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By V A Chernenko

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D. Coey, J. Magn. Magn. Mater. 167, L7 (1997). [129] H. C. Herper and P. Entel, MSE 2010, Darmstadt, Germany, August 24-28. [130] R. P. Bajpai, M. Ono, Y. Ohno and T. Toya, Phys. Rev. B 12, 2194 (1975). [131] G. C. Abell, Metall. Trans. 19A, 177 (1988). [132] P. Norman, Aust. J. Phys. 46, 689 (1993). [133] A. Y. Liu, A. A. Quong, J. K. Freericks, E. J. Nicol and E. C. Jones, Phys. Rev. B 59, 4028 (1999). [134] H. S. -H. Kwon, J. S. Baskin and B. Barwick, Nano Lett. 9, 3954 (2009). 31 Magnetic Anisotropy of Ferromagnetic Martensites Victor L´vov1,2,a and Volodymyr Chernenko3,4,b 1 Taras Shevchenko University, Department of Radiophysics, Kyiv 03127, Ukraine 2 Institute of Magnetism, Vernadsky str.

Siewert, M. E. Gruner, M. Wuttig and P. Entel, Proc. EMRS 2010, Strasbourg 2010, in print. [41] G. E. Bacon and J. S. Plant, J. Phys. F: Metal Phys. 1, 524 (1971). [42] J. Thoene, S. Chadov, G. Fecher, C. Felser and J. Kübler, J. Phys. D: Appl. Phys. 42, 084013 (2009). [43] G. Kresse and D. Joubert, Phys. Rev. B 59, 1758 (1999). [44] K. R. A. Ziebeck and P. J. Webster, Phil. Mag. 34, 973 (1976). [45] K. Miyamoto, A. Kimure, K. Iori, K. Sakamoto, T. Xie, T. Moko, S. Qiao, M. Taniguchi and K. Tsuchiya, J.

36) results in the expressions for MAED of the z- or y- variant, respectively (see Eqs. (10) and (20)). In the case when the volume fractions of z- and y-variants are equal to each other ( α = 1 / 2 ), the Equation (35) transforms into the expression FA( zy ) = 1 K u mx2 , 2 (37) which describes the ferromagnet with magnetocrystalline anisotropy of the "easy plane" type, because the anisotropy constant K u is positive (see Eq. (11) and take into account the inequalities δ < 0 and c / a < 1 ). According to the model, the fine yz-structure is isotropic in yz-plane when the volume fractions of twin components are equal to each other.

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