Please use this identifier to cite or link to this item: https://ri.ufs.br/jspui/handle/riufs/474
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dc.contributor.authorSouza, André Maurício Conceição de-
dc.contributor.authorHerrmann, Hans Jürgen-
dc.contributor.authorMaionchi, Daniela de Oliveira-
dc.date.accessioned2013-04-18T21:23:37Z-
dc.date.available2013-04-18T21:23:37Z-
dc.date.issued2007-07-
dc.identifier.citationSOUZA, A. M. C.; HERRMANN, H. J.; MAIOINCHI, D. O. Hölder mean applied to Anderson localization. Physical Review B, New York, v. 76, n. 3, jul. 2007. Disponível em: <http://link.aps.org/doi/10.1103/PhysRevB.76.035111>. Acesso em: 18 abr. 2013.pt_BR
dc.identifier.issn1550-235X-
dc.identifier.urihttps://ri.ufs.br/handle/riufs/474-
dc.description.abstractThe phase diagram of correlated, disordered electron systems is calculated within dynamical mean-field theory using the Hölder mean local density of states. A critical disorder strength is determined in the Anderson-Falicov-Kimball model, and the arithmetic and the geometric averages are found to be just particular means used, respectively, to detect or not the Anderson localization. Correlated metal, Mott insulator, and Anderson insulator phases, as well as coexistence and crossover regimes, are analyzed in this perspective.pt_BR
dc.language.isoenpt_BR
dc.publisherAmerican Physical Societypt_BR
dc.subjectLocalização de Andersonpt_BR
dc.subjectModelo de Falicov-Kimballpt_BR
dc.titleHölder mean applied to Anderson localizationpt_BR
dc.typeArtigopt_BR
dc.identifier.license© 2007 The American Physical Societypt_BR
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