Spin reorientation is a magnetic phase transition in which rotation of the magnetization vector with respect to the crystallographic axes occurs upon a change in the temperature or magnetic field. For example, SmFeO 3 shows a magnetization rotation from the c axis above 480K to the a axis below 450K, known as the ? 4 -> ? 2 transition. This work reports the successful synthesis of the new single-crystal perovskite SmFe 0.75 Mn 0.25 O 3 and finds interesting spin reorientations above and below room temperature. In addition to the spin reorientation of the ? 4 -> ? 2 magnetic phase transition observed at around T SR2 = 382K, a new spin reorientation, ? 2 -> ? 1, was seen at around T SR1 = 212K due to Mn doping, which could not be observed in the parent rare earth perovskite compound. This unexpected spin configuration has complete antiferromagnetic order without any canting-induced weak ferromagnetic moment, resulting in zero magnetization in the low-temperature regime. M-T and M-H measurements have been made to study the temperature and magnetic-field dependence of the observed spin reorientation transitions.

Spin-reorientation magnetic transitions in Mn-doped SmFeO 3

Stroppa A;
2017

Abstract

Spin reorientation is a magnetic phase transition in which rotation of the magnetization vector with respect to the crystallographic axes occurs upon a change in the temperature or magnetic field. For example, SmFeO 3 shows a magnetization rotation from the c axis above 480K to the a axis below 450K, known as the ? 4 -> ? 2 transition. This work reports the successful synthesis of the new single-crystal perovskite SmFe 0.75 Mn 0.25 O 3 and finds interesting spin reorientations above and below room temperature. In addition to the spin reorientation of the ? 4 -> ? 2 magnetic phase transition observed at around T SR2 = 382K, a new spin reorientation, ? 2 -> ? 1, was seen at around T SR1 = 212K due to Mn doping, which could not be observed in the parent rare earth perovskite compound. This unexpected spin configuration has complete antiferromagnetic order without any canting-induced weak ferromagnetic moment, resulting in zero magnetization in the low-temperature regime. M-T and M-H measurements have been made to study the temperature and magnetic-field dependence of the observed spin reorientation transitions.
2017
Istituto Superconduttori, materiali innovativi e dispositivi - SPIN
magnetic phase transitions
Mn doping
rare earth perovskites
spin reorientation transitions
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/370692
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