dc.contributorhttps://orcid.org/0000-0002-1478-7946
dc.contributorhttps://orcid.org/0000-0001-5324-1834
dc.creatorEspinoza, Augusto
dc.creatorChubykalo, Andrew
dc.creatorPerez Carlos, David
dc.date.accessioned2018-06-12T16:29:21Z
dc.date.available2018-06-12T16:29:21Z
dc.date.created2018-06-12T16:29:21Z
dc.date.issued2016-09
dc.identifier2153-120X
dc.identifier2153-1196
dc.identifierhttp://hdl.handle.net/20.500.11845/537
dc.identifierhttps://doi.org/10.48779/rfdk-vr73
dc.description.abstractIn the Jefimenko’s generalized theory of gravitation, it is proposed the existence of certain potentials to help us to calculate the gravitational and cogravitational fields, such potentials are also presumed non-invariant under certain gauge transformations. In return, we propose that there is a way to perform the calculation of certain potentials that can be derived without using some kind of gauge transformation, and to achieve this we apply the Helmholtz’s theorem. This procedure leads to the conclusion that both gravitational and cogravitational fields propagate simultaneously in a delayed and in an instant manner. On the other hand, it is also concluded that these potentials thus obtained can be real physical quantities, unlike potentials obtained by Jefimenko, which are only used as a mathematical tool for calculating gravitational and cogravitational fields.
dc.languageeng
dc.publisherScientific Research Publishing
dc.relationgeneralPublic
dc.relationhttps://www.scirp.org/journal/jmp/
dc.rightshttp://creativecommons.org/licenses/by-nc-sa/3.0/us/
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América
dc.sourceJournal of Modern Physics, Núm. 7, Septiembre 2016.
dc.titleGauge Invariance of Gravitodynamical Potentials in the Jefimenko’s Generalized Theory of Gravitation
dc.typeinfo:eu-repo/semantics/article


Este ítem pertenece a la siguiente institución