Based on the finite temperature Brueckner-Hartrec-Fock approach including a microscopic three-body force, the rearrangement correction V2(k) to the single nucleon potential in hot nuclear matter, and its density and t...Based on the finite temperature Brueckner-Hartrec-Fock approach including a microscopic three-body force, the rearrangement correction V2(k) to the single nucleon potential in hot nuclear matter, and its density and temperature dependence have been investigated by using the hole-line expansion for the mass operator.展开更多
The finite temperature Brueckner-Hartree-Fock approach (FTBHF) has been extended by introducing a microscopic three-body force. The three-body force is constructed from the meson-exchange current method[1]. Within the...The finite temperature Brueckner-Hartree-Fock approach (FTBHF) has been extended by introducing a microscopic three-body force. The three-body force is constructed from the meson-exchange current method[1]. Within the extended FTBHF framework, the equation of state (EOS) of hot symmetric nuclear matter has been investigated and the critical temperature of the liquid-gas transition has been calculated. The obtained展开更多
文摘Based on the finite temperature Brueckner-Hartrec-Fock approach including a microscopic three-body force, the rearrangement correction V2(k) to the single nucleon potential in hot nuclear matter, and its density and temperature dependence have been investigated by using the hole-line expansion for the mass operator.
文摘The finite temperature Brueckner-Hartree-Fock approach (FTBHF) has been extended by introducing a microscopic three-body force. The three-body force is constructed from the meson-exchange current method[1]. Within the extended FTBHF framework, the equation of state (EOS) of hot symmetric nuclear matter has been investigated and the critical temperature of the liquid-gas transition has been calculated. The obtained
