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Experiences with the Quadratic Korringa-Kohn-Rostoker Band Theory Method

Published online by Cambridge University Press:  25 February 2011

J. S. Faulkner*
Affiliation:
Alloy Research Center and Department of Physics, Florida Atlantic University, Boca Raton, Florida 33431.
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Abstract

The Quadratic Korringa-Kohn-Rostoker method is a fast band theory method in the sense that all eigenvalues for a given k are obtained from one matrix diagonalization, but it differs from other fast band theory methods in that it is derived entirely from multiple-scattering theory, without the introduction of a Rayleigh-Ritz variational step. In this theory, the atomic potentials are shifted by Δασ(r) with Δ equal to E-E0 and σ(r) equal to one when r is inside the Wigner-Seitz cell and zero otherwise, and it turns out that the matrix of coefficients is an entire function of Δ. This matrix can be terminated to give a linear KKR, quadratic KKR, cubic KKR, …, or not terminated at all to give the pivoted multiple-scattering equations. Full potentials are no harder to deal with than potentials with a shape approximation.

Type
Research Article
Copyright
Copyright © Materials Research Society 1992

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References

REFERENCES

1. Korringa, J., Physica 13, 392 (1947).Google Scholar
2. Kohn, W. and Rostoker, N., Phys. Rev. 94, 111 (1954).CrossRefGoogle Scholar
3. Rayleigh, Lord, Philos. Mag. 34, 481 (1892).Google Scholar
4. Faulkner, J. S., Phys. Rev. B 19(12): 6186-206 (1979).Google Scholar
5. Anderson, O. K., Phys. Rev. B 12, 3060 (1975).Google Scholar
6. Williams, A. R., Kubler, J., and Gelatt, G. D. Jr., Phys. Rev. B 19, 6094 (1979).CrossRefGoogle Scholar
7. Koelling, D. D. and Arbman, G. O., J. Phys. F 9, 661, (1975). See also O. K. Anderson, Mont Tremblant Lectures, unpublished (1974).Google Scholar
8. Faulkner, J. S. and Beaulac, T. P., Phys. Rev. B 26(4), 1597 (1982).CrossRefGoogle Scholar
9. Nicholson, D. M. and Faulkner, J. S., Phys. Rev. B 39, 8187 (1989).Google Scholar
10. Faulkner, J. S., Horvath, Eva A., and Nicholson, D. M., Phys. Rev. B 44, 8467 (1991).CrossRefGoogle Scholar
11. Wang, Y., Faulkner, J. S., and Nicholson, D. M., Phys. Rev. B, accepted for publication (1992).Google Scholar
12. Andriotis, A., Nicholson, D. M., and Faulkner, J. S., submitted (1992).Google Scholar
13. Faulkner, J. S., Phys. Rev. B 34, 5931(1986).Google Scholar
14. Faulkner, J. S., International Journal of Quantum Chemistry, accepted for publication(1992).Google Scholar