ar X iv : n uc l - th / 9 80 20 08 v 1 3 F eb 1 99 8 Nuclear breakup of 8 B in a direct fragmentation model ∗

ar X iv : n uc l - th / 9 80 20 12 v 1 3 F eb 1 99 8 COMPUTATION OF TWO - BODY MATRIX ELEMENTS FROM THE ARGONNE v 18 POTENTIAL

We discuss the computation of two-body matrix elements from the Argonne v 18 interaction. The matrix elements calculation is presented both in particle-particle and in particle-hole angular momentum coupling. The procedures developed here can be applied to the case of other NN potentials, provided that they have a similar operator format.

ar X iv : n uc l - th / 9 31 20 21 v 1 2 8 D ec 1 99 3 Meson phase space density from interferometry

X iv :n uc lth /9 31 20 21 v1 2 8 D ec 1 99 3 Meson phase space density from interferometry George F. Bertsch Dept. of Physics and Institute for Nuclear Theory, FM-15 University of Washington Seattle, WA 98195 Abstract The interferometric analysis of meson correlations provides a measure of the average phase space density of the mesons in the final state. This quantity is a useful indicator of ...

ar X iv : n uc l - th / 9 80 80 69 v 1 2 7 A ug 1 99 8 Coulomb and nuclear breakup of 8 B

The cross sections for the (8 B, 7 Be-p) breakup reaction on 58 Ni and 208 Pb targets at the beam energies of 25.8 MeV and 415 MeV have been calculated within a one-step prior-form distorted-wave Born approximation. The relative contributions of Coulomb and nuclear breakup of E1 and E2 multipolarities as well as their interference have been determined. The nuclear breakup contributions are foun...

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 10 16 v 1 8 J an 1 99 9 Experimental and Theoretical Search for a Phase Transition in Nuclear Fragmentation

Phase transitions of small isolated systems are signaled by the shape of the caloric equation of state e∗(T ), the relationship between the excitation energy per nucleon e∗ and temperature. In this work we compare the experimentally deduced e∗(T ) to the theoretical predictions. The experimentally accessible temperature was extracted from evaporation spectra from incomplete fusion reactions lea...