A simple theoretical model is proposed to explain the recently observed valence-band structure of CdSnP₂ and similar chalcopyrite crystals. The valence bands of a chalcopyrite crystal are regarded as equivalent to those of a strained version of its binary analog. This model predicts the signs and magnitudes of the valence-band splittings observed in CdSnP₂ and ZnSiAs₂. We show further that the quasicubic model explains quantitatively the unusual polarization dependences previously reported.
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Rowe et al. (1971) studied this question.
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