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A systematical study of the perpendicular component of the magnetization in single crystals is carried out. Using the model of Stoner and Wohlfarth and restricting to the first‐order anisotropy constant K 1 , the perpendicular component m ⊥ as a function of h for different angles 9 is calculated. A practicable alternative method to determine the anisotropy field H a from the point of intersection of the second derivatives of different m ⊥ (h) curves is presented.
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Hermann et al. (1992) studied this question.
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