2005/06/01 by W. Zuo, Liyun Cao, L. G. Cao +4 · 123 citations
Earth and Planetary Sciences · Physics and Astronomy · #Ansatz #High-pressure geophysics and materials #Isospin #Mean field theory #Neutron #Nuclear matter #Nuclear physics #Nuclear physics research studies #Nucleon #Physics #Quantum Chromodynamics and Particle Interactions #Quantum electrodynamics #Quantum mechanics #Scattering #Symmetry (geometry) #nucl-th
paper · pdf · doi:10.1103/physrevc.72.014005
published in Physical Review C 72(1) (American Institute of Physics) · 8 pages, 10 figures
arxiv created 2005/06/01 · openalex publication_date 2005/07/14 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The isospin splitting of the nucleon mean field is derived from the Brueckner theory extended to asymmetric nuclear matter. The Argonne V18 has been adopted as bare interaction in combination with a microscopic three-body force. The isospin splitting of the effective mass is determined from the Brueckner-Hartree-Fock self-energy: It is linear according to the Lane ansatz, such that mn*>mp* for neutron-rich matter. The symmetry potential is also determined, and a comparison is made with the predictions of the Dirac-Brueckner approach and the phenomenological interactions. The theoretical predictions are also compared with the empirical parametrizations of neutron and proton optical model potentials based on the experimental nucleon-nucleus scattering and the phenomenological ones adopted in transport model simulations of heavy-ion collisions. The direct contribution of the rearrangement term due to three-body forces to the single-particle potential and symmetry potential is discussed.