X iv : n uc l - th / 9 90 30 22 v 1 9 M ar 1 99 9 Weak reactions on 12 C within the Continuum Random Phase Approximation with partial occupancies

X iv : n uc l - th / 9 90 30 24 v 1 9 M ar 1 99 9 Method of integral transforms for few – body reactions

The method of integral transforms is reviewed. In the framework of this method reaction observables are obtained with the bound–state calculation techniques. New developments are reported.

ar X iv : n uc l - th / 9 70 50 03 v 1 1 M ay 1 99 7 Neutrino - nucleus reactions on 12 C and 16

Exclusive and inclusive (ν µ , µ −), (ν e , e −) cross-sections and µ −-capture rates are calculated for 12 C and 16 O using the consistent random phase approximation (RPA) and pairing model. After a pairing correction is introduced to the RPA results the flux-averaged theoretical (ν µ , µ −), (ν e , e −) cross-sections and µ −-capture rates in 12 C are in good agreement with experiment. In par...

ar X iv : n uc l - th / 9 90 50 49 v 1 2 1 M ay 1 99 9 η - and η ′ - meson production in the reaction pn → dM near threshold

ar X iv : n uc l - th / 9 90 10 54 v 1 1 9 Ja n 19 99 KVI

The chiral two-pion exchange component of the long-range pp interaction is studied in an energy-dependent partial-wave analysis. We demonstrate its presence and importance, and determine the chiral parameters c i (i = 1, 3, 4). The values agree well with those obtained from pion-nucleon amplitudes.

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 ?