dc.creatorSouza, André Maurício Conceição de
dc.creatorHerrmann, Hans Jürgen
dc.creatorMaionchi, Daniela de Oliveira
dc.date2013-04-18T21:23:37Z
dc.date2013-04-18T21:23:37Z
dc.date2007-07
dc.date.accessioned2023-09-28T22:55:14Z
dc.date.available2023-09-28T22:55:14Z
dc.identifierSOUZA, 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.
dc.identifier1550-235X
dc.identifierhttps://ri.ufs.br/handle/riufs/474
dc.identifier© 2007 The American Physical Society
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/9080568
dc.descriptionThe 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.
dc.formatapplication/pdf
dc.languageen
dc.publisherAmerican Physical Society
dc.subjectLocalização de Anderson
dc.subjectModelo de Falicov-Kimball
dc.titleHölder mean applied to Anderson localization
dc.typeArtigo


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