dc.creator | | |
dc.creator | | |
dc.creator | Andrew Chubykalo | |
dc.creator | | |
dc.date | 2013 | |
dc.date.accessioned | 2022-10-12T19:49:24Z | |
dc.date.available | 2022-10-12T19:49:24Z | |
dc.identifier | 2326-8867 | |
dc.identifier | 2326-8891 | |
dc.identifier | http://hdl.handle.net/20.500.11845/539 | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/4122772 | |
dc.description | In 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.description | Producción Científica de la Universidad Autónoma de Zacatecas UAZ | |
dc.format | application/pdf | |
dc.language | spa | |
dc.rights | info:eu-repo/semantics/openAccess | |
dc.rights | http://creativecommons.org/licenses/by-nc-nd/4.0 | |
dc.subject | info:eu-repo/classification/cti/1 | |
dc.subject | electromagnetic potentials | |
dc.title | Gauge Symmetries and gauge trnasformations for Maxwell Equations | |
dc.type | info:eu-repo/semantics/article | |
dc.audience | generalPublic | |