ar X iv : n uc l - th / 9 80 60 37 v 1 1 2 Ju n 19 98 Is SU ( 3 )

ar X iv : n uc l - th / 9 80 60 97 v 1 2 9 Ju n 19 98 3 P 2 - 3 F 2 pairing in neutron matter with modern nucleon - nucleon potentials

- th / 9 80 60 92 v 2 3 0 Ju n 19 98 Band Crossing studied by GCM with 3 D - CHFB

X iv :n uc lth /9 80 60 92 v2 3 0 Ju n 19 98 Band Crossing studied by GCM with 3D-CHFB Takatoshi Horibata, Makito Oi , Naoki Onishi c a Department of Information System Engineering, Aomori University, Aomori-city, Aomori 030-0943, Japan b Institute of Physics, College of Arts and Sciences, University of Tokyo Komaba, Meguro-ku, Tokyo 153-0041, Japan c Cyclotron Laboratory, Institute of Physical...

ar X iv : n uc l - th / 9 90 60 29 v 3 1 5 Ju l 1 99 9 1 Quark Matter ’ 99 — Theoretical Summary : What Next ?

ar X iv : n uc l - th / 9 90 60 71 v 1 2 4 Ju n 19 99 The Interference Term between the Spin and Orbital Contributions to M 1 Transitions

We study the cross-correlation between the spin and orbital parts of magnetic dipole transitions M1 in both isoscalar and isovector channels. In particular, we closely examine certain cases where ∑ B(M1) is very close to ∑ B(M1)σ + ∑ B(M1)l, implying a cancellation of the summed interference terms. We gain some insight into this problem by considering special cases approaching the SU(3) limit, ...

ar X iv : n uc l - th / 9 70 60 42 v 1 1 7 Ju n 19 97 Electromagnetic Form Factors of the Nucleon

We reanalyze the world data on the electromagnetic form factors of the nucleon. The calculations are performed in the framework of an algebraic model of the nucleon combined with vector meson dominance.