Abstract
A solution of Maxwell equations for the propagation of electromagnetic waves in a metallic ferromagnet is presented for the region of ferromagnetic antiresonance; the magnetization vector motion is described by the Landau-Liftshitz equation, the metal sample is in the form of a flat disc statistically magnetized in its surface plane (parallel configuration). The dispersion relations for the three waves of (complex) electromagnetic spin wave origin, the surface impedance and the shifts of antiresonance point due to the damping and electrical conductivity are computed in the analytical form.
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I would like to thank Z. Frait for valuable discussions concerning the AR effect and experimental details of AR measurements, also I am indebted to A. Sládek and M. Jirsa for their contributions and comments on the manuscript.
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Fraitová, D. Theory of ferromagnetic antiresonance in parallel configuration in metals. Czech J Phys 30, 563–572 (1980). https://doi.org/10.1007/BF01596305
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DOI: https://doi.org/10.1007/BF01596305