βγ–,γγ–coin,

deduced levels,J, π. REPT JAERI–TIARA 1993 Annual,P166,Sekine.

A = 128 128La

R

9 5Ha ZU :

NUCLEAR REACTIONS

9 8 Mo( 3 7 Cl,3nα),E=145

MeV;

1 1 5 In( 1 6 O,3n),E=68

MeV; measured Eγ,Iγ,γγ–coin,γγ(θ).

1 2 8 La

deduced levels,J,π,high–spin bands. BGO suppressed hyperpure Ge detector. REPT UTTAC 1994 Annual,P40, Hayakawa,UTTAC–62.

1006

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 131 1 3 1C e

R

9 4N o Z X :

NUCLEAR REACTIONS

100Mo(36S,X),E=155

MeV; measured γγ–,γγγ–,γγγγ–coin.

131,132Ce

deduced levels,

configuration,band structure. CONF Berkeley(Phys Large γ–Ray Detector Arrays) Proc,P99,Nolan. 9 4Wa ZV :

NUCLEAR REACTIONS

1 1 0 Pd( 2 6 Mg,4n),( 2 6 Mg,5n),E=130

MeV; measured γ line shapes,centroid shifts.

1 3 1 , 1 3 2 Ce

deduced levels,T1/2,superdeformed bands intrinsic quadrupole moments. CONF Berkeley(Phys Large γ–Ray Detector Arrays) Contrib,P4,Ward.

A = 132 1 3 2Ba

R

9 5LuZZ :

1 2 4 Sn( 1 3 C,5n),E=72

NUCLEAR REACTIONS

MeV; measured E γ,Iγ,γγ–coin,DCO ratios.

1 3 2 Ba

deduced levels,J,π,

high–spin bands. REPT UTTAC 1994 Annual,P45,Lu,UTTAC–62. 1 3 2C e

R

9 4N o Z X :

NUCLEAR REACTIONS

100Mo(36S,X),E=155

MeV; measured γγ–,γγγ–,γγγγ–coin.

131,132Ce

deduced levels,

configuration,band structure. CONF Berkeley(Phys Large γ–Ray Detector Arrays) Proc,P99,Nolan. 9 4Wa ZV :

NUCLEAR REACTIONS

1 1 0 Pd( 2 6 Mg,4n),( 2 6 Mg,5n),E=130

MeV; measured γ line shapes,centroid shifts.

1 3 1 , 1 3 2 Ce

deduced levels,T1/2,superdeformed bands intrinsic quadrupole moments. CONF Berkeley(Phys Large γ–Ray Detector Arrays) Contrib,P4,Ward.

A = 133 1 3 3X e

D

9 4Mu Z X :

RADIOACTIVITY

1 3 3 Xe(β – );

measured γ–spectra,I(ce). Iron–free β–ray spectrometer. REPT JAERI–TIARA 1993

Annual,P169,Muramatsu. 9 5Mu Z X :

RADIOACTIVITY

133Xe(β–);

measured E(ce),I(ce),Mossbauer isomer shift.

133Cs

deduced change of nuclear

charge radius. Ion implantation technique. REPT JAERI–TIARA 1994 Annual,P190,Muramatsu. 9 5Mu Z Y :

RADIOACTIVITY

1 3 3 Xe( β – );

measu r ed Mossbauer spec tr a,(c e).

1 3 3 Cs

deduc ed nu c lear c har ge r adiu s. Iron–free

double–focusing β–ray spectrometer. REPT INS 1994 Annual,P16,Muramatsu. 1 3 3C s

D

9 5Mu Z X :

RADIOACTIVITY

133Xe(β–);

measured E(ce),I(ce),Mossbauer isomer shift.

133Cs

deduced change of nuclear

charge radius. Ion implantation technique. REPT JAERI–TIARA 1994 Annual,P190,Muramatsu. 9 5Mu Z Y :

RADIOACTIVITY

1 3 3 Xe( β – );

measu r ed Mossbauer spec tr a,(c e).

1 3 3 Cs

deduc ed nu c lear c har ge r adiu s. Iron–free

double–focusing β–ray spectrometer. REPT INS 1994 Annual,P16,Muramatsu.

A = 134 1 3 4Ba

R

9 4Kn Z Z :

NUCLEAR REACTIONS

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

A = 136 1 3 6X e

R

9 4Ku Z P :

NUCLEAR REACTIONS C,Pb( 136 Xe, 136 Xe'),E=700 MeV/nucleon; Pb( 208 Pb, 208 Pb'),E=650 MeV/nucleon; measured σ vs excitation energy.

136Xe,208Pb

deduced double GDR,Γ. Other data input. CONF Dubna(Selected Topics Nucl

Struct) Proc,P39,Kulessa. 1 3 6Ba

R

9 4Kn Z Z :

NUCLEAR REACTIONS

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

A = 137 1 3 7Ba

R

9 4Bo ZS :

NUCLEAR REACTIONS

137Ba(n,γ),(n,n'γ),E=reactor;

measured γγ–coin,spectra.

