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

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 30 40 52 v 1 1 6 A pr 2 00 3

ar X iv : n uc l - th / 0 41 10 62 v 1 1 6 N ov 2 00 4 Nuclear vorticity and the low - energy nuclear response - Towards the neutron drip line

The transition density and current provide valuable insight into the nature of nuclear vibrations. Nuclear vorticity is a quantity related to the transverse transition current. In this work, we study the evolution of the strength distribution, related to density fluctuations, and the vorticity strength distribution, as the neutron drip line is approached. Our results on the isoscalar, natural-p...

ar X iv : n uc l - th / 0 41 10 83 v 1 1 9 N ov 2 00 4 Electromagnetic transitions for A = 3 nuclear systems

Recent advances in the study of pd radiative capture in a wide range of center-of-mass energy below and above deuteron breakup threshold are presented and discussed.

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...