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Magnetic phase transitions induced by the field H = (<i>H</i> <i>x</i>, <i>H</i> <i>y</i>, 0) in dysprosium orthoferrite

S. L. GnatchenkoPhysicotechnical Institute of Low Temperatures, Academy of Sciences of the Ukrainian SSR, Kharkov 1P. P. LebedevPhysicotechnical Institute of Low Temperatures, Academy of Sciences of the Ukrainian SSR, Kharkov 1N. F. KharchenkoPhysicotechnical Institute of Low Temperatures, Academy of Sciences of the Ukrainian SSR, Kharkov 1K. PiotrowskiInstitute of Physics, Polish Academy of Sciences, Warsaw 2R. SzymcżakInstitute of Physics, Polish Academy of Sciences, Warsaw 2
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Spin-flip transitions induced by a magnetic field oriented in the ab plane of a crystal are investigated in dysprosium orthoferrite. A tilted field H = (Hx, Hy, 0) is shown to induce a first-order phase transition between the Γ124-type states with a spatial orientation of the ferro- and antiferromagnetism vectors. The magnetic H-T phase diagrams of DyFeO3 with different orientations of the field in the ab plane are constructed. It is found that the orientation of H at an angle of α* ≈ 62° to the a-axis is such that the high-temperature (Γ ′124) and low-temperature (Γ ″124) phases at the Morin point are energetically equivalent in the entire interval of investigated magnetic fields. The magnetic field H = (Hx, Hy. 0) induces in the temperature interval T &amp;lt; TM a phase transition between the Γ124-type states only for α &amp;gt; α*, and in the temperature region T &amp;gt; TM, only for α &amp;lt; α*.

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