Lorentz-Lorenz Quenching for the Gamow-Teller Sum Rules

1984 ◽  
pp. 201-204
Author(s):  
J. Delorme ◽  
M. Ericson ◽  
A. Figureau ◽  
N. Giraud
Keyword(s):  
2019 ◽  
Vol 223 ◽  
pp. 01053
Author(s):  
Hiroyuki Sagawa

We study the sum rules of double Gamow-Teller (DGT) excitations through double spin-isospin operator (σt­)2 In general, 2+states in the granddaughter nuclei have dominant transition strength in DGT excitations and 0+states are weak, except in T = 1 mother nuclei in which 0+strength is competitive with 2+strength. A possibility to extract the unit cross section for the DGT transition strength is pointed out in the (#x03C3;t­)2 excitation of double isobaric analog state (DIAS) in T = 1 nuclei.


1995 ◽  
Vol 587 (2) ◽  
pp. 301-317 ◽  
Author(s):  
M.K. Cheoun ◽  
Amand Faessler ◽  
F. Šimkovic ◽  
G. Teneva ◽  
A. Bobyk

2006 ◽  
Vol 15 (08) ◽  
pp. 1925-1931
Author(s):  
HARUKI KURASAWA ◽  
TOSHIO SUZUKI

The roles of anti-nucleon degrees of freedom in nuclear relativistic models are discussed. They are necessary for sum rules. It is also pointed out that the no-sea approximation, where the divergent terms due to the anti-nucleon degrees of freedom are neglected, has no physical justification and is a serious problem. These facts are shown in an analytic way by using the sum rule and RPA response function for the giant Gamow-Teller states.


1986 ◽  
Vol 182 (3-4) ◽  
pp. 265-268 ◽  
Author(s):  
M.H. Macfarlane
Keyword(s):  

1992 ◽  
Vol 277 (1-2) ◽  
pp. 13-17 ◽  
Author(s):  
Kazuo Muto
Keyword(s):  

1987 ◽  
Vol 65 (6) ◽  
pp. 626-632 ◽  
Author(s):  
M. H. Macfarlane

This paper deals with the sum rules obtained from the energy moments of multipole-excitation strength functions. An explicit expression in terms of ground-state orbit-occupation probabilities is given for the total, non-energy-weighted strength of isovector excitations. For the Gamow–Teller (GT) excitation, separate sum rules are obtained for the total (p, n) and (n, p) strengths; these sum rules satisfy the Ikeda relation (S(p, n)–S(n, p) = 3(N – Z)) exactly. The GT sum rules are then used to estimate the influence of ground-state correlations on total (p, n) and (n, p) strengths in 208Pb. Sizeable strength enhancements are obtained, ranging from around 15% (in units of 3(N – Z) for longer range random-phase approximation correlations to 50% or more if short-range nuclear-matter correlations are included. An assessment is then given of the current status of the problem of missing Gamow–Teller strength in heavy nuclei. Brief concluding sections deal with the isospin splitting of isovector excitations and further development of the energy–moment sum rules.


1980 ◽  
Vol 22 (3) ◽  
pp. 1138-1144 ◽  
Author(s):  
W. R. Wharton ◽  
C. D. Goodman ◽  
D. C. Hensley
Keyword(s):  

1988 ◽  
Vol 102 ◽  
pp. 343-347
Author(s):  
M. Klapisch

AbstractA formal expansion of the CRM in powers of a small parameter is presented. The terms of the expansion are products of matrices. Inverses are interpreted as effects of cascades.It will be shown that this allows for the separation of the different contributions to the populations, thus providing a natural classification scheme for processes involving atoms in plasmas. Sum rules can be formulated, allowing the population of the levels, in some simple cases, to be related in a transparent way to the quantum numbers.


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