Abstract
Abstract The existing BUU theory of heavy ion collisions is modified to conserve total momentum and retain the two-particle correlations induced by the collision term. In this framework the two-proton correlation function is investigated for heavy ion collisions. For light heavy-ion systems ( 16 O, 12 C) and intermediate beam energies (25–85 MeV/nucleon) the experimental features of the correlation function are reproduced.
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