Measurements on single crystals of yttrium iron garnet (YIG) doped with cobalt, some counterdoped with silicon or calcium, show that the magnetocrystalline anisotropy is dominated by octahedral Co²⁺ and tetrahedral Co³⁺. Both are present in uncompensated material. We calculate the single-ion anisotropy of ions of the (3d)ⁿ series (n=4-9), incorporated into the various sites of YIG. We find qualitative agreement with experiment in the case of cobalt. A preliminary study of ferrimagnetic resonance in uncompensated cobalt-doped crystals shows that octahedral Co²⁺ does not make the large contribution to the linewidth at 0^∘{}K predicted by Haas and Callen, and indicates that either octahedral Co²⁺ or tetrahedral Co³⁺ relaxes through an excited state 130 cm^-1 above the ground state.
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Sturge et al. (1969) studied this question.
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