2011
DOI: 10.1016/j.jmmm.2011.05.050
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Magnetic dynamics of charge ordered Nd0.80Na0.20MnO3 compound

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Cited by 7 publications
(2 citation statements)
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“…This large bifurcation is a signature of magnetic anisotropy in the compound arising from competing weak ferromagnetic and anti-ferromagnetic behavior and presence of spin glass like phase. 35,47 Structural anisotropy also may be a reason of magnetic anisotropy. This gure also shows that ICAFM and c-AFM regions are divided by a peak.…”
Section: Magnetic Properties Of Undoped and Na-doped Gdmno 3 Compoundsmentioning
confidence: 99%
“…This large bifurcation is a signature of magnetic anisotropy in the compound arising from competing weak ferromagnetic and anti-ferromagnetic behavior and presence of spin glass like phase. 35,47 Structural anisotropy also may be a reason of magnetic anisotropy. This gure also shows that ICAFM and c-AFM regions are divided by a peak.…”
Section: Magnetic Properties Of Undoped and Na-doped Gdmno 3 Compoundsmentioning
confidence: 99%
“…15 However, the in depth structural characterization and study of the monovalent cation doping effect on octahedral distortion were not addressed previously. [24][25][26][27][28] NdMnO 3 shows a paramagnetic to antiferromagnetic phase transition with Neel temperature at 67 K. 29 On the other hand, both 15 mol% Na-and K-doped NdMnO 3 compounds show paramagnetic to ferromagnetic phase transitions with a Curie temperature at ∼100 K. [25][26][27][28][29] In this article emphasis is given on the following aspects: (i) detailed crystal structures, microstructures and lattice distortions in these three compounds due to monovalent doping, (ii) the effect of sintering temperature on the formation of these compounds and (iii) temperature dependent magnetization to elucidate the effect of monovalent doping on the magnetic properties of NdMnO 3 .…”
Section: Introductionmentioning
confidence: 99%