Expansion of the Hexagonal Phase-Forming Region of
Lu<sub>1–<i>x</i></sub>Sc<sub><i>x</i></sub>FeO<sub>3</sub> by Containerless Processing
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Abstract
Hexagonal Lu<sub>1–<i>x</i></sub>Sc<sub><i>x</i></sub>FeO<sub>3</sub> (0
≤ <i>x</i> ≤ 0.8) was directly solidified
from an undercooled melt by containerless processing with an aerodynamic
levitation furnace. The hexagonal phase-forming region was considerably
extended compared to that of the conventional solid-state reaction
(<i>x</i> ∼ 0.5). Synchrotron X-ray diffraction measurements
revealed that the crystal structure of the hexagonal phase was isomorphous
to hexagonal ferroelectric RMnO<sub>3</sub> (R = a rare earth ion)
with a polar space group of <i>P</i>6<sub>3</sub><i>cm</i>. As <i>x</i> increased, the <i>a</i>-axis lattice constant decreased linearly, strengthening the antiferromagnetic
interaction between the Fe<sup>3+</sup> ions on the <i>a–b</i> plane. Accordingly, the weak ferromagnetic transition temperature
increased from 150 K for <i>x</i> = 0 to 175 K for <i>x</i> = 0.7. These transition temperatures were much higher
than those of hexagonal Lu<sub>1–<i>x</i></sub>Sc<sub><i>x</i></sub>MnO<sub>3</sub>. The results indicate that
hexagonal Lu<sub>1–<i>x</i></sub>Sc<sub><i>x</i></sub>FeO<sub>3</sub> is a suitable alternative magnetic dielectric
for use at higher temperatures