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Simplified LCAO Method for the Periodic Potential Problemby: J. C. Slater, G. F. Koster
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AbstractThe LCAO; or Bloch; or tight binding; approximation for solids is discussed as an interpolation method; to be used in connection with more accurate calculations made by the cellular or orthogonalized plane-wave methods. It is proposed that the various integrals be obtained as disposable constants; so that the tight binding method will agree with accurate calculations at symmetry points in the Brillouin zone for which these calculations have been made; and that the LCAO method then be used for making calculations throughout the Brillouin zone. A general discussion of the method is given; including tables of matrix components of energy for simple cubic; face-centered and body-centered cubic; and diamond structures. Applications are given to the results of Fletcher and Wohlfarth on Ni; and Howarth on Cu; as illustrations of the fcc case. In discussing the bcc case; the splitting of the energy bands in chromium by an antiferromagnetic alternating potential is worked out; as well as a distribution of energy states for the case of no antiferromagnetism. For diamond; comparisons are made with the calculations of Herman; using the orthogonalized plane-wave method. The case of such crystals as InSb is discussed; and it is shown that their properties fit in with the energy band picture.
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