Abstract

A nonperturbative theory of anharmonic multiphonon decay of strong local vibrations in crystals is presented. The theory predicts a slow-down of the decay at large amplitudes, and a jump-like acceleration of the decay near the critical amplitudes of ~ 0.3 Å. A local vibration with such or larger amplitude is created, e.g. on exciting self-trapped excitons in solid Xe. The time evolution of this vibration manifests itself in the hot luminescence of this crystal. A comparison of the calculated and the observed spectra allows one to conclude that the relaxation rate of the self-trapped exciton in solid Xe has indeed a strong maximum at the amplitude of ~ 0.3 Å.

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