ar X iv : n uc l - th / 9 40 60 13 v 1 1 0 Ju n 19 94 Shape Coexistence Around 4416 S 28 : The Deformed N = 28 Region

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

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 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.

ar X iv : n uc l - th / 9 31 00 28 v 1 2 1 O ct 1 99 3 An antiproton - proton partial - wave analysis

ar X iv : n uc l - th / 9 70 60 46 v 1 1 8 Ju n 19 97 THEORETICAL STUDY OF THE NN → NNππ REACTION

We have developed a model for the NN → NNππ reaction and evaluated cross sections for the different charged channels. The low energy part of those channels where the pions can be in an isospin zero state is dominated by N∗ excitation, driven by an isoscalar source recently found experimentally, followed by the decay N∗ → N(ππ)T=0 S−wave. At higher energies, and in channels where the pions are n...