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Theory of Antiferromagnetic Resonance
Phys. Rev. 85, 329 – Published 15 January, 1952
DOI: https://doi.org/10.1103/PhysRev.85.329
Abstract
The spin resonance condition previously given by Kittel for a disk-shaped single-domain uniaxial or cubic antiferromagnetic crystal at 0°K with parallel to the domain axis is extended by classical calculations to cover finite temperature, ellipsoidal shape, orthorhombic symmetry, generalized two-lattice anisotropy, and arbitrary static field direction. The normal precessional modes are discussed. A quantum-mechanical derivation of the resonance equations is carried out by the method developed by Van Vleck for ferromagnetic resonance; no new features are introduced by the quantum-mechanical calculation. Several factors contributing to the line width are considered. Existing experimental data on antiferromagnetic resonance are reviewed; the data are scanty and taken in circumstances not closely related to the situation envisaged by the theory.
References (19)
- C. Kittel, Phys. Rev. 82, 565 (1951)
- Poulis, van den Handel, Ubbink, Poulis, and Gorter, Phys. Rev. 82, 552 (1951)
- J. H. Van Vleck, Phys. Rev. 78, 266 (1950)
- J. H. Van Vleck, J. Chem. Phys. 9, 85 (1941) J. phys. et radium 12, 262 (1951)
- P. W. Anderson, Phys. Rev. 83, 1260 (1951)
- Shull, Strauser, and Wollan, Phys. Rev. 83, 333 (1951)
- J. H. Van Vleck, Phys. Rev. 74, 1168 (1948)
Omitted endnote
Omitted endnote
- [2]
- T. Nagamiya, Prog. Theor. Phys. 6, 342 (1951)
Omitted endnote
- J. H. Van Vleck, Phys. Rev. 52, 1178 (1937)
- C. Guillaud, Ferromagnétisme des alliages binaires de manganèse, thesis, Strasbourg, 1943
- J. H. Van Vleck, Phys. Rev. 74, 1168 (1948)
- [6]
- C. A. Hutchison (private communication)
- Trounson, Bleil, Wangsness, and Maxwell, Phys. Rev. 79, 542 (1950)
- Okamura, Torizuka, and Kojima, Phys. Rev. 82, 285 (1951)