137Ba

deduced levels,J,π,

configurations. Interacting boson–fermion model. CONF Dubna(Selected Topics Nucl Structure) Contrib,P23, Bondarenko.

A = 138 1 3 8Ba

R

9 4Kn Z Z :

NUCLEAR REACTIONS measured Eγ,asymmetry.

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4 116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

1007

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 140 1 4 0C e

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

A = 142 1 4 2 Nd

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

A = 143 1 4 3 Nd

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl.

A = 144 1 4 4 Nd

R

9 4B l ZX :

1 4 2 , 1 4 4 , 1 4 6 , 1 4 8 , 1 5 0 Nd(p,p'),E=30.5

NUCLEAR REACTIONS 148Nd(p,t),E=25

MeV; measured σ(θ).

144,146Nd

1 4 2 , 1 4 4 , 1 4 6 Nd(p,t),E=35.6

MeV; (d,d'),E=50.8 MeV;

MeV;

levels deduced B(λ). Quasiparticle–phonon model. CONF

Dubna(Selected Topics Nucl Struct) Proc,P160,Blasi. 1 4 4 Pm

R

9 3G o ZM :

1 4 4 Gd

R

9 6U t Z Z :

1 4 N( 1 3 6 Xe,6n), 1 6 O( 1 3 6 Xe,7n), 2 0 Ne( 1 3 6 Xe,7nα),E=8.5,10

NUCLEAR REACTIONS 144 Pm, 145 Sm

MeV/nucleon; measured Eγ,Iγ,γγ(t).

deduced levels,high–spin isomers. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P99,Gono.

NUCLEAR REACTIONS

100 Mo( 48 Ti,4n),E=215,209

MeV; measured γγ–coin.

144 Gd

deduced superdeformed band. REPT

1 4 N( 1 3 6 Xe,6n), 1 6 O( 1 3 6 Xe,7n), 2 0 Ne( 1 3 6 Xe,7nα),E=8.5,10

MeV/nucleon; measured Eγ,Iγ,γγ(t).

KFA–IKP 1995 Annual,P133,Utzelmann.

A = 145 1 4 5 Sm

R

9 3G o ZM :

NUCLEAR REACTIONS 144 Pm, 145 Sm

9 3Od Z X :

deduced levels,high–spin isomers. REPT Kyushu Univ Tandem Acc Lab Rept,1991–1992,P99,Gono. 2 0 Ne( 1 3 6 Xe,7nα),E=8.5,10

NUCLEAR REACTIONS 145Sm

MeV/nucleon;

1 3 9 La( 1 0 B,4n),E=47

MeV; measured Eγ,Iγ,γγ–coin.

deduced levels,J,π,high–spin isomers related features. REPT Kyushu Univ Tandem Acc Lab Rept,

1991–1992,P104,Odahara. 9 5Od Z Z :

1 3 9 La( 1 0 B,4n),E=47

NUCLEAR REACTIONS

MeV;

2 0 Ne( 1 3 6 Xe,7nα),E=8.2

not given; measured Eγ,Iγ,γγ–coin,γ(θ).

16O(136Xe,7n),E

MeV/nucleon;

145,145mSm

1 3 8 Ba( 1 3 C,6n),E=95

MeV;

deduced high–spin levels,J,π,T1/2,

deformation parameters. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P66,Odahara.

A = 146 1 4 6 Nd

R

9 4B l ZX :

1 4 2 , 1 4 4 , 1 4 6 , 1 4 8 , 1 5 0 Nd(p,p'),E=30.5

NUCLEAR REACTIONS 148Nd(p,t),E=25

MeV; measured σ(θ).

144,146Nd

MeV; (d,d'),E=50.8 MeV;

1 4 2 , 1 4 4 , 1 4 6 Nd(p,t),E=35.6

MeV;

levels deduced B(λ). Quasiparticle–phonon model. CONF

Dubna(Selected Topics Nucl Struct) Proc,P160,Blasi. 9 4Ya ZT :

146Nd(n,n'γ),E

NUCLEAR REACTIONS measured Eγ,Iγ,γ(θ),DSA.

146Nd

not given; measured not abstracted.

162,164Dy(n,n'γ),E

deduced levels,branching ratios,B(λ),configurations.

not given;

162,164Dy

deduced

levels,J,π,T 1/2 . CONF Dubna(Selected Topics Nucl Struct) Proc,P300,Yates. 1 4 6 Gd

D

9 5Ka Z Y :

RADIOACTIVITY

1 4 6 Gd(EC),(β + )

[from

1 4 4 Sm(α,2n),E=23.5

MeV]; measured γ(θ,H).

1 4 6 Gd

deduced g–factor. REPT

CYRIC 1994 Annual,P22,Kawamura. R

9 4D e ZV :

NUCLEAR REACTIONS

160Gd,162Dy(36S,4n),E=168

superdeformed band levels T1/2.

Mev; measured Eγ,recoil distances.

122Sn(29Si,5n),E=155,158

MeV; measured DSA.

