Abstract
The band structure of body-centered cubic beryllium is reported, both at the Hartree and exact-exchange Hartree-Fock level. There is no gap immediately above the valence band. This is consistent with the resistivity experiments by Amonenko et al. which rises sharply, but not discontinuously above the h.c.p.-to-b.c.c. phase transition at 1254°C.
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