2 research outputs found
Room-Temperature Polar Ferromagnet ScFeO<sub>3</sub> Transformed from a High-Pressure Orthorhombic Perovskite Phase
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 = LaāLu 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 FeāOāFe bond angle, indicating
that the A-site cation-size-dependent octahedral tilting dominates
the magnetic transition through the FeāOāFe 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
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 = LaāLu 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 FeāOāFe bond angle, indicating
that the A-site cation-size-dependent octahedral tilting dominates
the magnetic transition through the FeāOāFe superexchange
interaction. This work provides a general and versatile strategy to
create materials in which ferroelectricity and ferromagnetism coexist
at high temperatures