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Materials undergoing magnetoelastic and magnetostructural phase transitions hold significant promise for various applications. These transitions involve changes in both the magnetic and elastic subsystems, with the order of the transition governed by the interaction between these subsystems. A special version of Landau-type theory has been developed to quantitatively capture the physical effects accompanying magnetostructural and magnetoelastic phase transitions in multiferroic materials. This approach is based on the analysis of the Gibbs potential, incorporating both magnetic and elastic subsystems and their interplay. This framework allows to describe:
1) the influence of magnetoelastic coupling on the H-T phase diagram during the anisotropic magnetoelastic phase transition in (Mn, Fe)?(P, Si) alloys [1]. It has been shown that the jump in lattice parameters leads to the appearance of hysteresis during the paramagnetic-ferromagnetic phase transition. The magnetoelastic coupling also affects the coordinates of the critical point on the H-T phase diagram, where the first-order phase transition becomes a second-order transition. It’s noteworthy that the interrelation between the critical point and thermal hysteresis has been theoretically predicted for structural phase transitions in Heusler alloys [2] and confirmed experimentally for Fe–Pd alloys [3].
2) the inverse magnetocaloric effect in the Fe-Rh alloy, which undergoes the isotropic magnetoelastic ferromagnetic-antiferromagnetic phase transition [4]. The magnetic-field-induced shift of the phase transition temperature has been calculated and the dependence of the phase transition field on the temperature has been computed. The experimentally observed features of the MCE in the Fe-Rh alloy were explained.
3) the conventional MCE observed during the magnetic Curie transition and giant inverse MCE caused by the magnetostructural phase transition from ferromagnetic austenite to a weakly magnetic martensite [5,6]. It has been shown that the contributions of the elastic and magnetic subsystems to the specific heat are close in magnitude in the temperature range of magnetostructural phase transition.
The Landau-type phenomenological approach bridges macroscopic observations and microscopic models, enhancing the understanding of phase transitions to facilitate the development of novel materials with tailored properties.
[1] Z. Wang, E. Dengina, A. Kosogor, T. Hiroto, X. Tang, N. Kulesh, ... & H. Sepehri-Amin, Materialia, 37, 102195 (2024).
[2] A. Kosogor, N.J. Matsishin, V.A. L’vov, Phase Trans. 86, 796 (2013).
[3] F. Xiao, T. Fukuda, T. Kakeshita, Phil. Mag. 95, 1390 (2015).
[4] V.A. L'vov, A. Kosogor, J. Magn. Magn. Mater. 517, 167269 (2021).
[5] V.A. L'vov, A. Kosogor, J.M. Barandiaran, V.A. Chernenko, J. Appl. Phys. 119, 013902 (2016).
[6] A. Kosogor, J.M. Barandiaran, V.A. L'vov, J.R. Fernandez, V.A. Chernenko, J. Appl. Phys. 121, 183901 (2017).