dc.contributor0000-0001-5324-1834
dc.contributor0000-0002-1478-7946
dc.creatorChubykalo, Andrew
dc.creatorEspinoza, Augusto
dc.creatorKosyakov, Boris Pavlovich
dc.date.accessioned2018-06-11T19:14:17Z
dc.date.accessioned2022-10-14T15:13:49Z
dc.date.available2018-06-11T19:14:17Z
dc.date.available2022-10-14T15:13:49Z
dc.date.created2018-06-11T19:14:17Z
dc.date.issued2011-12
dc.identifier1286-4854
dc.identifier0295-5075
dc.identifierhttp://hdl.handle.net/20.500.11845/523
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4247238
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.
dc.languageeng
dc.publisherThe European Physical Society (EPS)
dc.relationgeneralPublic
dc.relationhttp://iopscience.iop.org/journal/0295-5075
dc.rightshttp://creativecommons.org/licenses/by-nc-sa/3.0/us/
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América
dc.sourceEPL Journal, Núm. 96, Diciembre 2011.
dc.titleNo-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worlds
dc.typeArtículos de revistas


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