192Hg,194Pt

146Gd

deduced

deduced intrinsic

quadrupole moments for superdeformed bands. CONF Dubna(Selected Topics Nucl Struct) Proc,P368,Dewald. 9 5Ka Z Y :

NUCLEAR REACTIONS

144 Sm(α,2n),E

= 23.5 MeV; measured γ(θ,H).

146 Gd

deduced isomer g factor. REPT CYRIC

1994 Annual,P22,Kawamura.

A = 147 1 4 7 Gd

R

9 4 V i ZV :

NUCLEAR REACTIONS

122Sn(30Si,5n),E=158

MeV; measured γ spectra.

147Gd

deduced high–spin levels,

superdeformed band. CONF Berkeley(Phys Large γ–Ray Detector Arrays) Contrib,P15,Vivien.

1008

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 148 148Tb

R

9 5 I d ZX :

1 4 1 Pr( 1 3 C,6n),E=95,98,100,108

NUCLEAR REACTIONS

MeV; measured E γ,Iγ(θ),γγ–coin,DCO,T 1 / 2 .

1 4 8 Tb

deduced

high–spin levels,J,π. REPT RIKEN–94,P53,Ideguchi. 9 5 I d ZY :

NUCLEAR REACTIONS γ(θ).

9 5 I dZZ :

148 Tb

141 Pr( 13 C,6n),E=95,100,108

MeV;

27 Al( 130 Te,9n),E=7.5

MeV/nucleon; measured Eγ,Iγ,γγ–coin,

deduced high–spin levels,J, π. REPT Kyushu Univ Tandem Acc Lab Rept,1993–1994,P72,Ideguchi. 141Pr(13C,6n),E=95,98,100,108

NUCLEAR REACTIONS

MeV; measured Eγ,Iγ,σ(E),γ(θ),γγ–coin.

148Tb

deduced

high–spin levels,J,π,isomer. REPT JAERI–TV 1994 Annual,P13,Ideguchi.

A = 150 1 5 0 Nd

R

9 4Kn Z Z :

1 1 6 , 1 2 4 Sn, 1 3 4 , 1 3 6 , 1 3 8 Ba, 1 4 0 Ce, 1 4 2 , 1 4 3 , 1 5 0 Nd, 1 6 0 Gd, 1 6 2 , 1 6 4 Dy(γ,γ'),E=4

NUCLEAR REACTIONS measured Eγ,asymmetry.

116,124Sn,134,136,138Ba,140Ce,142,143,150Nd

MeV bremsstrahlung;

deduced γ multipolarity,Γ,B(E1). CONF

Dubna(Selected Topics Nucl Struct) Proc,P290,Kneissl. 9 4K r Z Z :

NUCLEAR REACTIONS

116 , 124 Sn, 150 Nd, 208 Pb(α,α'),E=120

(α,α'),E=14–20 MeV; measured σ(θ).

MeV; measured GDR excitation σ(θ),γα–coin.

116,124Sn,150Nd,208Pb

150 Nd(α,α),

deduced proton,neutron density distribution

differences,deformation parameters. DWBA,deformed optical model. CONF Dubna(Selected Topics Nucl Struct) Proc,P86,Krasznahorkay.

A = 152 1 5 2 Sm

D

9 5A s ZZ :

RADIOACTIVITY 152 Gd, 126 Ba

1 5 2 Eu

D

9 5A s ZZ :

RADIOACTIVITY 152 Gd, 126 Ba

R

9 3 V i ZU :

1 5 2 Eu(β – ),(β + ),(EC); 1 2 6 La(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,n3p),E=195

MeV]; measured γγ(θ).

1 5 2 Sm,

deduced A 2 ,A 4 for γγ(θ). ISOL. REPT JAERI–TIARA 1994 Annual,P184,Asai. 1 5 2 Eu(β – ),(β + ),(EC); 1 2 6 La(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,n3p),E=195

MeV]; measured γγ(θ).

1 5 2 Sm,

deduced A 2 ,A 4 for γγ(θ). ISOL. REPT JAERI–TIARA 1994 Annual,P184,Asai.

NUCLEAR REACTIONS

1 5 1 Eu, 1 8 1 Ta, 1 9 7 Au(n,γ),E=thermal;

measured isomeric ratios,γ–spectra.

1 5 2 Eu, 1 8 2 Ta, 1 9 8 Au

deduced transition feature. CONF Dubna,P75,Vishnevsky. 1 5 2 Gd

D

9 5A s ZZ :

RADIOACTIVITY 152 Gd, 126 Ba

1 5 2 Eu(β – ),(β + ),(EC); 1 2 6 La(β + ),(EC)

[from

9 4 Mo( 3 6 Ar,n3p),E=195

MeV]; measured γγ(θ).

1 5 2 Sm,

deduced A 2 ,A 4 for γγ(θ). ISOL. REPT JAERI–TIARA 1994 Annual,P184,Asai.

A = 153 1 5 3 Gd

R

9 6SpZZ :

NUCLEAR REACTIONS 154Gd

153,152Gd(n,γ),E=thermal;

measured Eγ,Iγ,I(ce); deduced capture σ(E) for

153Gd. 153,

deduced levels,J,π,γ–multipolarity,B(λ),neutron binding energies. Double neutron capture on

152Gd.

