The change in the absorption coefficient $\ensuremath{\Delta}\ensuremath{\alpha}=\ensuremath{\alpha}(\ensuremath{\omega}, \mathcal{E})\ensuremath{-}\ensuremath{\alpha}(\ensuremath{\omega}, 0)$ due to the presence of an electric field $\mathcal{E}$ has been measured for the indirect-absorption edges of silicon and germanium and for the direct-absorption edge in germanium. The results show good qualitative agreement with the theoretical predictions. The quantitative deviations are caused by the presence of excitons and thermal and electric-field broadening, which have not been taken into account in the theory. The energies of the phonons which take part in indirect optical absorption have been determined from the room-temperature data and are in very good agreement with the values found at liquid-helium temperatures by other means.
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