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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/76417
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dc.contributor.authorAparicio Alcalde, M.-
dc.contributor.authorPimentel, B. M.-
dc.date.accessioned2014-05-27T11:30:32Z-
dc.date.accessioned2016-10-25T18:53:11Z-
dc.date.available2014-05-27T11:30:32Z-
dc.date.available2016-10-25T18:53:11Z-
dc.date.issued2013-09-01-
dc.identifierhttp://dx.doi.org/10.1016/j.physa.2013.04.003-
dc.identifier.citationPhysica A: Statistical Mechanics and its Applications, v. 392, n. 17, p. 3765-3779, 2013.-
dc.identifier.issn0378-4371-
dc.identifier.urihttp://hdl.handle.net/11449/76417-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/76417-
dc.description.abstractIn this work we study two different spin-boson models. Such models are generalizations of the Dicke model, it means they describe systems of N identical two-level atoms coupled to a single-mode quantized bosonic field, assuming the rotating wave approximation. In the first model, we consider the wavelength of the bosonic field to be of the order of the linear dimension of the material composed of the atoms, therefore we consider the spatial sinusoidal form of the bosonic field. The second model is the Thompson model, where we consider the presence of phonons in the material composed of the atoms. We study finite temperature properties of the models using the path integral approach and functional methods. In the thermodynamic limit, N→∞, the systems exhibit phase transitions from normal to superradiant phase at some critical values of temperature and coupling constant. We find the asymptotic behavior of the partition functions and the collective spectrums of the systems in the normal and the superradiant phases. We observe that the collective spectrums have zero energy values in the superradiant phases, corresponding to the Goldstone mode associated to the continuous symmetry breaking of the models. Our analysis and results are valid in the limit of zero temperature β→∞, where the models exhibit quantum phase transitions. © 2013 Elsevier B.V. All rights reserved.en
dc.format.extent3765-3779-
dc.language.isoeng-
dc.sourceScopus-
dc.subjectCollective excitations-
dc.subjectDicke model-
dc.subjectQuantum phase transition-
dc.subjectAsymptotic behaviors-
dc.subjectPath integral approach-
dc.subjectQuantum phase transitions-
dc.subjectRotating wave approximations-
dc.subjectThermal phase transition-
dc.subjectThermodynamic limits-
dc.subjectPhase transitions-
dc.subjectQuantum optics-
dc.subjectFerroelectric materials-
dc.titleThermal phase transition for some spin-boson modelsen
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationInstituto de Física Teórica UNESP - São Paulo State University, Caixa Postal 70532-2, 01156-970 São Paulo, SP-
dc.description.affiliationUnespInstituto de Física Teórica UNESP - São Paulo State University, Caixa Postal 70532-2, 01156-970 São Paulo, SP-
dc.identifier.doi10.1016/j.physa.2013.04.003-
dc.identifier.wosWOS:000320488800029-
dc.rights.accessRightsAcesso restrito-
dc.relation.ispartofPhysica A: Statistical Mechanics and Its Applications-
dc.identifier.scopus2-s2.0-84878397320-
Appears in Collections:Artigos, TCCs, Teses e Dissertações da Unesp

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