Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/81243
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dc.contributor.authorKizilersu, A.-
dc.contributor.authorSizer, T.-
dc.contributor.authorWilliams, A.-
dc.date.issued2013-
dc.identifier.citationPhysical Review D: Particles, Fields, Gravitation and Cosmology, 2013; 88(4):1-48-
dc.identifier.issn1550-7998-
dc.identifier.issn1550-2368-
dc.identifier.urihttp://hdl.handle.net/2440/81243-
dc.description.abstractWe study unquenched QED in four dimensions using renormalized Schwinger-Dyson equations and focus on the behaviour of the fermion and photon propagators. For this purpose we use an improved Kızılersü-Pennington (KP) vertex which respects gauge invariance, multiplicative renormalizability for the massless case, agrees with perturbation theory in the weak coupling regime, and is free of kinematic singularities. We find that the KP vertex performs very well as expected especially in comparison with other vertex choices. We find that the Landau pole problem familiar from perturbative QED persists in the nonperturbative case with the renormalized inverse photon propagator having zero crossing.-
dc.description.statementofresponsibilityAyşe Kızılersü, Tom Sizer, and Anthony G. Williams-
dc.language.isoen-
dc.publisherAmerican Physical Society-
dc.rights© 2013 American Physical Society-
dc.source.urihttp://dx.doi.org/10.1103/physrevd.88.045008-
dc.titleStrongly-coupled unquenched QED₄ propagators using Schwinger-Dyson equations-
dc.title.alternativeStrongly-coupled unquenched QED(4) propagators using Schwinger-Dyson equations-
dc.typeJournal article-
dc.identifier.doi10.1103/PhysRevD.88.045008-
dc.relation.granthttp://purl.org/au-research/grants/arc/DP0558878-
dc.relation.granthttp://purl.org/au-research/grants/arc/LX0776452-
pubs.publication-statusPublished-
dc.identifier.orcidKizilersu, A. [0000-0003-2096-8900]-
dc.identifier.orcidWilliams, A. [0000-0002-1472-1592]-
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Chemistry and Physics publications

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