REPT BLG 703,Spits.

A = 154 1 5 4 Gd

R

9 6SpZZ :

NUCLEAR REACTIONS 154Gd

153,152Gd(n,γ),E=thermal;

measured Eγ,Iγ,I(ce); deduced capture σ(E) for

153Gd. 153,

deduced levels,J,π,γ–multipolarity,B(λ),neutron binding energies. Double neutron capture on

152Gd.

REPT BLG 703,Spits.

A = 155 1 5 5D y

R

9 6F i ZZ :

NUCLEAR REACTIONS

1 2 4 Sn( 3 6 S,5n),E=175

MeV; measured γγ–coin.

1 5 5 Dy

deduced superdeformed band. CONF

Argonne(Nuclear Structure at the Limits) Contrib,P14,Fischer.

A = 156 1 5 6 Ho

R

9 5 Bh Z Y :

NUCLEAR REACTIONS

1 4 0 Ce( 1 9 F,3n),E=79,82,85

MeV; measured Eγ,Iγ,γγ–coin,γγ(θ),DCO ratios.

1 5 6 Ho

deduced

levels,J,π,high–spin bands. BGO suppressed hyperpure Ge detector. REPT UTTAC 1994 Annual,P30,Bhatti, UTTAC–62.

A = 160 1 6 0D y

R

9 4P i ZZ :

NUCLEAR REACTIONS 164Dy

160 , 161 , 162 , 163 , 164 Dy(γ,γ'),E=4

MeV bremsstrahlung; measured Eγ,asymmetry.

160 , 161 , 162 , 163 ,

deduced levels,Γ,dipole transition strength distributions. Other data reviewed. CONF

Dubna(Selected Topics Nucl Struct) Proc,P319,Pitz.

1009

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 161 1 6 1D y

R

9 4P i ZZ :

NUCLEAR REACTIONS 164Dy

160 , 161 , 162 , 163 , 164 Dy(γ,γ'),E=4

MeV bremsstrahlung; measured Eγ,asymmetry.

160 , 161 , 162 , 163 ,

deduced levels,Γ,dipole transition strength distributions. Other data reviewed. CONF

Dubna(Selected Topics Nucl Struct) Proc,P319,Pitz.

A = 162 1 6 2D y

R

9 3 An Z P :

NUCLEAR REACTIONS

161 Dy(α, 3 He), 163 Dy( 3 He,α),E=50

Mev; measured σ(Eα,θ),σ(E( 3 He),θ).

162 Dy

deduced levels,J,

π,L,band structure. Enriched targets,magnetic spectrograph. DWBA,comparison with other Dy isotopes. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P7,Andersen. 9 4P i ZZ :

NUCLEAR REACTIONS 164Dy

160 , 161 , 162 , 163 , 164 Dy(γ,γ'),E=4

MeV bremsstrahlung; measured Eγ,asymmetry.

160 , 161 , 162 , 163 ,

deduced levels,Γ,dipole transition strength distributions. Other data reviewed. CONF

Dubna(Selected Topics Nucl Struct) Proc,P319,Pitz. 9 4Ya ZT :

146Nd(n,n'γ),E

NUCLEAR REACTIONS measured Eγ,Iγ,γ(θ),DSA.

146Nd

not given; measured not abstracted.

162,164Dy(n,n'γ),E

deduced levels,branching ratios,B(λ),configurations.

not given;

162,164Dy

deduced

levels,J,π,T 1/2 . CONF Dubna(Selected Topics Nucl Struct) Proc,P300,Yates.

A = 163 1 6 3D y

R

9 4P i ZZ :

NUCLEAR REACTIONS 164Dy

160 , 161 , 162 , 163 , 164 Dy(γ,γ'),E=4

MeV bremsstrahlung; measured Eγ,asymmetry.

160 , 161 , 162 , 163 ,

deduced levels,Γ,dipole transition strength distributions. Other data reviewed. CONF

Dubna(Selected Topics Nucl Struct) Proc,P319,Pitz. 1 6 3Lu

R

9 2 S c ZL :

1 3 9 La( 2 8 Si,xnyp),E=150

NUCLEAR REACTIONS distance.

163Lu

MeV;

1 4 7 Sm( 1 9 F,xnyp),E=85

MeV; measured γγ–coin,DSA,recoil

deduced high–spin levels,J,π,band structure,Nilsson assignment,shape coexistence,B(λ).

THESIS W Schmitz,Rheinischen Friedrich–Wilhelms–Univ,Bonn.

A = 164 1 6 4D y

R

9 4P i ZZ :

NUCLEAR REACTIONS 164Dy

160 , 161 , 162 , 163 , 164 Dy(γ,γ'),E=4

MeV bremsstrahlung; measured Eγ,asymmetry.

