dc.creatorSouza, André Maurício Conceição de
dc.creatorMacedo, Antônio Murilo Santos
dc.date2013-03-18T23:48:07Z
dc.date2013-03-18T23:48:07Z
dc.date2005-06
dc.date.accessioned2023-09-28T22:44:00Z
dc.date.available2023-09-28T22:44:00Z
dc.identifierSOUZA, A. M. C.; MACÊDO, A. M. S. Formation of Fabry-Perot resonances in double-barrier chaotic billiards. Physical Review E, New York, v. 71, n. 6, jun. 2005. Disponível em: <http://link.aps.org/doi/10.1103/PhysRevE.71.066218>. Acesso em: 18 mar. 2013.
dc.identifier1550-2376
dc.identifierhttp://link.aps.org/doi/10.1103/PhysRevE.71.066218
dc.identifierhttps://ri.ufs.br/handle/riufs/463
dc.identifierCopyrights American Physical Society
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/9076567
dc.descriptionWe study wave transport through a chaotic quantum billiard attached to two waveguides via barriers of arbitrary transparencies in the semiclassical limit of a large number of open scattering channels. We focus attention on the ergodic regime, which is described by using a random-matrix approach to chaotic resonance scattering together with an extended version of Nazarov’s circuit theory. By varying the relative strength of the barriers’ transparencies a reorganization of the relevant resonances in the energy interval where transport takes place leads to a full suppression of high transmission modes. We provide a detailed quantitative description of the process by means of both numerical and analytical evaluations of the average density of transmission eigenvalues. We show that the density of Fabry-Perot modes can be used as a kind of order parameter for this quantum transition. A diagram is presented as a function of the transparencies of the barriers exhibiting the transport regimes and the transition lines.
dc.formatapplication/pdf
dc.languageen
dc.publisherAmerican Physical Society
dc.subjectinterferômetro Fabry-Perot
dc.subjectTransporte de ondas
dc.titleFormation of Fabry-Perot resonances in double-barrier chaotic billiards
dc.typeArtigo


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