Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/2583
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dc.contributor.authorNieves, Jose. F-
dc.contributor.authorPalash, B. Pal-
dc.date.accessioned2008-07-09T07:25:16Z-
dc.date.available2008-07-09T07:25:16Z-
dc.date.issued1995-05-
dc.identifier.citationPhysical Review D, Vol. 51, No. 9, pp. 5300 - 5304en
dc.identifier.issn0556-2821-
dc.identifier.urihttp://hdl.handle.net/2248/2583-
dc.description.abstractIn general the zero momentum limit of thermal self-energies calculated in perturbation theory depends on the order in which the time and the space components of the momentum are taken to zero. We show that this is an artifact of the perturbative calculation, and in fact the nonanalyticity of the one-loop self-energy disappears when it is calculated with improved vertices and/or improved propagators that incorporate the imaginary part of the self-energyen
dc.format.extent782221 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherThe American Physical Societyen
dc.relation.urihttp://prola.aps.org/abstract/PRD/v51/i9/p5300_1en
dc.subjectThermal self-energiesen
dc.subjectZero momentumen
dc.subjectPerturbation Theoryen
dc.subjectModels-Thermal self-energies at Zero momentumen
dc.subjectThermal field theoryen
dc.titleThermal self-energies at zero momentumen
dc.typeArticleen
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