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Neutron-proton effective mass splitting in neutron-rich matter

Sibo Wang1, Hui Tong2, Qiang Zhao3, Chencan Wang4, Peter Ring5, and Jie Meng6,7,*

  • 1Department of Physics, Chongqing University, Chongqing 401331, China
  • 2Helmholtz-Institut für Strahlen- und Kernphysik and Bethe Center for Theoretical Physics, Universität Bonn, D-53115 Bonn, Germany
  • 3Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Korea
  • 4School of Physics and Astronomy, Sun Yat-Sen University, Zhuhai 519082, China
  • 5Department of Physik, Technische Universität München, D-85747 Garching, Germany
  • 6State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China
  • 7Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, Japan

  • *mengj@pku.edu.cn

Phys. Rev. C 108, L031303 – Published 18 September, 2023

DOI: https://doi.org/10.1103/PhysRevC.108.L031303

Abstract

Nucleon effective masses in neutron-rich matter are studied with the relativistic Brueckner-Hartree-Fock (RBHF) theory in the full Dirac space. The neutron and proton effective masses for symmetric nuclear matter are 0.80 times rest mass, which agrees well with the empirical values. In neutron-rich matter, the effective mass of the neutron is found to be larger than that of the proton, and the neutron-proton effective mass splittings at the empirical saturation density are predicted as 0.187α with α being the isospin asymmetry parameter. The result is compared to other ab initio calculations and is consistent with the constraints from the nuclear reaction and structure measurements, such as the nucleon-nucleus scattering, the giant resonances of Pb208, and the Hugenholtz–Van Hove theorem with systematics of nuclear symmetry energy and its slope. The predictions of the neutron-proton effective mass splitting from the RBHF theory in the full Dirac space might be helpful to constrain the isovector parameters in phenomenological density functionals.

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