1965 年 20 巻 6 号 p. 980-984
The ferrimagnetic resonance in a cubic phase single crystal of CuFe2O4 was measured with an X-band spectrometer from 77°K to 300°K. At room temperature, K1⁄M (the 1’st order cubic anisotropy field) and geff (effective g-value) are −172 Oe and 2.09, respectively. At liquid nitrogen temperature, they are −810 Oe and 2.44. The half line width is maximum (85 Oe at RT) around [100] (a hard direction of magnetization). K1⁄M extraporated down to 0°K is about −900 Oe and K1 (0°K) is −9.7×10−2 cm−1 per molecule. This value of K1 (0°K) may be understood as arising from the single ion anisotropy of Fe3+ due to cubic crystal field splitting, and a value of aB (Fe3+) (fine structure constant of Fe3+ on B-site in cubic crystal field) derived under some assumptions is +2.8×10−2 cm−1.
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