It is shown that it should be possible to reduce the dominant two-magnon linewidth well below the smallest value obtained to date by choosing the radius R and thickness S of a thin film of ferromagnetic insulator such that there are no modes degenerate with the main-resonance mode. For a sufficiently thin sample (S1μ) the frequencies of the exchange modes are well above that of the main-resonance mode, and for a sufficiently small aspect ratio (2R/S3×10³) the low-order magnetostatic modes are also well resolved. In the limit of no two-magnon scattering, the resonance linewidth of yttrium iron garnet at 9.3 GHz approaches 0.2 Oe at 300^∘{}K, or a few mOe at 4.2^∘{}K.
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M. Sparks (1969) studied this question.
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