We explore the mechanism of the isospin splitting of neutron and proton effective masses in neutronrich nuclear matter within the framework of the Brueckner-Hartree-Fock (BHF) approach. First we find that the neutron-...We explore the mechanism of the isospin splitting of neutron and proton effective masses in neutronrich nuclear matter within the framework of the Brueckner-Hartree-Fock (BHF) approach. First we find that the neutron-proton effective mass splitting in neutron-rich matter is dominated by the nonlocality of the microscopic s. p. potentials in spatial space,i. e.,by the isospin splitting of the k-mass shown in Fig.展开更多
We extend the Brueckner-Hartree-Fock (BHF) approach by including the rearrangement contribution of a microscopic three-body force in calculating the single particle properties of nuclear matter. In the BHF approach, t...We extend the Brueckner-Hartree-Fock (BHF) approach by including the rearrangement contribution of a microscopic three-body force in calculating the single particle properties of nuclear matter. In the BHF approach, the TBF contribution is included by reducing the TBF to an equivalent effective two-body force V3eff. This effective force V3eff is density dependent. Due to the density dependence of the effective force V3eff, inclusion of the TBF in the BHF calculation may introduce an extra contribution UTBF to the single nu-展开更多
We investigate the isospin splitting of neutron and proton effective masses in neutron-rich nuclear matter by using Brueckner-Hartree-Fock (BHF) approach and the extended BHF (EBHF) approach including the ground state...We investigate the isospin splitting of neutron and proton effective masses in neutron-rich nuclear matter by using Brueckner-Hartree-Fock (BHF) approach and the extended BHF (EBHF) approach including the ground state correlation contributions. The realistic nucleon-nucleon interaction adopted in our calculation is the Argonne V18 two-body force supplemented with a microscopic three-body force constructed from the meson-exchange current approach. The result is reported in Fig. 1 where the neutron and proton effective masses are plotted as functions of isospin asymmetry parameterβ. It is shown that in both cases by adopting the BHF and EBHF approaches, the predicted neutron effective mass is greater展开更多
The effect of a microscopic nuclear three-body force (TBF) on the critical baryon density ρc for kaon condensation in chemical equilibrium neutron star matter has been investigated in the framework of the Brueckner-H...The effect of a microscopic nuclear three-body force (TBF) on the critical baryon density ρc for kaon condensation in chemical equilibrium neutron star matter has been investigated in the framework of the Brueckner-Hartree-Fock approach. The calculated values of the critical density are given in Tab.1 for both cases with and without including the TBF contribution and for three different choices of the proton strangeness content (i.e.,展开更多
The critical properties of the liquid-gas phase transition of hot nuclear matter have been investigated within the finite temperature Brueckner-Hartree-Fook (FTBHF) approach extended by introducing a microscopic three...The critical properties of the liquid-gas phase transition of hot nuclear matter have been investigated within the finite temperature Brueckner-Hartree-Fook (FTBHF) approach extended by introducing a microscopic three-body force (TBF). In Fig.1 is plotted the calculated equation of state (EOS) of symmetric nuclear matter, where the solid and dashed isothermal curves of pressure (corresponding to T = 0,8,10,12,14,16 MeV from the展开更多
In the framework of the isospin dependent Brueckner-Hartree-Fock approach, the density and momentum dependence of symmetry potential has been investigated by adopting the Argonne V18(AV18) two-body nucleon-nucleon int...In the framework of the isospin dependent Brueckner-Hartree-Fock approach, the density and momentum dependence of symmetry potential has been investigated by adopting the Argonne V18(AV18) two-body nucleon-nucleon interaction plus a microscopic three-body force (TBF). The symmetry potential is defined as,展开更多
Medium polarization eflects are studied for 1S0 pairing in nuclear matter within BHF approach. The screening potential is calculated in the RPA limit, suitably renormalized to cure the low density mechanical instabili...Medium polarization eflects are studied for 1S0 pairing in nuclear matter within BHF approach. The screening potential is calculated in the RPA limit, suitably renormalized to cure the low density mechanical instability of nuclear matter. The self-energy corrections are consistently included resulting in a strong depletion of the Fermi surface. The self-energy effects always lead to a quenching of the gap, whereas it is almost completely compensated by the anti-screening effect in nuclear matter.展开更多
文摘We explore the mechanism of the isospin splitting of neutron and proton effective masses in neutronrich nuclear matter within the framework of the Brueckner-Hartree-Fock (BHF) approach. First we find that the neutron-proton effective mass splitting in neutron-rich matter is dominated by the nonlocality of the microscopic s. p. potentials in spatial space,i. e.,by the isospin splitting of the k-mass shown in Fig.
