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Highly crystalline corundum structured α-(Ga0.42Fe0.58)2O3 alloy thin film showed magnetic properties at room temperature. Microstructure analysis of cross-sectional transmission electron microscope (TEM) observation and TEM energy dispersive X-ray spectroscopy measurement indicated that different crystal phase could not be detected as well as there is no remarkable phase separating area, that is, Fe and Ga ions are distributed uniformly in the film. Magnetic measurements were performed on α-(Ga1−xFex)2O3 (x = 0.24, 0.44, 0.58, 1.00) alloy thin films at 110 K. The induced magnetic moment per a Fe ion of α-(Ga0.42Fe0.58)2O3 at 5000 Oe is about 6 times larger than α-Fe2O3 thin film. Compared to the α-Fe2O3 thin films, the value of coercivity is also about 6 times in α-(Ga0.42Fe0.58)2O3, in contrast, there is no significant difference in value of coercivity of α-(Ga1−xFex)2O3 (x = 0.24, 0.44, 1.00) thin films. These means that the origin of magnetism is not the separation region of α-Fe2O3 in α-(Ga0.42Fe0.58)2O3 thin film.
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Kaneko et al. (2013) studied this question.
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