160 , 161 , 162 , 163 ,

deduced levels,Γ,dipole transition strength distributions. Other data reviewed. CONF

Dubna(Selected Topics Nucl Struct) Proc,P319,Pitz. 9 4Ya ZT :

NUCLEAR REACTIONS

146Nd(n,n'γ),E

measured Eγ,Iγ,γ(θ),DSA.

146Nd

not given; measured not abstracted.

162,164Dy(n,n'γ),E

deduced levels,branching ratios,B(λ),configurations.

not given;

162,164Dy

deduced

levels,J,π,T 1/2 . CONF Dubna(Selected Topics Nucl Struct) Proc,P300,Yates. 9 5O s Z Z :

NUCLEAR REACTIONS

164Dy(74Ge,74Ge'),E=295

MeV;

γ(particle)–coin following Coulomb excitation.

164Dy(58Ni,58Ni'),E=235

164Dy

MeV; measured Eγ,Iγ,γγ–,

deduced levels,J,π,B(E2). Multiple Coulomb

excitation. REPT JAERI–TV 1994 Annual,P11,Oshima.

A = 166 166Tb

D

9 5T s ZZ :

RADIOACTIVITY

1 6 6 Tb(β – )

[from

2 3 8 U(p,F),E=16

MeV]; measured Eγ,βγ–coin,T 1 / 2 .

1 6 6 Dy

deduced levels. On–line

1 6 6 Dy

deduced levels. On–line

mass separator. REPT JAERI–TV 1994 Annual,P16,Tsukada. 1 6 6D y

D

9 5T s ZZ :

RADIOACTIVITY

1 6 6 Tb(β – )

[from

2 3 8 U(p,F),E=16

MeV]; measured Eγ,βγ–coin,T 1 / 2 .

mass separator. REPT JAERI–TV 1994 Annual,P16,Tsukada. 1 6 6E r

D

9 3Ad ZY :

RADIOACTIVITY A4.

1 6 6 Tm

D

9 3Ad ZY :

166 Er

RADIOACTIVITY A4.

166 Er

166 Tm(EC),(β + )

[from

166 Yb

decay produced by Ta(p,X),E=660 MeV]; measured γγ(θ); deduced A 2 ,

transitions deduced δ. Ge(Li) detectors. CONF Dubna,P388,Adam. 166 Tm(EC),(β + )

[from

166 Yb

decay produced by Ta(p,X),E=660 MeV]; measured γγ(θ); deduced A 2 ,

transitions deduced δ. Ge(Li) detectors. CONF Dubna,P388,Adam.

A = 170 170P t

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth.

A = 171 1 7 1E r

D

9 3 Bu ZW :

RADIOACTIVITY

171Er(β–);

measured Auger spectra.

Magnetic β–spectrometer. CONF Dubna,P192,Bulgakov.

1010

171Tm

deduced Auger spectrum KLL–electron energies.

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 171 1 7 1 Tm

D

9 3 Bu ZW :

RADIOACTIVITY

171Er(β–);

continued

measured Auger spectra.

171Tm

deduced Auger spectrum KLL–electron energies.

Magnetic β–spectrometer. CONF Dubna,P192,Bulgakov. 171P t

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth.

A = 172 172P t

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth.

A = 173 1 7 3R e

R

9 3We Z Z :

150 Sm( 27 Al,4n),E=125

NUCLEAR REACTIONS

MeV; measured not given.

173 Re

deduced levels,J,π,T 1/2 ,deformation,

B(λ). Recoil distance,Doppler broadend line shape techniques. BAPSA 38 1014,K6 6,Wells. 173P t

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth.

A = 174 1 7 4H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. R

9 5 L i ZY :

9 Be( 170 Er,5n),E=7.0

NUCLEAR REACTIONS

MeV/nucleon; measured Eγ,Iγ,γγ–coin.

174 Hf

deduced possible isomers,

J,π,K. High–spin isomer–beam technique. REPT RIKEN–94,P54,Liu. 9 5Mo Z X :

2 0 8 Pb( 1 7 4 Hf, 1 7 4 Hf'),E

NUCLEAR REACTIONS

not given; measured Eγ.

1 7 4 Hf

deduced levels,J,π,B(E2). Projectile

Coulomb excitation,high–spin isomer–beam technique,174Hf isomer excitation by

9Be(170Er,5n)

reaction.

REPT RIKEN–94,P51,Morikawa. 9 5Mo Z Z :

NUCLEAR REACTIONS

1 7 4 Hf( 1 7 0 Er, 1 7 0 Er'),E=7.0

isomer Coulomb excitation.

174Hf

MeV/nucleon; measured E γ,Iγ,γγ–coin,γ(θ) following high–spin

deduced levels,J,π,B(E2). High–spin isomer beam technique. REPT Kyushu

Univ Tandem Acc Lab Rept,1993–1994,P75,Morikawa.

A = 176 1 7 6H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. 1 7 6W

R

9 4B r ZX :

NUCLEAR REACTIONS

148Nd(28Si,X),E=147

MeV; measured γ strength function,Iγ(θ).

176W

deduced GDR

parameters vs compound nucleus spin. CONF Dubna(Selected Topics Nucl Struct) Proc,P48,Bracco.