文摘We extend the Brueckner-Hartree-Fock (BHF) approach by including the rearrangement contribution of a microscopic three-body force in calculating the single particle properties of nuclear matter. In the BHF approach, the TBF contribution is included by reducing the TBF to an equivalent effective two-body force V3eff. This effective force V3eff is density dependent. Due to the density dependence of the effective force V3eff, inclusion of the TBF in the BHF calculation may introduce an extra contribution UTBF to the single nu-
文摘We investigate the isospin splitting of neutron and proton effective masses in neutron-rich nuclear matter by using Brueckner-Hartree-Fock (BHF) approach and the extended BHF (EBHF) approach including the ground state correlation contributions. The realistic nucleon-nucleon interaction adopted in our calculation is the Argonne V18 two-body force supplemented with a microscopic three-body force constructed from the meson-exchange current approach. The result is reported in Fig. 1 where the neutron and proton effective masses are plotted as functions of isospin asymmetry parameterβ. It is shown that in both cases by adopting the BHF and EBHF approaches, the predicted neutron effective mass is greater
文摘The effect of a microscopic nuclear three-body force (TBF) on the critical baryon density ρc for kaon condensation in chemical equilibrium neutron star matter has been investigated in the framework of the Brueckner-Hartree-Fock approach. The calculated values of the critical density are given in Tab.1 for both cases with and without including the TBF contribution and for three different choices of the proton strangeness content (i.e.,
文摘The critical properties of the liquid-gas phase transition of hot nuclear matter have been investigated within the finite temperature Brueckner-Hartree-Fook (FTBHF) approach extended by introducing a microscopic three-body force (TBF). In Fig.1 is plotted the calculated equation of state (EOS) of symmetric nuclear matter, where the solid and dashed isothermal curves of pressure (corresponding to T = 0,8,10,12,14,16 MeV from the
文摘In the framework of the isospin dependent Brueckner-Hartree-Fock approach, the density and momentum dependence of symmetry potential has been investigated by adopting the Argonne V18(AV18) two-body nucleon-nucleon interaction plus a microscopic three-body force (TBF). The symmetry potential is defined as,
基金Supported by NSFC (10875150)the grant appointed to European Community Project Asia-Europe Link in Nuclear Physics and Astrophysics, CN/ASIA-LINK/008(94791)
文摘Medium polarization eflects are studied for 1S0 pairing in nuclear matter within BHF approach. The screening potential is calculated in the RPA limit, suitably renormalized to cure the low density mechanical instability of nuclear matter. The self-energy corrections are consistently included resulting in a strong depletion of the Fermi surface. The self-energy effects always lead to a quenching of the gap, whereas it is almost completely compensated by the anti-screening effect in nuclear matter.
基金National Natural Science Foundation of China(11175219,10875151,10740420550)Knowledge Innovation Project of Chinese Academy of Sciences(KJCX3-SYW-N2)+2 种基金Chinese Academy of Sciences Visiting Professorship for Senior International Scientists(2009J2-26)CAS/SAFEA International Partnership Program for Creative Research Teams(CXTD-J2005-1)Major State Basic Research Development of China(2007CB15004)~~