Parallel pump and subsidiary absorption thresholds at 9.1 GHz and effective linewidth (ΔHeff) at 9.9 GHz have been measured for polycrystalline YIG samples with average grain diameter a0 from 1 to 30 μ. The spin-wave linewidths extrapolated to zero wavenumber, ΔHk→0, vary as a0−1. The ΔHk for a0=1 μ shows an inverse k dependence. A simple model in which the spin-wave transit time across individual grains limits ΔHk explains the a0−1 dependence but not the observed k dependences for ΔHk. The high-field ΔHeff is 5.5 Oe for a0=1 μ and varies as a0−1/2. These ΔHeff are significantly larger than single-crystal linewidths. Two-magnon interactions cannot contribute to the high-field ΔHeff. A recently proposed magnetostriction mechanism is consistent with the a0−1/2 dependence, but the predicted magnitudes are much smaller than observed.
No takes yet. Share an insight, caveat, or question.
Carl E. Patton (1970) studied this question.
Synapse has enriched 3 closely related papers on similar clinical questions. Consider them for comparative context: