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.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.accessioned2022-10-07T15:37:02Z
dc.date.available2022-10-07T15:37:02Z
dc.date.issued2005-05
dc.identifier0003-4916
dc.identifierhttp://www.repositorio.ufba.br/ri/handle/ri/6506
dc.identifierv. 317, n. 1
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/4005423
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.
dc.languageen
dc.publisherElsevier
dc.sourcehttp://dx.doi.org/10.1016/j.aop.2004.11.011
dc.subjectFermionic Casimir effect
dc.subjectFinite temperature
dc.titleThermofield dynamics and Casimir effect for fermions
dc.typeArtigo de Periódico


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