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Transport Theory in Strong Magnetic Fields

H. F. Budd*

  • Groupe de Physique des Solides de l'Ecole Normale Supérieure 9, quai Saint-Bernard, Paris, France

  • *Associated with Centre National de la Recherche Scientifique.

Phys. Rev. 175, 241 – Published 5 November, 1968

DOI: https://doi.org/10.1103/PhysRev.175.241

Abstract

A unified treatment of transport phenomena in crossed electric and magnetic fields is presented. This theory is limited to strong magnetic fields, ωcτ¯1, where ωc and 1τ¯ are the cyclotron and mean collision frequencies, respectively. It is not, however, limited to linear response in the electric field nor is a relaxation time approximation introduced. The semiclassical and quantum theories are developed along parallel lines.

An irreversible transport equation is derived for the asymptotic state of the system, ωcτ, and it is shown that the asymptotic electron distribution is independent of the absolute values of the coupling constants to the scattering system, but dependent on the form of the scattering interaction. A perturbation theory in 1ωcτ¯ is performed and a generalized orbit-jump formula for the dissipative current is derived. Explicit expressions are derived for the ohmic case and are applied as an example to polar optical-phonon scattering.

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