Abstract
We theoretically investigated magnetocrystalline anisotropy (MA) at a finite temperature in ferromagnetic metals. Assuming a Rashba-type ferromagnet with uniaxial MA, we defined the MA constants derived from several different concepts. Our purpose was to examine the equality between them and to confirm a power law between and magnetization in the form of . We demonstrate that equals 2 in the itinerant-electron limit and increases with the localized feature of electrons passing through , predicted for the single-ion MA in spin models.
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