dc.creator
dc.creator
dc.creatorAndrew Chubykalo
dc.creator
dc.date2013
dc.date.accessioned2022-10-12T19:49:24Z
dc.date.available2022-10-12T19:49:24Z
dc.identifier2326-8867
dc.identifier2326-8891
dc.identifierhttp://hdl.handle.net/20.500.11845/539
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4122772
dc.descriptionIn 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.descriptionProducción Científica de la Universidad Autónoma de Zacatecas UAZ
dc.formatapplication/pdf
dc.languagespa
dc.rightsinfo:eu-repo/semantics/openAccess
dc.rightshttp://creativecommons.org/licenses/by-nc-nd/4.0
dc.subjectinfo:eu-repo/classification/cti/1
dc.subjectelectromagnetic potentials
dc.titleGauge Symmetries and gauge trnasformations for Maxwell Equations
dc.typeinfo:eu-repo/semantics/article
dc.audiencegeneralPublic


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