A = 177 1 7 7H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos.

A = 178 1 7 8H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. 1 7 8W

D

9 5FuZS :

RADIOACTIVITY

178Re(β+)

[from

180W(p,3n)];

measured γγ(t),γ(ce)(t).

178W

level deduced T1/2,B(E2). On–line

mass separation,BaF 2 scintillator. REPT CYRIC 1994 Annual,P25,Fujita. 1 7 8R e

D

9 5FuZS :

RADIOACTIVITY

178Re(β+)

[from

180W(p,3n)];

measured γγ(t),γ(ce)(t).

178W

mass separation,BaF 2 scintillator. REPT CYRIC 1994 Annual,P25,Fujita.

1011

level deduced T1/2,B(E2). On–line

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 179 1 7 9H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. 179Ta

D

9 5Wa ZV :

179Ta(EC)

RADIOACTIVITY parameters.

[from

180Hf(d,3n),179Hf(d,2n),E=19

MeV]; measured hfs; deduced hyperfine

level deduced µ,quadrupole moment. Laser–RF double–resonance spectroscopy. REPT

179Ta

RIKEN–94,P44,Wakasugi.

A = 180 1 8 0H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. 180Ta

D

9 5 J i ZZ :

180mTa;

RADIOACTIVITY

measured hfs; deduced hyperfine parameters.

180mTa

level deduced µ,quadrupole

moment. Laser–RF double–resonance spectroscopy. REPT RIKEN–94,P45,Jin. R

9 4D e ZU :

NUCLEAR REACTIONS 180 Ta

180Ta(32S,32S'γ),E=130

MeV; measured Eγ,Iγ following Coulomb excitation,(32S)γ–coin.

deduced levels,J,π. Enriched target. CONF Dubna(Selected Topics Nucl Struct) Proc,P407,de Boer.

A = 181 1 8 1H f

D

9 3 S o ZU :

RADIOACTIVITY

1 8 1 Hf(β – );

measured γγ(θ,H,t) vs T; deduced

1 8 1 Ta

magnetic hyperfine field in NdFe 2 . CONF

Dubna,P365,Sorokin. 1 8 1 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 9 3B i ZY :

RADIOACTIVITY

181,182,183,184,185,186Au,181,182,183,184,185Pt(α)

MeV]; measured Eα,Iα,αγ–coin.

181,182,183,184Au

deduced T1/2.

[from Ta(12C,X),E=153 MeV; Yb(19F,X),E=165 186Au

deduced Qα. Some transitions in Ir

isotopes identified. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P735,Bingham.

A = 182 1 8 2H f

J

9 4 B o ZR :

NUCLEAR MOMENTS

174,176,177,178m,179,180,182Hf;

measured hfs,isotope,isomeric shifts; deduced charge rms

radius differences,deformation parameters β2,quadrupole moment.

177,179Hf

deduced µ ratios. High

resolution laser spectroscopy. CONF Dubna(Selected Topics Nucl Structure) Contrib,P24,Boos. 182Ta

R

9 3 V i ZU :

NUCLEAR REACTIONS

1 5 1 Eu, 1 8 1 Ta, 1 9 7 Au(n,γ),E=thermal;

measured isomeric ratios,γ–spectra.

1 5 2 Eu, 1 8 2 Ta, 1 9 8 Au

deduced transition feature. CONF Dubna,P75,Vishnevsky. 1 8 2 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 9 3B i ZY :

RADIOACTIVITY

181,182,183,184,185,186Au,181,182,183,184,185Pt(α)

MeV]; measured Eα,Iα,αγ–coin.

181,182,183,184Au

deduced T1/2.

[from Ta(12C,X),E=153 MeV; Yb(19F,X),E=165 186Au

deduced Qα. Some transitions in Ir

isotopes identified. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P735,Bingham.

A = 183 1 8 3 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 9 3B i ZY :

RADIOACTIVITY

181,182,183,184,185,186Au,181,182,183,184,185Pt(α)

MeV]; measured Eα,Iα,αγ–coin.

181,182,183,184Au

deduced T1/2.

[from Ta(12C,X),E=153 MeV; Yb(19F,X),E=165 186Au

deduced Qα. Some transitions in Ir

isotopes identified. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P735,Bingham.

A = 184 1 8 4 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 9 3B i ZY :

RADIOACTIVITY

181,182,183,184,185,186Au,181,182,183,184,185Pt(α)

MeV]; measured Eα,Iα,αγ–coin.

181,182,183,184Au

deduced T1/2.

[from Ta(12C,X),E=153 MeV; Yb(19F,X),E=165 186Au

deduced Qα. Some transitions in Ir

isotopes identified. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P735,Bingham.

1012

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 185 185P t

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 1 8 5 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham.

A = 186 1 8 6O s

R

9 3 B a ZC :

NUCLEAR REACTIONS

1 8 6 W( α,4n),E=55

MeV; measu r ed γγ –c oin,Eγ.

