Abstract

Multifragmentation resulting from an expanding nuclear matter is investigated on the basis of quantum molecular dynamics. In particular, the dependence of the fragment mass distribution on the initial temperature ${(T}_{\mathrm{init}})$ and the radial flow velocity $(h)$ is studied. When $h$ is large, the distribution shows exponential shape, whereas for small $h,$ it obeys the power law. Although the power law is what Fisher's droplet model predicts, the fragmentation mechanism in an expanding system is found to be different from the one in a thermally equilibrated system.

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