Phonon dispersion and density-of-states measurements are presented for VN, a cubic transition-metal compound with ten valence electrons. The acoustic phonons differ strongly from those observed in nine-valence-electron compounds. In particular, the prominent soft-mode region has moved from the interior to the boundary of the Brillouin zone. Using the theory of Varma and Weber, we find that these changes arise primarily from a rigid-band-like increase in the Fermi energy.
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Weber et al. (1979) studied this question.
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