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- W4237656102 abstract "The spin resonance condition $frac{ensuremath{omega}}{ensuremath{gamma}}={H}_{0}ifmmodepmelsetextpmfi{}{[{H}_{A}(2{H}_{E}+{H}_{A})]}^{frac{1}{2}}$ previously given by Kittel for a disk-shaped single-domain uniaxial or cubic antiferromagnetic crystal at 0ifmmode^circelsetextdegreefi{}K with ${H}_{0}$ 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." @default.
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- W4237656102 date "1952-01-15" @default.
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- W4237656102 title "Theory of Antiferromagnetic Resonance" @default.
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- W4237656102 doi "https://doi.org/10.1103/physrev.85.329" @default.
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