dc.contributor0000-0001-5324-1834
dc.contributor0000-0002-1478-7946
dc.creatorChubykalo, Andrew
dc.creatorEspinoza, Augusto
dc.creatorAlvarado Flores, Rolando
dc.date.accessioned2018-06-12T16:29:38Z
dc.date.accessioned2022-10-14T15:15:01Z
dc.date.available2018-06-12T16:29:38Z
dc.date.available2022-10-14T15:15:01Z
dc.date.created2018-06-12T16:29:38Z
dc.date.issued2013
dc.identifier2326-8867
dc.identifier2326-8891
dc.identifierhttp://hdl.handle.net/20.500.11845/539
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4247883
dc.description.abstractIn a previous publication [5] we introduced gauge invariant electromagnetic potentials. However the field equations that were derived for them turn out to be the Coulomb gauge field equations. This raises the question of the nature of these new gauge invariant potentials and its relations with Coulomb gauge potentials. In this paper we prove that this new potentials are in fact gauge invariant and identical with the Coulomb gauge potentials. In other words: the Coulomb gauge potentials are gauge invariant potentials that cannot be related to Lorenz gauge potentials because, contrary to current ideas, there is not anything like a gauge transformation relating both gauges.
dc.languagespa
dc.publisherSciencie Publishing Group
dc.publisherCoulomb gauge potentials
dc.publisherMaxwell equations
dc.relationgeneralPublic
dc.relationhttp://www.sciencepublishinggroup.com/journal/index?journalid=122
dc.rightshttp://creativecommons.org/licenses/by-nc-sa/3.0/us/
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América
dc.sourceAmerican Journal of Modern Physics, Vol. 4, Núm 1 y 2, 2013.
dc.titleGauge Symmetries and gauge trnasformations for Maxwell Equations
dc.typeArtículos de revistas


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