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This paper reports the first observation of the optical mixing due to conduction electrons in n-type germanium. The measured magnitude and anisotropy of the third-order susceptibilities are found to be in good agreement with the nonparabolicity effect calculated with a →k·→p method involving eight bands at the L point in the reciprocal lattice. It is concluded that the mechanism of momentum-dependent relaxation times contributes negligibly to the observed nonlinearity.
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Wang et al. (1970) studied this question.
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