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Nonrelativistic band calculations of Mattheiss for Nb and Petroff and Viswanathan for Mo are used to calculate the imaginary part ε₂ of the dielectric function for these metals. The structure resulting from interband transitions in the frequency range 0.1-0.5 Ry is found to give fairly good agreement with experiment. The calculation indicates that structure in ε₂ can arise from transitions away from symmetry points and lines in the Brillouin zone. The difficulty in distinguishing between the direct and indirect transition models for ε₂ is shown to arise from a lack of strong optical critical points. Predictions of the rigid-band model for the optical properties of Nb-Mo alloys are presented.
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Pickett et al. (1975) studied this question.
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