Tensor-force effects on shell-structure evolution in N=82 isotones and Z=50 isotopes in the relativistic Hartree-Fock theory

被引:4
作者
Wang, Zhiheng [1 ,2 ,3 ]
Naito, Tomoya [4 ,5 ]
Liang, Haozhao [4 ,5 ]
机构
[1] Lanzhou Univ, Sch Nucl Sci & Technol, Lanzhou 730000, Peoples R China
[2] Lanzhou Univ, Joint Dept Nucl Phys, Lanzhou 730000, Peoples R China
[3] Chinese Acad Sci, Inst Modern Phys, Lanzhou 730000, Peoples R China
[4] Univ Tokyo, Grad Sch Sci, Dept Phys, Tokyo 1130033, Japan
[5] RIKEN, Nishina Ctr, Wako, Saitama 3510198, Japan
关键词
INTERACTION CROSS-SECTIONS; GROUND-STATE PROPERTIES; MEAN-FIELD; BOGOLIUBOV THEORY; RADII; SPECTROSCOPY; NUCLEI;
D O I
10.1103/PhysRevC.103.064326
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The evolutions of the energy difference between the neutron states 1i(13/2) and 1h(9/2) in the N = 82 isotones and that between the proton states 1h(11/2) and 1g(7/2) in the Z = 50 isotopes are investigated within the framework of the relativistic Hartree-Fock theory, using the density-dependent effective (interactions )PKA1, PKOi (i = 1, 2, 3), and a new interaction developed in this study. By identifying the contributions of the tensor force, which is naturally induced via the Fock terms, we find that the tensor force plays crucial roles in the evolution of the shell structure. The strength of the tensor force is also explored. It is found that moderately increasing the coupling strength of pion-nucleon coupling, i.e., f(pi), will significantly improve the description of the shell-structure evolution. In particular, reducing the density dependence of f(pi) is shown to be preferable, in comparison to enlarging f(pi) with a factor. This is consistent with the idea of "tensor renormalization persistency" and provides valuable guidance for the development of the nuclear energy density functional in the relativistic framework.
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页数:14
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