The energy spectra of atoms ejected as a result of the electronic excitation of rare-gas solids by keV electrons and He⁺ ions are presented. These spectra are found to have a well-defined structure with two distinct features indicative of nonradiative electronic relaxation processes. The higher-energy peak is due to radiative decay of vibrationally relaxed dimers that are either desorbed or weakly bound to the surface. The lower-energy peak exhibits a trend from Ar to Xe which is shown to be determined by subsurface dimer decays and is consistent with the trend in the cohesive energy.
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O’Shaughnessy et al. (1988) studied this question.
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