Explanation of the keywords

Explanation of the keywords

NUCLEAR Explanation SHEETS DATA o f the K E Y W O R D S The XEYWORDS are designed to tell a reader what experimental results are reported in an ar...

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NUCLEAR Explanation

SHEETS

DATA

o f the K E Y W O R D S

The XEYWORDS 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 ( f o r MOMENTS, R A D I O A C T I V I T Y ) , o r r e a c t i o n (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 b y t h e ASTM 'CODEN' a b b r e v i a t i o n s . The abbreviations can be identified by referring to the table oh the next page or by occasional checking of the reference list, where all references are giwm in detail.

EXAMPLES Several

keyword

strings

are

printed

below

along

with

translations

into

'plain

English.'

75Di09 ,RADIOACTIVITY t0ZAg(EC),(fl+);m e a s u r e d E T , l % 7 - ] - c o i n , T i / z ; d e d u c e d log f t . 1°3Pd d e d u c e d l e v e l s , J , I r . PHSTB 12 80. Through

the electron

capture,

fl+-decay

o f t°aAg, p r o p e r t i e s

of i°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 R E A C T I O N S t°3Rh(p,nT),E=6.3-12 MeV; m e a s u r e d a(E,ET,8), I(ce),TT-coin,7(t). t°SPd deduced levels,J,Tr,Tl/z,ICC,k.P H S T B 12 80. Through observation over the incident

of the angular parLicle 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 ET, Ea, Ep', Et, E(aHe} EC ENDOR EPR, ESR EWSR fragment gK, gR HFB

distribution of v - r a y s f r o m r a n g e 6 . 3 - 1 2 MeV, p r o p e r t i e s

Izl,t32,13eCs;m e a s u r e d N U P A B A 2 4 8 157.

o f 131,i3z,t36cs w e r e d e d u c e d

Explanation

from

t h e (p,n~') 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 .

hfs,a,b; deduced ~,

measurements

of h y p e r f i n e

structure

Symbol

dipole, q u a d ~ u p o l e , octupole h y p ' e r f i n e interaction constants atomic-beam magnetic resonance B ( E L ) . o r B(ML) d e l a y e d coincidence, s o m e t i m e s W r i t t e n as TT(t), a m ( t ) direet-semidirect model ( w i t h o u t s u b s c r i p t ) e n e r g y of i n c o m i n g 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) E~, Ea, Ep,, E t , E(3He) electron capture electron-nucleus double-resonance electron paramagnetic, spin resonance energy-weighted sum rule f i s s i o n or h e a v y i o n r e a c t i o n f r a g m e n t gK, gR Har t r e e - F o c k - B o g o l i u b o v

l(Auger) IT, Ifl IB ICO P(n), P ( a )

p(p+) Q, QP RPA S (y TDA TDHF width X T-branching

483

Iea I~, 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 -: Pp, n - w i d t h =- Fn, v - w i d t h ~ F~ X - r a y in 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 i n (a,X), (taC,X) relative T-ray branching from a level