Magnetic and transport properties of polycrystalline La0.7Sr0.3Mn1-xFexO3

dc.contributor.authorAraújo, José Humberto de
dc.contributor.authorFeitosa, Carlos Chesman de Araújo
dc.contributor.authorDumelow, T.
dc.contributor.authorXavier Jr, M. M.
dc.contributor.authorCabral, F. A. O.
dc.date.accessioned2020-05-14T13:51:01Z
dc.date.available2020-05-14T13:51:01Z
dc.date.issued2000-12-12
dc.description.abstractThe effect of Fe doping (<10%) on polycrystalline samples of La0.7Sr0.3MnO3 has been studied by means of x-ray diffraction, resistivity, ac susceptibility, magnetization, and magnetoresistance measurements. Fe doping does not affect the lattice structure, but it weakens the ferromagnetism and substantially augments the resistivity of the samples. The magnetoresistance of a sample with 10% Fe doping, in a 5 T magnetic field, was 4 times greater than that of the undoped sample near the peak in the resistivity. The results were explained in terms of the formation of antiferromagnetic clusters of Fe ions. At 5 K the magnetoresistance showed no significant dependence on Fe doping, but it displayed large variations in fields below 0.5 T for all samples. This behavior was attributed to spin-polarized tunneling at the grain boundaries of the polycrystalline samples. A variable-range hopping behavior in the resistivity was also encountered in all the samples at low temperatures.pt_BR
dc.description.resumoThe effect of Fe doping (<10%) on polycrystalline samples of La0.7Sr0.3MnO3 has been studied by means of x-ray diffraction, resistivity, ac susceptibility, magnetization, and magnetoresistance measurements. Fe doping does not affect the lattice structure, but it weakens the ferromagnetism and substantially augments the resistivity of the samples. The magnetoresistance of a sample with 10% Fe doping, in a 5 T magnetic field, was 4 times greater than that of the undoped sample near the peak in the resistivity. The results were explained in terms of the formation of antiferromagnetic clusters of Fe ions. At 5 K the magnetoresistance showed no significant dependence on Fe doping, but it displayed large variations in fields below 0.5 T for all samples. This behavior was attributed to spin-polarized tunneling at the grain boundaries of the polycrystalline samples. A variable-range hopping behavior in the resistivity was also encountered in all the samples at low temperatures.pt_BR
dc.identifier.citationARAUJO, José Humberto de et al. Magnetic and transport properties of polycrystalline La0.7Sr0.3Mn1¿xFexO3. Physical Review. B: Condensed Matter and Materials Physics, v. 63, p. 12408-12411, 2000. ISSN 2469-9969 versão online. DOI https://doi.org/10.1103/PhysRevB.63.012408. Disponivel em: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.63.012408. Acesso em: 14 maio 2020.pt_BR
dc.identifier.doi10.1103/PhysRevB.63.012408
dc.identifier.issn2469-9969 (online), 2469-9950 (print).
dc.identifier.urihttps://repositorio.ufrn.br/jspui/handle/123456789/28978
dc.languageenpt_BR
dc.publisherAmerican Physical Societypt_BR
dc.subjectMagneticpt_BR
dc.subjectTransportpt_BR
dc.subjectPropertiespt_BR
dc.subjectPolycrystallinept_BR
dc.titleMagnetic and transport properties of polycrystalline La0.7Sr0.3Mn1-xFexO3pt_BR
dc.typearticlept_BR

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