Use este identificador para citar ou linkar para este item: https://repositorio.ufba.br/handle/ri/6506
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dc.contributor.authorQueiroz, H.-
dc.contributor.authorSilva, J. C. da-
dc.contributor.authorKhanna, Faqir C.-
dc.contributor.authorMalbouisson, J. M. C.-
dc.contributor.authorRevzen, M.-
dc.contributor.authorSantana, Ademir Eugênio de-
dc.creatorQueiroz, H.-
dc.creatorSilva, J. C. da-
dc.creatorKhanna, Faqir C.-
dc.creatorMalbouisson, J. M. C.-
dc.creatorRevzen, M.-
dc.creatorSantana, Ademir Eugênio de-
dc.date.accessioned2012-07-30T19:05:05Z-
dc.date.issued2005-05-
dc.identifier.issn0003-4916-
dc.identifier.urihttp://www.repositorio.ufba.br/ri/handle/ri/6506-
dc.descriptionTrabalho completo: acesso restrito, p. 220–237pt_BR
dc.description.abstractA generalization of the Bogoliubov transformation is developed to describe a space compactified fermionic field. The method is the fermionic counterpart of the formalism introduced earlier for bosons [Phys. Rev. A 66 (2002) 052101], and is based on the thermofield dynamics approach. We analyze the energy–momentum tensor for the Casimir effect of a free massless fermion field in a d-dimensional box at finite temperature. As a particular case the Casimir energy and pressure for the field confined in a three-dimensional parallelepiped box are calculated. It is found that the attractive or repulsive nature of the Casimir pressure on opposite faces changes depending on the relative magnitude of the edges. We also determine the temperature at which the Casimir pressure in a cubic box changes sign and estimate its value when the edge of the cube is of the order of the confining lengths for baryons.pt_BR
dc.language.isoenpt_BR
dc.publisherElsevierpt_BR
dc.sourcehttp://dx.doi.org/10.1016/j.aop.2004.11.011pt_BR
dc.subjectFermionic Casimir effectpt_BR
dc.subjectFinite temperaturept_BR
dc.titleThermofield dynamics and Casimir effect for fermionspt_BR
dc.title.alternativeAnnals of Physicspt_BR
dc.typeArtigo de Periódicopt_BR
dc.identifier.numberv. 317, n. 1pt_BR
dc.embargo.liftdate10000-01-01-
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