Skip to main content

Optical Properties of the Alkalis Using the KKR-Z Method

  • Chapter
Computational Methods in Band Theory

Part of the book series: The IBM Research Symposia Series ((IRSS))

  • 261 Accesses

Abstract

We have calculated the inter band absorption of potassium and sodium by means of a KKR-Z pseudopotential1,2 obtained from a fit to the experimental Fermi surface data. Previous calculations of the optical properties of the alkali metals have relied either on a local pseudopotential3 or else introduced non-locality as arising solely from the corrections due to the atomic core.4 However, it has been demonstrated that the local pseudopotential formulation5 is inadequate to account for the measured Fermi surface of K. It has also been shown6 that the pseudopotential that appears in the optical matrix element will incorporate the effects of many-body correlations only if it is consistent with the experimental data of Fermi surface measurements (such as dHvA results). The method used here was applied with this requirement being satisfied. Recent theoretical results6 and the successful application of a phenomenological model for the optical properties of Aℓ7 suggest that a one-electron potential which has been fitted to the experimental Fermi surface should implicitly contain electron-electron effects in the optical absorption. The measurement of the inter-band absorption of the alkalis, although difficult to carry out, is nevertheless of some importance as the absorption depends critically on the pseudopotential.

This work was sponsored by the Department of the Air Force.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 39.99
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 54.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Preview

Unable to display preview. Download preview PDF.

Unable to display preview. Download preview PDF.

References

  1. G. J. Morgan, Proc. Phys. Soc. 89, 365 (1966).

    Article  Google Scholar 

  2. J. M. Ziman, Proc. Phys. Soc., 86 337 (1965).

    Article  Google Scholar 

  3. P. N. Butcher, Proc. Phys. Soc. 64, 765 (1951).

    Google Scholar 

  4. J. A. Appelbaum, Phys. Rev. 144, 435 (1966); A. O. E. Aimalu, Phys. Rev. 163, 557 (1967).

    Article  Google Scholar 

  5. M. J. G. Lee and L. M. Falicov, Proc. Roy. Soc. A304, 319 (1968).

    Article  Google Scholar 

  6. C-Y. Young, Bull. Am. Phys. Soc. Series II, 15, 368 (1970) and also to be published.

    Google Scholar 

  7. G. Dresselhaus, M. S. Dresselhaus and D. Beaglehole, Proc. Density of States Conf. (1969).

    Google Scholar 

  8. M. J. G. Lee, Proc. Roy. Soc. A295, 440 (1966).

    Article  Google Scholar 

  9. D. Shoenberg and P. J. Stiles, Proc. Roy. Soc. A281, 62 (1964).

    Article  Google Scholar 

  10. M. J. G. Lee, Phys. Rev. 178, 953 (1969). In his fit of the Fermi surface, Lee has used the APW method with 30 plane waves. We have used as few as possible (19) to allow us to obtain a reasonably accurate fit, since the computation time involved in the calculation of the optical absorption would be prohibitive with a larger matrix. Because a different number of plane waves were used, the phase shifts obtained by us cannot be directly compared with those of Lee.

    Article  Google Scholar 

  11. N. W. Ashcroft, Phys. Rev. 140, A935 (1965).

    Article  Google Scholar 

  12. N. V. Smith, Phys. Rev. 183, 634 (1969).

    Article  Google Scholar 

  13. C. J. Powell, Bull. Am. Phys. Soc. Series II, 15, 576 (1970) and also to be published.

    Google Scholar 

  14. A major contribution to the volume integral comes from the matrix element \(\left\langle {\overrightarrow k + {{\overrightarrow G }_{110}}\left| \Gamma \right|\overrightarrow k } \right\rangle\) in the direction of backscattering \(\cos {\theta _{\overrightarrow k ,\overrightarrow k + {{\overrightarrow G }_{110}}}} = \pi .\). The value of the corresponding matrix element in Lee’s calculation10 is about the same as ours. We would consequently expect that the optical absorption in K calculated by the two methods be similar.

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Editor information

Editors and Affiliations

Rights and permissions

Reprints and permissions

Copyright information

© 1971 Plenum Press, New York

About this chapter

Cite this chapter

Wilson, A.R., Dresselhaus, G., Young, CY. (1971). Optical Properties of the Alkalis Using the KKR-Z Method. In: Marcus, P.M., Janak, J.F., Williams, A.R. (eds) Computational Methods in Band Theory. The IBM Research Symposia Series. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-1890-3_18

Download citation

  • DOI: https://doi.org/10.1007/978-1-4684-1890-3_18

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4684-1892-7

  • Online ISBN: 978-1-4684-1890-3

  • eBook Packages: Springer Book Archive

Publish with us

Policies and ethics