Gravitation without the equivalence principle

dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorAldrovandi, R.
dc.creatorPereira, J. G.
dc.creatorVu, K. H.
dc.date2014-05-20T14:07:44Z
dc.date2016-10-25T17:12:59Z
dc.date2014-05-20T14:07:44Z
dc.date2016-10-25T17:12:59Z
dc.date2004-01-01
dc.date.accessioned2017-04-05T21:42:36Z
dc.date.available2017-04-05T21:42:36Z
dc.identifierGeneral Relativity and Gravitation. New York: Kluwer Academic/plenum Publ, v. 36, n. 1, p. 101-110, 2004.
dc.identifier0001-7701
dc.identifierhttp://hdl.handle.net/11449/23789
dc.identifierhttp://acervodigital.unesp.br/handle/11449/23789
dc.identifier10.1023/B:GERG.0000006696.98824.4d
dc.identifierWOS:000186983100006
dc.identifierhttp://dx.doi.org/10.1023/B:GERG.0000006696.98824.4d
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/868832
dc.descriptionIn the general relativistic description of gravitation, geometry replaces the concept of force. This is possible because of the universal character of free fall, and would break down in its absence. on the other hand, the teleparallel version of general relativity is a gauge theory for the translation group and, as such, describes the gravitational interaction by a force similar to the Lorentz force of electromagnetism, a non-universal interaction. Relying on this analogy it is shown that, although the geometric description of general relativity necessarily requires the existence of the equivalence principle, the teleparallel gauge approach remains a consistent theory for gravitation in its absence.
dc.languageeng
dc.publisherKluwer Academic/plenum Publ
dc.relationGeneral Relativity and Gravitation
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subjectgravitation
dc.subjectteleparallelism
dc.subjectequivalence principle
dc.titleGravitation without the equivalence principle
dc.typeOtro


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