1 8 6 Os

dedu c ed h igh–spin levels,J, π,shape

features. REPT KFA–IKP 1992 Annual,P92,Balabanski. 1 8 6 Au

D

9 2B i ZZ :

RADIOACTIVITY

181,182,183,184,185,186Au(α),185Pt(α);

measured Eα,Iα,Eγ,Iγ,E X–ray,I X–ray,αγ–coin,

α(X–ray)–coin; deduced daughter nuclei transitions in some cases. CONF Bernkastel–Kues(Nuclei Far from Stability) Contrib,PE47,Bingham. 9 3B i ZY :

RADIOACTIVITY

181,182,183,184,185,186Au,181,182,183,184,185Pt(α)

MeV]; measured Eα,Iα,αγ–coin.

181,182,183,184Au

deduced T1/2.

[from Ta(12C,X),E=153 MeV; Yb(19F,X),E=165 186Au

deduced Qα. Some transitions in Ir

isotopes identified. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P735,Bingham. 1 8 6 Hg

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth.

A = 188 1 8 8 Hg

R

9 3Be Z J :

NUCLEAR REACTIONS

160Gd(34S,5n),(34S,4n),(34S,6n),E

deduced high–spin levels,J,π,superdeformed bands.

not given; measured Eγ,Iγ,DCO ratios.

188Hg

189,190Hg

deduced high–spin levels,band structure,J,π.

THESIS I G Bearden Purdue Univ.

A = 189 1 8 9 Hg

R

9 3Be Z J :

NUCLEAR REACTIONS

160Gd(34S,5n),(34S,4n),(34S,6n),E

deduced high–spin levels,J,π,superdeformed bands.

not given; measured Eγ,Iγ,DCO ratios.

188Hg

189,190Hg

deduced high–spin levels,band structure,J,π.

THESIS I G Bearden Purdue Univ.

A = 190 1 9 0 Hg

D

9 3 T o ZY :

RADIOACTIVITY

1 7 0 , 1 7 1 , 1 7 2 , 1 7 3 Pt(α)

[from

1 4 4 Sm( 3 2 S,X),E=200

MeV];

1 8 6 , 1 9 0 Hg(α)

[from W( 1 2 C,X)]; measured Eα,

Iα. CONF Bernkastel–Kues(Nuclei Far from Stability) Proc,P589,Toth. R

9 3Be Z J :

NUCLEAR REACTIONS

160Gd(34S,5n),(34S,4n),(34S,6n),E

deduced high–spin levels,J,π,superdeformed bands.

not given; measured Eγ,Iγ,DCO ratios.

188Hg

189,190Hg

deduced high–spin levels,band structure,J,π.

THESIS I G Bearden Purdue Univ.

A = 192 1 9 2 Hg

R

9 4D e ZV :

NUCLEAR REACTIONS

160Gd,162Dy(36S,4n),E=168

superdeformed band levels T1/2.

Mev; measured Eγ,recoil distances.

122Sn(29Si,5n),E=155,158

MeV; measured DSA.

192Hg,194Pt

146Gd

deduced

deduced intrinsic

quadrupole moments for superdeformed bands. CONF Dubna(Selected Topics Nucl Struct) Proc,P368,Dewald.

A = 194 194

Ir

R

9 4K o ZQ :

NUCLEAR REACTIONS

193Ir(n,γ),E

not given; measured γγ–coin,γγ(t).

194Ir

deduced levels,J,π,γ–branching.

CONF Fribourg(Capture Gamma–Ray Spec Related Topics) Proc,398. 194P t

R

9 4D e ZV :

NUCLEAR REACTIONS

160Gd,162Dy(36S,4n),E=168

superdeformed band levels T1/2.

Mev; measured Eγ,recoil distances.

122Sn(29Si,5n),E=155,158

MeV; measured DSA.

192Hg,194Pt

146Gd

deduced

deduced intrinsic

quadrupole moments for superdeformed bands. CONF Dubna(Selected Topics Nucl Struct) Proc,P368,Dewald.

1013

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 198 1 9 8 Au

R

9 3 V i ZU :

1 5 1 Eu, 1 8 1 Ta, 1 9 7 Au(n,γ),E=thermal;

NUCLEAR REACTIONS

measured isomeric ratios,γ–spectra.

1 5 2 Eu, 1 8 2 Ta, 1 9 8 Au

deduced transition feature. CONF Dubna,P75,Vishnevsky.

A = 207 207Pb

R

9 5Ma Z Y :

1 2 C, 2 0 8 Pb(p,X),E=390.6

NUCLEAR REACTIONS

MeV; measured

2 He

spectra.

2 0 7 Pb

deduced deeply–bound pionic

states. REPT RCNP 1994 Annual,P3,Matsuoka.

A = 208 208Pb

R

9 4 B e ZV :

NUCLEAR REACTIONS

209 Bi, 208 Pb(γ,n),E=7–26

MeV bremsstrahlung; measured σ(E).

208 Pb

deduced isovector GQR

structure. Quasiparticle–phonon model. CONF Dubna(Selected Topics Nucl Structure) Contrib,P21,Belyaev. 9 4Da Z Y :

208 Pb(α,α'),E=200

NUCLEAR REACTIONS

MeV; measured σ(θ).

