2002
DOI: 10.1088/0253-6102/37/4/457
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Nuclear Level Density and Thermodynamic Functions for Nuclei with Static Deformation

Abstract: The level densities of even-odd and even-even isotopes , and were calculated using microscopic theory of interacting fermions and compared with experiments. It is found that the data can be well reproduced with level density formalism for nuclei with static deformation. The nuclear temperature as well as the entropy of nuclear system as a function of excitation energy has been extracted from the BCS theory. It is shown that the entropy exhibits an -formed shape as a function of excitation energy. This is int… Show more

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Cited by 9 publications
(15 citation statements)
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“…[6,7], briefly described in Appendix B, is valid only in the last case and, in fact, it has already been applied to heavier deformed lanthanides measured by the Oslo group, such as 161,162 Dy, 166 Er, and 171,172 Yb [35,36].…”
Section: Numerical Resultsmentioning
confidence: 99%
“…[6,7], briefly described in Appendix B, is valid only in the last case and, in fact, it has already been applied to heavier deformed lanthanides measured by the Oslo group, such as 161,162 Dy, 166 Er, and 171,172 Yb [35,36].…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Therefore, the problem is reduced to the BCS quasi-particle as non-interacting fermions. For this, the second quantization formalism is applied [7][8][9][10]. There are many parameters in the Hamiltonian that describe a system of interacting fermions [11].…”
Section: Microscopic Theory Of Interacting Fermionsmentioning
confidence: 99%
“…N is the entropy of the system and det D is a 3 × 3 determinant of second order partial differentials of partition function ln Z(β 0 , α 0 ) versus β and α i in the saddle point. In microscopic formalism, grand partition function is determined by realistic single particle levels [7][8][9][10]12] ln…”
Section: Microscopic Theory Of Interacting Fermionsmentioning
confidence: 99%
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