Influence of inhomogeneities in magnetic crystal on ferromagnetic resonance line shape

The general theory of the preceding paper is applied to a concrete case. The spin wave interaction operator, ^s , is derived by quantizing a phenomenological expression, which expresses the contribution to the energy of the magnetic sample, caused by fluctuations in the anisotropic and exchange interaction. The influence of thermally excited spin waves on the absorption of energy from a high-frequency field and the justification for the application of the general results of the preceding paper are discussed on the basis of the form of the operator ^s . The interaction operator of the magnetic sample with the h-f field is also determined, and it is used to give a definite form to the expression for the resonance curve of the imaginary part of the susceptibility '. Using the matrix elements of the operator ^s we calculate the quantitiy, which formally corresponds to the width of the resonance -curve. The magnitude of is estimated numerically and our results are compared with those obtained by A. M. Clogston et al. and E. Schlömann for the line width in monocrystals and the shape of the resonance curve in polycrystals respectively. The expression obtained on the basis of the theory of the preceding paper for the frequency shift diverges in our case. The way in which to avoid this divergence is indicated.

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. , ^s , , , . ^s , , . , . ^s , . . . , , . .

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The author would like to thank S. Krupika for advice and remarks during the work, J. Duek, V. Syneek, and J. ternberk for valuable discussions and F. Zounová for help in the numerical calculations.