Delineating effects of tensor force on the density dependence of nuclear symmetry energy

被引:35
作者
Xu, Chang [1 ,2 ]
Li, Ang [2 ,3 ]
Li, Bao-An [2 ,4 ]
机构
[1] Nanjing Univ, Sch Phys, Nanjing 210008, Jiangsu, Peoples R China
[2] Texas A&M Univ, Dept Phys & Astron, Commerce, TX 75429 USA
[3] Xiamen Univ, Dept Phys & Inst Theoret Phys, Xiamen 361005, Peoples R China
[4] Xi An Jiao Tong Univ, Dept Appl Phys, Xian 710049, Peoples R China
来源
11TH INTERNATIONAL CONFERENCE ON NUCLEUS-NUCLEUS COLLISIONS (NN2012) | 2013年 / 420卷
基金
美国国家科学基金会; 中国国家自然科学基金; 美国国家航空航天局;
关键词
HEAVY-ION COLLISIONS; NEUTRON-STARS; ISOSPIN PHYSICS; MATTER; STATE; EQUATION; POTENTIALS; DYNAMICS;
D O I
10.1088/1742-6596/420/1/012090
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
In this talk, we report results of our recent studies to delineate effects of the tensor force on the density dependence of nuclear symmetry energy within phenomenological models. The tensor force active in the isosinglet neutron-proton interaction channel leads to appreciable depletion/population of nucleons below/above the Fermi surface in the single-nucleon momentum distribution in cold symmetric nuclear matter (SNM). We found that as a consequence of the high momentum tail in SNM the kinetic part of the symmetry energy E-sym(kin)(rho) is significantly below the well-known Fermi gas model prediction of approximately 12.5(rho/rho(0))(2/3). With about 15% nucleons in the high momentum tail as indicated by the recent experiments at J-Lab by the CLAS Collaboration, the E-sym(kin) (rho) is negligibly small. It even becomes negative when more nucleons are in the high momentum tail in SNM. These features have recently been confirmed by three independent studies based on the state-of-the-art microscopic nuclear many-body theories. In addition, we also estimate the second-order tensor force contribution to the potential part of the symmetry energy. Implications of these findings in extracting information about nuclear symmetry energy from nuclear reactions are discussed briefly.
引用
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页数:12
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