Please use this identifier to cite or link to this item: http://ricaxcan.uaz.edu.mx/jspui/handle/20.500.11845/523
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dc.contributor.otherhttps://orcid.org/0000-0001-5324-1834es_ES
dc.contributor.otherhttps://orcid.org/0000-0002-1478-7946es_ES
dc.coverage.spatialGlobales_ES
dc.creatorChubykalo, Andrew-
dc.creatorEspinoza, Augusto-
dc.creatorKosyakov, Boris Pavlovich-
dc.date.accessioned2018-06-11T19:14:17Z-
dc.date.available2018-06-11T19:14:17Z-
dc.date.issued2011-12-
dc.identifierinfo:eu-repo/semantics/publishedVersiones_ES
dc.identifier.issn1286-4854es_ES
dc.identifier.issn0295-5075es_ES
dc.identifier.urihttp://hdl.handle.net/20.500.11845/523-
dc.identifier.urihttps://doi.org/10.48779/9y1s-6t06-
dc.description.abstractIf the conventional Maxwell-Lorentz formulation of classical electrodynamics is adopted in a flat spacetime of arbitrary odd dimension, then the retarded vector potential Aμ generated by a point charge turns out to be pure gauge, Aμ = μ . By Gauss’ law, the charge shows up as zero. The classical electromagnetic coupling is thus missing from odd-dimensional worlds. If the action is augmented by the addition of the Chern-Simons term, then the classical interaction picture in the three-dimensional world becomes nontrivial.es_ES
dc.language.isoenges_ES
dc.publisherThe European Physical Society (EPS)es_ES
dc.relationhttp://iopscience.iop.org/journal/0295-5075es_ES
dc.relation.urigeneralPublices_ES
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/3.0/us/*
dc.sourceEPL Journal, Núm. 96, Diciembre 2011.es_ES
dc.subject.classificationCIENCIAS FISICO MATEMATICAS Y CIENCIAS DE LA TIERRA [1]es_ES
dc.subject.otherClassical electromagnetismes_ES
dc.subject.otherMaxwell equationses_ES
dc.subject.otherField theories in dimensions other than foures_ES
dc.titleNo-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worldses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
Appears in Collections:*Documentos Académicos*-- UA Física

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