Use este identificador para citar ou linkar para este item: https://ri.ufs.br/jspui/handle/riufs/21917
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dc.contributor.authorSouza, Andre Mauricio Conceicao de-
dc.contributor.authorRodríguez-Pérez, Sergio-
dc.contributor.authorMacêdo, Antonio Murilo Santos-
dc.date.accessioned2025-05-07T15:18:29Z-
dc.date.available2025-05-07T15:18:29Z-
dc.date.issued2010-
dc.identifier.citationSOUZA, A. M. C.; RODRÍGUEZ-PÉREZ, S.; MACÊDO, A. M. S. Transport observables for a FNF mesoscopic system in the extreme quantum limit regime. Journal of Physics: Conference Series, v. 200, 2010. Seção 5. Trabalho apresentado em 18º International Conference on Magnetism, 2009, [Karlsruhe]. Disponível em: https://iopscience.iop.org/article/10.1088/1742-6596/200/5/052027/pdf. Acesso em: 7 maio 2025.pt_BR
dc.identifier.issn1742-6596-
dc.identifier.issn1742-6588-
dc.identifier.urihttps://ri.ufs.br/jspui/handle/riufs/21917-
dc.languageengpt_BR
dc.publisherIOP Publishingpt_BR
dc.relation.ispartofJournal of Physics: Conference Seriespt_BR
dc.subjectFerromagnet/normal-metal/ferromagnet (FNF)eng
dc.titleTransport observables for a FNF mesoscopic system in the extreme quantum limit regimept_BR
dc.typeTrabalhos em Eventospt_BR
dc.identifier.licenseCreative Commons Atribuição 4.0 Internacional (CC BY 4.0)pt_BR
dc.description.resumoWe study the current-induced torque for electrons on ferromagnet-normal metalferromagnet (FNF) trilayer with non-collinear magnetizations. Our system is composed of a chaotic cavity and two junctions, coupled with ideal contacts to ferromagnetic reservatories in local equilibrium by means of a small number of scattering channels. We assume that the normal part is disordered. Each junction is related to the direction of the reservoirs magnetization. The system is taken out of equilibrium causing a spin accumulation. We suppose that all elements have a length smaller than the coherence phase and the spin flip lengths. This consideration lets us neglect decoherence and spin flip processes. The conductance and torque were found numerically by employing the random-matrix theory and scattering matrix formalism for the spin-flux. The observables are presented as a function of the number of propagating channels in the extreme quantum limit regime and of the angle between the magnetizations of the different ferromagnet layers.pt_BR
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