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 La 0.7 Sr x Ca 0.3− x MnO 3 ( x  = 0.10, 0.15, and 0.20) manganites were synthesized and characterized using different techniques. In the series, both the bulk and nanostructured La 0.7 Sr 0.10 Ca 0.20 MnO 3 and La 0.7 Sr 0.20 Ca 0.10 MnO 3 manganites have orthorhom...

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Veröffentlicht in:Rare metals 2017-06, Vol.36 (6), p.501-511
Hauptverfasser: Praveen Kumar, Somasundaram, Sakthipandi, Kathiresan, Gayathiri, Ramamurthy, Sridhar Panday, Mathu, Karthik, Arumugam, Rajendran, Venkatachalam
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Sprache:eng
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Zusammenfassung:Series of bulk and nanostructured La 0.7 Sr x Ca 0.3− x MnO 3 ( x  = 0.10, 0.15, and 0.20) manganites were synthesized and characterized using different techniques. In the series, both the bulk and nanostructured La 0.7 Sr 0.10 Ca 0.20 MnO 3 and La 0.7 Sr 0.20 Ca 0.10 MnO 3 manganites have orthorhombic and rhombohedral structures, whereas La 0.7 Sr 0.15 Ca 0.15 MnO 3 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 La 0.7 Sr x Ca 0.3− x MnO 3 perovskite samples show the particle size distribution in the range of 197–943 and 24–93 nm, respectively. The addition of Sr 2+ 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 ( T C ) in both bulk and nanocrystalline perovskites. In addition, the shift in T C and the magnitude and width of observed anomaly are correlated with the value of x to study the behavior of T C .
ISSN:1001-0521
1867-7185
DOI:10.1007/s12598-015-0516-3