Absorption and emission edge singularities are calculated in the presence of a nonequilibrium Fermi sea μ₁--μ₂ instead of 0--{μ}. The result is used to derive the absorption spectra of highly excited semiconductors. It is also of importance in the problem of x-ray-like singularities as it shows that the well-accepted physical interpretation proposed by Hopfield is actually invalid.
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Tanguy et al. (1992) studied this question.
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