ar X iv : n uc l - th / 9 60 90 03 v 1 3 0 A ug 1 99 6 Nearthreshold Large Q 2 Electroproduction off Polarized Deuteron

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 60 80 57 v 2 1 8 N ov 1 99 6 Strong decays of nonstrange q 3 baryons

ar X iv : n uc l - th / 9 90 50 50 v 1 2 1 M ay 1 99 9 GAMMA - DEUTERON SCATTERING

We discuss a recent computation of Compton scattering on the deuteron at photon energies of order the pion mass. An interaction kernel is computed in baryon chiral perturbation theory and sewn to phenomenological deuteron wave functions. As an appetizer, we consider a computation of the pion-deuteron scattering length using this method.

ar X iv : n uc l - th / 0 30 70 01 v 1 3 0 Ju n 20 03 - 1 - CORRELATION BETWEEN THE DEUTERON CHARACTERISTICS AND THE LOW - ENERGY TRIPLET np SCATTERING PARAMETERS

ar X iv : n uc l - th / 9 90 71 09 v 1 2 8 Ju l 1 99 9 1 Charged current weak production of the ∆ resonance

The reactions e − p → ∆ 0 ν e and e + p → ∆ ++ ¯ ν e are considered as a possible source of information about the weak N∆ transition form factors. The low q 2 BNL data on ν µ production of ∆ are used to extract the axial vector N∆ coupling, taking into account the deuteron structure and the ∆ width. Finally, pion production induced by neutrinos in 16 O in the ∆ region, relevant to atmospheric ν...