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首页> 外文期刊>Chemistry of Materials: A Publication of the American Chemistry Society >Fe_(3_x)inSn_xO6 (x = 0, 0.25, or 0.5): A Family of Corundum Derivatives with Sn-lnduced Polarization and Above Room Temperature Antiferromagnetic Ordering
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Fe_(3_x)inSn_xO6 (x = 0, 0.25, or 0.5): A Family of Corundum Derivatives with Sn-lnduced Polarization and Above Room Temperature Antiferromagnetic Ordering

机译:Fe_(3_x)inSn_xO6 (x = 0, 0.25, or 0.5): A Family of Corundum Derivatives with Sn-lnduced Polarization and Above Room Temperature Antiferromagnetic Ordering

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摘要

Three new double corundum derivative compounds, Fe_(3-x)InSn_xO6 (x = 0. 0.2S, or 0.5), were synthesized at high pressure and temperature (6 GPa and 1400-1450 °C). All of the compounds order antiferromagnetically well above room temperature (T_N = 608, 532, and 432 K for x = 0, 0.25, and 0.5, respectively). The x = 0 phase crystallizes as centrosymmetric R3c, but the inclusion of closed-shell d~(10) Sn ~(4+) induces x = 0.25 and 0.5 to crystallize as noncentrosymmetric R3c. Microprobe measurements indicate that for x = 0.25 and 0.5, the substitution of Sn~(4+) is not offset by vacancies, which implies the presence of Fe~(2+), as corroborated by X-ray absorption near-edge spectroscopy and single-crystal X-ray structure refinements. Neutron powder diffraction experiments on x = 0.5 indicate that these compounds are canted A-type antiferromagnets that, like Fe2O3 and InFeO3, consist of ferromagnetic layers that stack antiferromagnetically with a single magnetic transition. Weak ferromagnetic interactions persist to very high temperatures. Temperature-dependent second harmonic generation (SHG) measurements on x = 0.25 and 0.5 show a SHG responsewith ferroelectric-like hysteretic maxima that correspond with the respective magnetic transitions, which suggest coupling of the magnetic and polarization order. These new compounds provide more information about fine-tuning the electronic, magnetic, and structural properties of corundum-derived mutlferroics in the search for tunable high-temperature magnetoelectric materials.

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