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Correlation Functions for Single-Particle Problems

  • Wilhelm Brenig

Abstract

An important field for the application of transport theories has always been electrical conduction in solids. Particularly simple, at least with respect to many-body effects, is the residual resistivity due to the scattering of electrons by impurities and imperfections. Normally this mechanism governs the conduction at low temperatures, where contributions from electron-phonon and electron-electron interactions are frozen out and one can describe the situation approximately by a single-particle Hamiltonian
$$\underset{\raise0.3em\hbox{$\smash{\scriptscriptstyle-}$}}{H} = {\sum {\bar h\omega } _\mu }c_\mu ^*{c_u}.$$
(42.1)

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References

  1. 42.1
    Greenwood, D.A.: Proc. R. Soc. London 87, 775 (1966)CrossRefGoogle Scholar
  2. 42.2
    Lindhard, J.: K. Dansk. Vidensk. Selsk., Mat.-Fys. Medd. 28, No. 8 (1954)MathSciNetGoogle Scholar

Copyright information

© Springer-Verlag Berlin Heidelberg 1989

Authors and Affiliations

  • Wilhelm Brenig
    • 1
  1. 1.Physik-DepartmentTechnische Universität MünchenGarchingFed. Rep. of Germany

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