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 values. As before, this derivation is carried out to second order in , 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