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Inter-valence-band scattering induced by carrier-carrier interaction and carrier acoustic-phonon interaction has been neglected in our calculations.
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Using a thermopile we have found that the surface temperature of the samples is generally higher (by ∼25–40 K) than room temperature due to heating by the pump beam. For our pump geometry, the carrier density mentioned in the text corresponded to an average pump beam power of ∼100 mW.
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