Theory of spin resonance in dilute magnetic alloys. II

John Sweer, David C. Langreth, and John W. Wilkins
Phys. Rev. B 13, 192 – Published 1 January 1976
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Abstract

The previous derivation by two of the authors of coupled Bloch equations appropriate to conduction-electron spin resonance is extended to the case where the conduction electrons and localized spins have different g values. As before, this derivation is carried out to second order in J, the exchange interaction between the two species. The derivation is also carried out in the presence of the hyperfine interaction between the nuclear spins and the electon spins of the localized impurities. Finally the form of the coupled equations when there exists "direct relaxation" is discussed and some rather unexpected features are found.

  • Received 3 March 1975

DOI:https://doi.org/10.1103/PhysRevB.13.192

©1976 American Physical Society

Authors & Affiliations

John Sweer*,†

  • Department of Physics, Rutgers University, New Brunswick, New Jersey 08903

David C. Langreth†,‡

  • Department of Physics, University of California, San Diego, La Jolla, California 92037
  • Department of Physics, Rutgers University, New Brunswick, New Jersey 08903

John W. Wilkins§

  • Laboratory of Atomic and Solid State Physics, Cornell University, Ithaca, New York 14853

  • *This work was based in part on the dissertation notes of John Sweer, a pre-doctoral student at Rutgers University, whose untimely death occurred on October 26, 1973.
  • Work supported in part by the National Science Foundation Grants NOSO GP-29262 and GH-38995.
  • Rutgers University Research Council Fellow.
  • §Work supported in part by the National Science Foundation through Grant No. DMR74-23494.

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Vol. 13, Iss. 1 — 1 January 1976

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