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We present a full-potential band-structure scheme based on the linear combination of overlapping nonorthogonal orbitals. The crystal potential and density are represented as a lattice sum of local overlapping nonspherical contributions. The decomposition of the exchange and correlation potential into local parts is done using a technique of partitioning of unity resulting in local shape functions, which add exactly to unity in the whole crystal and which are very easily treated numerically. The method is all-electron, which means that core relaxation is properly taken into account. Nevertheless, the eigenvalue problem is reduced to the dimension of a minimum valence orbital basis only. Calculations on sp and transition metals give results comparable to other full-potential methods. The calculations on the diamond lattice demonstrate the applicability of our approach to open structures. The consequent local description of all real-space functions allows the treatment of substitutional disordered materials.
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Klaus Koepernik
United States Naval Research Laboratory
H. Eschrig
Uppsala University
Physical review. B, Condensed matter
Max Planck Institute for the Physics of Complex Systems
Leibniz Institute for Solid State and Materials Research
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Koepernik et al. (Fri,) studied this question.
synapsesocial.com/papers/69d9a2df1ad561c673684d16 — DOI: https://doi.org/10.1103/physrevb.59.1743
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