Ferromagnetic–paramagnetic transition temperature in bulk and nanostructured La0.7SrxCa0.3-xMnO3(x=0.10, 0.15, and 0.20) manganite materials
Series of bulk and nanostructured La0.7SrxCa0.3-xMnO3(x = 0.10, 0.15, and 0.20) manganites were synthesized and characterized using different techniques. In the series, both the bulk and nanostructured La0.7Sr0.10Ca0.20MnO3 and La0.7Sr0.20Ca0.10MnO3 manganites have orthorhombic and rhombohedral stru...
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Veröffentlicht in: | 稀有金属:英文版 2017 (6), p.501-511 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Series of bulk and nanostructured La0.7SrxCa0.3-xMnO3(x = 0.10, 0.15, and 0.20) manganites were synthesized and characterized using different techniques. In the series, both the bulk and nanostructured La0.7Sr0.10Ca0.20MnO3 and La0.7Sr0.20Ca0.10MnO3 manganites have orthorhombic and rhombohedral structures, whereas La0.7Sr0.15Ca0.15MnO3 manganite has rhombohedral and orthorhombic structures, respectively. Online ultrasonic velocity and attenuation measurements were taken through an indigenously designed ultrasonic setup, and the analysis was done from 300 to 400 K during the aging of the samples to explore the structural/phase transitions. The bulk and nanocrystalline La0.7SrxCa0.3-xMnO3 perovskite samples show the particle size distribution in the range of 197–943 and 24–93 nm, respectively. The addition of Sr2+ alters the size of particles, which decrease in size. The observed anomaly in ultrasonic velocities, attenuations, and elastic moduli is correlated with the ferromagnetic–paramagnetic(FM–PM) transition temperature(TC) in both bulk and nanocrystalline perovskites. In addition, the shift in TC and the magnitude and width of observed anomaly are correlated with the value of x to study the behavior of TC. |
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ISSN: | 1001-0521 1867-7185 |