2 research outputs found

    Room-Temperature Polar Ferromagnet ScFeO<sub>3</sub> Transformed from a High-Pressure Orthorhombic Perovskite Phase

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    Multiferroic materials have been the subject of intense study, but it remains a great challenge to synthesize those presenting both magnetic and ferroelectric polarizations at room temperature. In this work, we have successfully obtained LiNbO<sub>3</sub>-type ScFeO<sub>3</sub>, a metastable phase converted from the orthorhombic perovskite formed under 15 GPa at elevated temperatures. A combined structure analysis by synchrotron X-ray and neutron powder diffraction and high-angle annular dark-field scanning transmission electron microscopy imaging reveals that this compound adopts the polar <i>R</i>3<i>c</i> symmetry with a fully ordered arrangement of trivalent Sc and Fe ions, forming highly distorted ScO<sub>6</sub> and FeO<sub>6</sub> octahedra. The calculated spontaneous polarization along the hexagonal <i>c</i>-axis is as large as 100 Ī¼C/cm<sup>2</sup>. The magnetic studies show that LiNbO<sub>3</sub>-type ScFeO<sub>3</sub> is a weak ferromagnet with <i>T</i><sub>N</sub> = 545 K due to a canted <i>G</i>-type antiferromagnetic ordering of Fe<sup>3+</sup> spins, representing the first example of LiNbO<sub>3</sub>-type oxides with magnetic ordering far above room temperature. A comparison of the present compound and rare-earth orthorhombic perovskites RFeO<sub>3</sub> (R = Laā€“Lu and Y), all of which possess the corner-shared FeO<sub>6</sub> octahedral network, allows us to find a correlation between <i>T</i><sub>N</sub> and the Feā€“Oā€“Fe bond angle, indicating that the A-site cation-size-dependent octahedral tilting dominates the magnetic transition through the Feā€“Oā€“Fe superexchange interaction. This work provides a general and versatile strategy to create materials in which ferroelectricity and ferromagnetism coexist at high temperatures

    Room-Temperature Polar Ferromagnet ScFeO<sub>3</sub> Transformed from a High-Pressure Orthorhombic Perovskite Phase

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    Multiferroic materials have been the subject of intense study, but it remains a great challenge to synthesize those presenting both magnetic and ferroelectric polarizations at room temperature. In this work, we have successfully obtained LiNbO<sub>3</sub>-type ScFeO<sub>3</sub>, a metastable phase converted from the orthorhombic perovskite formed under 15 GPa at elevated temperatures. A combined structure analysis by synchrotron X-ray and neutron powder diffraction and high-angle annular dark-field scanning transmission electron microscopy imaging reveals that this compound adopts the polar <i>R</i>3<i>c</i> symmetry with a fully ordered arrangement of trivalent Sc and Fe ions, forming highly distorted ScO<sub>6</sub> and FeO<sub>6</sub> octahedra. The calculated spontaneous polarization along the hexagonal <i>c</i>-axis is as large as 100 Ī¼C/cm<sup>2</sup>. The magnetic studies show that LiNbO<sub>3</sub>-type ScFeO<sub>3</sub> is a weak ferromagnet with <i>T</i><sub>N</sub> = 545 K due to a canted <i>G</i>-type antiferromagnetic ordering of Fe<sup>3+</sup> spins, representing the first example of LiNbO<sub>3</sub>-type oxides with magnetic ordering far above room temperature. A comparison of the present compound and rare-earth orthorhombic perovskites RFeO<sub>3</sub> (R = Laā€“Lu and Y), all of which possess the corner-shared FeO<sub>6</sub> octahedral network, allows us to find a correlation between <i>T</i><sub>N</sub> and the Feā€“Oā€“Fe bond angle, indicating that the A-site cation-size-dependent octahedral tilting dominates the magnetic transition through the Feā€“Oā€“Fe superexchange interaction. This work provides a general and versatile strategy to create materials in which ferroelectricity and ferromagnetism coexist at high temperatures
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