ar X iv : n uc l - th / 0 40 40 46 v 1 1 6 A pr 2 00 4 Analytical relationship for the cranking inertia

- th / 0 40 40 46 v 2 1 8 A pr 2 00 4 Analytical relationship for the cranking inertia

The wave function of a spheroidal harmonic oscillator without spin-orbit interaction is expressed in terms of associated Laguerre and Hermite polynomials. The pairing gap and Fermi energy are found by solving the BCS system of two equations. Analytical relationships for the matrix elements of inertia are obtained function of the main quantum numbers and potential derivative. They may be used to...

ar X iv : n uc l - th / 0 30 40 52 v 1 1 6 A pr 2 00 3

ar X iv : n uc l - th / 0 50 40 62 v 1 2 1 A pr 2 00 5 1 Structure of 8 B and astrophysical S 17 factor

ar X iv : n uc l - th / 0 40 40 77 v 1 2 7 A pr 2 00 4 Skyrme - HFB deformed nuclear mass table

The Skyrme-Hartree-Fock-Bogoliubov code HFBTHO using the axial (2D) Transformed Harmonic Oscillator basis is tested against the HFODD (3D Cartesian HO basis) and HFBRAD (radial coordinate) codes. Results of large-scale ground-state calculations are presented for the SLy4 and SkP interactions.

ar X iv : n uc l - th / 0 40 40 04 v 1 2 A pr 2 00 4 N - N Interactions in the Extended Chiral SU ( 3 ) Quark Model

The chiral SU(3) quark model is extended to include coupling between vector chiral field and quarks. By using this model, the phase shifts of NN scattering for different partial waves are studied. The results are very similar to those of the chiral SU(3) quark model calculation, in which one gluon exchange (OGE) plays dominate role in the short range part of the quark-quark interactions. Only i...