Abstract
The contribution to the magnetocrystalline anisotropy of transition-metal ions in ferrites on octahedral sites is calculated for the strong crystalline-field case for d1, d2, d4, and d5 configurations. The single-ion model is used which requires small concentrations of such ions. Good agreement with experiment was found for trivalent ruthenium. For this case, anisotropy measurements of Ru3+ (4d5)-doped yttrium-iron garnet of the composition Y3yCayFe5xRuxO12 were carried out in the temperature range of 4.2-500°K. By fitting the theory to the measured anisotropy data, one finds for the product of the g factor times the exchange field, gHe=1.1×107 Oe and the ratio of the trigonal field to the spin-orbit energy vξ=1.