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 |
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Hauptverfasser: | , , , , , |
Format: | Artikel |
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
. |
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ISSN: | 1001-0521 1867-7185 |
DOI: | 10.1007/s12598-015-0516-3 |