208 Pb

deduced isoscalar GDR,high–energy octupole

resonance. DWBA. CONF Dubna(Selected Topics Nucl Struct) Proc,P68,Davis. 9 4K r Z Z :

116 , 124 Sn, 150 Nd, 208 Pb(α,α'),E=120

NUCLEAR REACTIONS

(α,α'),E=14–20 MeV; measured σ(θ).

MeV; measured GDR excitation σ(θ),γα–coin.

116,124Sn,150Nd,208Pb

150 Nd(α,α),

deduced proton,neutron density distribution

differences,deformation parameters. DWBA,deformed optical model. CONF Dubna(Selected Topics Nucl Struct) Proc,P86,Krasznahorkay. 9 4Ku Z P :

NUCLEAR REACTIONS C,Pb( 136 Xe, 136 Xe'),E=700 MeV/nucleon; Pb( 208 Pb, 208 Pb'),E=650 MeV/nucleon; measured σ vs excitation energy.

136Xe,208Pb

deduced double GDR,Γ. Other data input. CONF Dubna(Selected Topics Nucl

Struct) Proc,P39,Kulessa. 9 4ThZZ :

NUCLEAR REACTIONS

120 Sn(α,α'γ),E=160,200

MeV;

208 Pb(α,α'γ),E=160

MeV; measured σ(Eα'),αγ–coin.

120 Sn, 208 Pb

deduced GDR width vs excitation energy. CONF Dubna(Selected Topics Nucl Struct) Proc,P224,Thoennessen. 2 0 8B

i

R

9 4Ha Z T :

NUCLEAR REACTIONS

208Pb(3He,t),E=450

MeV; measured σ(Et,θ),tp–coin.

208Bi

deduced Gamow–Teller,IAR

resonances,proton escape widths. CONF Dubna(Selected Topics Nucl Struct) Proc,P19,Harakeh. 9 5Ak Z Z :

NUCLEAR REACTIONS

208Pb(3He,t),E=450

MeV; measured E(t),E(p),tp–coin.

208Bi

deduced total widths for

Gamow–Teller and spin–dipole giant resonances,total and partial proton escape widths. REPT OULNS 1994 Annual,P89,Akimune.

A = 209 209Pb

R

9 4Fo ZZ :

NUCLEAR REACTIONS

9 0 Zr, 2 0 8 Pb(α, 3 HeX),E=120

MeV; measured E( 3 He),( 3 He)n–coin,nn(θ).

9 1 Zr, 2 0 9 Pb

deduced

n–decay branching ratios for high–spin states. CONF Dubna(Selected Topics Nucl Struct) Proc,P269, Fortier.

A = 233 2 3 3Th

R

9 3Ob Z Z :

NUCLEAR REACTIONS

2 3 2 Th, 2 3 8 U(n,γ),E

not given; measured γγ(t).

2 3 3 Th, 2 3 9 U

deduced no evidence for shape

isomer. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P353,Oberstedt.

A = 239 2 3 9U

R

9 3Ob Z Z :

NUCLEAR REACTIONS

2 3 2 Th, 2 3 8 U(n,γ),E

not given; measured γγ(t).

2 3 3 Th, 2 3 9 U

deduced no evidence for shape

isomer. CONF Dubna(Nucl Struct Nucl Reactions) Proc,P353,Oberstedt.

A = 262 262104

D

9 4 L a ZX :

RADIOACTIVITY

2 6 5 , 2 6 6 106(α)

[from

2 4 8 Cm( 2 2 Ne,X)];

measured E α,T 1 / 2 .

2 6 2 104(SF);

measured T 1 / 2 . Gas–filled

recoil separator. CONF Dubna(Selected Topics Nucl Structure) Contrib,P70,Lazarev.

A = 265 265106

D

9 4 L a ZX :

RADIOACTIVITY

2 6 5 , 2 6 6 106(α)

[from

2 4 8 Cm( 2 2 Ne,X)];

measured E α,T 1 / 2 .

2 6 2 104(SF);

measured T 1 / 2 . Gas–filled

recoil separator. CONF Dubna(Selected Topics Nucl Structure) Contrib,P70,Lazarev. 9 5N o Z Z :

RADIOACTIVITY

265 106(α)

[from

232 Th( 40 Ar,3nα),E=5.2

1994 Annual,P158,Nomura.

1014

MeV/nucleon]; measured measured Eα,T 1/2 . Tof. REPT INS

SECONDARY SOURCES (Reports,Abstracts,etc. ONLY)

A = 266 266106

D

9 4 L a ZX :

RADIOACTIVITY

2 6 5 , 2 6 6 106(α)

[from

2 4 8 Cm( 2 2 Ne,X)];

measured E α,T 1 / 2 .

2 6 2 104(SF);

recoil separator. CONF Dubna(Selected Topics Nucl Structure) Contrib,P70,Lazarev.

1015

measured T 1 / 2 . Gas–filled