uc l - th / 0 30 10 72 v 1 2 3 Ja n 20 03 Mapping exchange in relativistic Hartree - Fock

ar X iv : n uc l - th / 9 40 30 03 v 1 3 M ar 1 99 4 NUCLEAR BREATHING MODE IN THE RELATIVISTIC MEAN - FIELD THEORY

The breathing-mode giant monopole resonance is studied within the framework of the rel-ativistic mean-field (RMF) theory. Using a broad range of parameter sets, a systematic analysis of constrained incompressibility and excitation energy of isoscalar monopole states in finite nuclei is performed. A comparison is made with the incompressibility derived from the semi-infinite nuclear matter and w...

X iv : n uc l - th / 9 30 30 18 v 1 2 6 M ar 1 99 3 Dirac Hartree - Fock for Finite Nuclei Employing Realistic

We discuss two different approximation schemes for the self-consistent solution of the relativistic Brueckner-Hartree-Fock equation for finite nuclei. In the first scheme, the Dirac effects are deduced from corresponding nuclear matter calculations, whereas in the second approach the local-density approximation is used to account for the effects of correlations. The results obtained by the two ...

n uc l - th / 0 40 20 75 v 1 2 3 Fe b 20 04 1 Charge - and parity - projected Hartree - Fock study with the tensor force of light nuclei

We propose a mean field framework in which the charge and the parity symmetries of a single-particle state are broken. We break these symmetries to incorporate the correlation induced by the tensor force into a nuclear mean field model. We perform the chargeand the parity projections before variation and obtain a Hartree-Fock-like equation (chargeand parity-projected Hartree-Fock equation), whi...

uc l - th / 0 30 10 54 v 1 1 6 Ja n 20 03 The ( π − , γγ ) reaction in nuclei and the σ meson in the medium

ar X iv : n uc l - th / 9 41 10 03 v 1 7 N ov 1 99 4 Closed shells at drip - line nuclei

The shell structure of magic nuclei far from stability is discussed in terms of the self-consistent spherical Hartree-Fock-Bogoliubov theory. In particular, the sensitivity of the shell-gap sizes and the two-neutron separation energies to the choice of particle-hole and particle-particle components of the effective interaction is investigated.