THE SELF-CONSISTENT FIELD EQUATIONS AT FINITE NUCLEAR TEMPERATURE——THE GENERALIZED HFB EQUATIONS

  • In order to study the variation of shell effects as well as pairing effects with nuclear temperature, we have extended the work of Sano and Yamasaki to generalize the HFB equations to finite nuclear temperature with the help of variational principle. When nullear temperature θ→0, sulh generalized HFB equations reduce to the conventional HFB equations. While the fermi gas model results can be obtained in the high temperature limit.
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  • [1] 金炳年、陆中道、陈星集、王顺金,高能物理与核物理,4(1980) 236.[2] M. Sano and S. Yamasaki, Proyr. Theor. Phys., 29 (1963), 397[3] Y. S. Ramamurthy, S. S. gapoor and S. S. gataria, Phys. Rev. Lett., 25 (1970), 386.
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WANG SHUN-JIN. THE SELF-CONSISTENT FIELD EQUATIONS AT FINITE NUCLEAR TEMPERATURE——THE GENERALIZED HFB EQUATIONS[J]. Chinese Physics C, 1981, 5(1): 92-99.
WANG SHUN-JIN. THE SELF-CONSISTENT FIELD EQUATIONS AT FINITE NUCLEAR TEMPERATURE——THE GENERALIZED HFB EQUATIONS[J]. Chinese Physics C, 1981, 5(1): 92-99. shu
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Received: 1979-10-15
Revised: 1900-01-01
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THE SELF-CONSISTENT FIELD EQUATIONS AT FINITE NUCLEAR TEMPERATURE——THE GENERALIZED HFB EQUATIONS

  • Lanzhou University

Abstract: In order to study the variation of shell effects as well as pairing effects with nuclear temperature, we have extended the work of Sano and Yamasaki to generalize the HFB equations to finite nuclear temperature with the help of variational principle. When nullear temperature θ→0, sulh generalized HFB equations reduce to the conventional HFB equations. While the fermi gas model results can be obtained in the high temperature limit.

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