Effect of nuclear structure on the single particle β− transitions in deformed nuclei

1995 ◽  
Vol 45 (6) ◽  
pp. 477-489 ◽  
Author(s):  
J. Řízek ◽  
M. Ryšavý ◽  
V. Brabec
2009 ◽  
Vol 18 (04) ◽  
pp. 1099-1103 ◽  
Author(s):  
BOŻENA NERLO-POMORSKA ◽  
KRZYSZTOF POMORSKI

Evaluation of shell effects in nuclei plays an important role in studying the nuclear structure. In the Strutinsky method the smooth energy of the nucleus is obtained by a folding procedure of the single-particle (s.p.) energy density in the s.p. energy space e. An alternative way of energy smoothing is obtained by folding the s.p. energy sum in the particle-number space [Formula: see text]. For non degenerated s.p. spectra both types of folding yield smooth energies which are close to each other. In the case of strongly degenerated spectra which appear at sphericity or in regions of shape isomers, the smooth energy obtained by the [Formula: see text]-folding is a couple of MeV larger than the traditional average Strutinsky energy. It is shown that this smooth energy difference can serve as a simple tool to search for magic or quasi-magic structures in the s.p. spectra, e.g. to find shape isomers in the multidimensional deformation space.


2018 ◽  
Vol 178 ◽  
pp. 02009
Author(s):  
Ani Aprahamian ◽  
Shelly R. Lesher

Low-lying oscillations of the intrinsic deformed shape of a nucleus remain an open challenge in nuclear structure. The question or challenge revolves around the viability of single or multiple quanta of vibrational excitations superimposed on the equilibrium, deformed shape of a nucleus. The K=2 or “γ” vibrations are fairly widespread and nominally conform to expectations whereas the existence of the K=0 or “β” vibrational excitation is yet to be distinguished from other possible origins including the coexistence of other potential minima.


1993 ◽  
Vol 551 (1) ◽  
pp. 93-108 ◽  
Author(s):  
A.A. Raduta ◽  
D.S. Delion ◽  
N. Lo Iudice

1976 ◽  
Vol 35 (1) ◽  
pp. 115-124 ◽  
Author(s):  
P. Christillin ◽  
M. Rosa-Clot

The field theory of elementary particles has so far failed to predict the detailed form of the interaction between neutrons and protons (nucleons), but the nucleon-nucleon scattering experiments are now sufficiently complete that for most purposes the interaction may be taken as known. At the same time a wealth of data concerning energy levels, transition probabilities and so on is available for literally hundreds of nuclei. Such measurements reveal that nuclei have an extremely rich structure, with both single-particle and collective properties, illustrating almost every feature of a many-body system. It is the purpose of this talk to review the extent to which we are able to understand these properties on the basis of the known two-body interaction. It will be shown how some features may be understood quite readily while others still pose fascinating problems.


1989 ◽  
Vol 196 (1) ◽  
pp. 89-134 ◽  
Author(s):  
Johann Bartel ◽  
Mikkel B Johnson ◽  
M.K Singham

1968 ◽  
Vol 121 (1) ◽  
pp. 153-160 ◽  
Author(s):  
V. Feifrlík ◽  
J. Řízek

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