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Magnetic and magnetotransport behavior of overdoped nanocrystalline Nd_(1-x)Sr_xMnO_3 (0.50≤x≤0.63) 被引量:1

Magnetic and magnetotransport behavior of overdoped nanocrystalline Nd_(1-x)Sr_xMnO_3 (0.50≤x≤0.63)
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摘要 The nanocrystalline samples of Nd1-xSrxMnO3 (NSMO) (x=0.5, 0.55, 0.60, 0.63) were synthesized by sol-gel based polymeric pre-cursor route. Structural, magnetic and magnetotransport properties were studied systematically. It was found that in the composition range (x=0.50-0.63), Nd1-xSrxMnO3 showed paramagnetic to ferromagnetic (PM-FM) transition in the vicinity of TC~270 K but the FM phase was weakened as the Sr concentration increased. The appearance of weak ferromagnetism was explained in terms of the core-shell model. More-over, for x=0.63 sample, a second transition is observed below TC at T=185 K, which is possibly due to the appearance of A-AFM/ C-AFM or a mixture of both the phases. Resistivity vs temperature (ρ-T) curve showed that the resistivity of all the samples was much larger than the sin-gle crystals of corresponding compositions due to large contribution of the grain boundaries in the present nanocrystalline samples. In all samples, extrinsic kind of MR behavior dominated because of nanocrystalline nature of the samples, which was nearly of the same order (~10%) in all samples. However, the intrinsic kind of MR behavior was also significant in x=0.50 sample, because of the strongest FM feature in this sample. The nanocrystalline samples of Nd1-xSrxMnO3 (NSMO) (x=0.5, 0.55, 0.60, 0.63) were synthesized by sol-gel based polymeric pre-cursor route. Structural, magnetic and magnetotransport properties were studied systematically. It was found that in the composition range (x=0.50-0.63), Nd1-xSrxMnO3 showed paramagnetic to ferromagnetic (PM-FM) transition in the vicinity of TC~270 K but the FM phase was weakened as the Sr concentration increased. The appearance of weak ferromagnetism was explained in terms of the core-shell model. More-over, for x=0.63 sample, a second transition is observed below TC at T=185 K, which is possibly due to the appearance of A-AFM/ C-AFM or a mixture of both the phases. Resistivity vs temperature (ρ-T) curve showed that the resistivity of all the samples was much larger than the sin-gle crystals of corresponding compositions due to large contribution of the grain boundaries in the present nanocrystalline samples. In all samples, extrinsic kind of MR behavior dominated because of nanocrystalline nature of the samples, which was nearly of the same order (~10%) in all samples. However, the intrinsic kind of MR behavior was also significant in x=0.50 sample, because of the strongest FM feature in this sample.
出处 《Journal of Rare Earths》 SCIE EI CAS CSCD 2011年第7期654-659,共6页 稀土学报(英文版)
关键词 MANGANITES MAGNETORESISTANCE spin polarized tunnelling rare earths manganites magnetoresistance spin polarized tunnelling rare earths
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