Chiral Sigma Model with Pion Mean Field in Finite Nuclei

Details Chiral Sigma Model with Pion Mean Field in Finite Nuclei Chiral Sigma Model with Pion Mean Field in Finite Nuclei

2003-12-13

arxiv.org/abs/nucl-th/0312042v1

Prog.Theor.Phys. 111 (2004) 75-92

Physics

Nuclear Physics

Nuclear Theory

19 pages, 9 figures. Prog. Theor. Phys. to be published

Scientific paper

10.1143/PTP.111.75

The properties of infinite matter and finite nuclei are studied by using the chiral sigma model in the framework of the relativistic mean field theory. We reconstruct an extended chiral sigma model in which the omega meson mass is generated dynamically by the sigma condensation in the vacuum in the same way as the nucleon mass. All the parameters of chiral sigma model are essentially fixed from the hadron properties in the free space. In nuclear matter, the saturation property comes out right, but the incompressibility is too large and the scalar and vector potentials are about a half of the phenomenological ones, respectively. This fact is reflected to the properties of finite nuclei. We calculate N = Z even-even mass nuclei between N = 16 and N = 34. The extended chiral sigma model without the pion mean field leads to the result that the magic number appears at N = 18 instead of N = 20 and the magic number does not appear at N = 28 due to the above mentioned nuclear matter properties. The latter problem, however, could be removed by the introduction of the finite pion mean field with the appearance of the magic number at N = 28. We find that the energy differences between the spin-orbit partners are reproduced by the finite pion mean field which is completely a different mechanism from the standard spin-orbit interaction.

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