Abstract
Dynamic susceptibility of a 3d metal is obtained in the Brooks tight-binding mean-field approximation (including orbital moments and spin-orbit interaction). The result is compatible with the Kittel-Van Vleck g-factor theory and the classical phenomenology of anisotropy shifts. Values ofg for Ni and Fe are computed numerically. Dominant contributions to anisotropy in Ni are derived from Bloch states with wave vectors close to 〈001〉 and orbital moments “quenched” along these axes. The role of non-collinearity of spin alignment in Bloch representation is pointed out.
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Dedicated to Academician Vladimír Hajko on the occasion of his 65th birthday.
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Kamberský, V. Magnetic anisotropy and dynamic susceptibility of 3d metals. Czech J Phys 35, 1239–1258 (1985). https://doi.org/10.1007/BF01597010
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DOI: https://doi.org/10.1007/BF01597010