A simple method, analogous to the Thomas‐Fermi approximation, is described for constructing approximations to electronic states in structurally disordered ‘solids’ when at least part of the Hamiltonian may be represented in terms of localised orbitals and when the range of interaction of the orbitals is comparable with short‐range order present in the solid. A resistivity formula is also proposed for liquid transition metals.
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Brown et al. (1979) studied this question.
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