Toward a New Theory of Spherical Nuclei. I

1967 ◽  
Vol 156 (4) ◽  
pp. 1159-1166 ◽  
Author(s):  
G. Do Dang ◽  
A. Klein
Keyword(s):  
1980 ◽  
Vol 41 (C1) ◽  
pp. C1-141-C1-142
Author(s):  
L. M. Dautov ◽  
R. N. Kasymbalinov ◽  
D. K. Kaipov ◽  
M. M. Kadykenov

1967 ◽  
Vol 45 (10) ◽  
pp. 3241-3245 ◽  
Author(s):  
P. A. Simard

A method is presented in the scheme of the boson approximation such that the antisymmetry between the quasi-particles is introduced naturally. Based on the transcription of the quasi-particle into the ideal space, the method enables one to give a unified description of the anharmonic corrections in the even–even and odd spherical nuclei.


2005 ◽  
Vol 26 (1) ◽  
pp. 25-32 ◽  
Author(s):  
S. Péru ◽  
J. F. Berger ◽  
P. F. Bortignon

1983 ◽  
Vol 130 (3-4) ◽  
pp. 134-138 ◽  
Author(s):  
Ch. Stoyanov ◽  
A.I. Vdovin

1962 ◽  
Vol 35 ◽  
pp. 219-231 ◽  
Author(s):  
M.G. Urin ◽  
D.F. Zaretsky

Pramana ◽  
2010 ◽  
Vol 74 (4) ◽  
pp. 541-553 ◽  
Author(s):  
Necla Cakmak ◽  
Kaan Manisa ◽  
Serdar Unlu ◽  
Cevad Selam
Keyword(s):  
Β Decay ◽  

1993 ◽  
Vol 02 (supp01) ◽  
pp. 71-79 ◽  
Author(s):  
KRISHNA KUMAR

Energy minimization is not sufficient to determine whether a nucleus is spherical or deformed. The quantal zero-point motion can make a nucleus spherical even if the potential energy has a deformed minimum. However, some general conditions give deformed shape as the natural state of atomic nuclei. They are spherical only under some special conditions. Some general criteria for distinguishing spherical nuclei from deformed, as well as some advantages of using a deformed-shell model rather than a spherical-shell model, are presented.


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