Abstract

The classical limit of the statistical description of light-particle emission from spherical and deformed nuclei is outlined. Topics covered include classical integral representation for vector addition coefficients and spherical functions, the validity criterion of the classical limit, incorporation of the emitter deformation into statistical theory and a Monte Carlo algorithm for the angular distribution of light particles evaporated by deformed nuclei. Examples are given of the strong influence of deformation on the spectroscopic information concerning continuum states extracted via particle emission.

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