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Weyl-invariant Kaluza-Klein theory and the teleparallel equivalent of Weyl-invariant general relativity

dc.citation.epage0en_US
dc.citation.issue6en_US
dc.citation.spage0en_US
dc.citation.volume88en_US
dc.citation.woscount2en_US
dc.contributor.authorChang, ChiaMingen_US
dc.contributor.authorKao, W. F.en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.date.accessioned2019-04-03T06:43:38Z
dc.date.available2019-04-03T06:43:38Z
dc.date.issued2013-09-03en_US
dc.description.abstractA simple method is shown to demonstrate that the teleparallel equivalent of general relativity can be generalized to the Weyl-invariant models. We will also show explicitly that Weyl symmetry is preserved step by step throughout the 5D Kaluza-Klein dimensional-reduction process. As a result, the dimensional reduced model will be shown to be a theory with two scalar fields. When a symmetry-breaking potential is introduced, a strong constraint will effectively turn off one of the scalar fields. For heuristic reasons, the stability properties of the power-law solution associated with the resulting one-scalar-field model will be presented explicitly. In particular, all stable modes can be solved explicitly as functions of the free parameter associated with the symmetry-breaking potential.en_US
dc.identifier.doi10.1103/PhysRevD.88.063504en_US
dc.identifier.issn2470-0010en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.88.063504en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/22517
dc.identifier.wosnumberWOS:000323894000008en_US
dc.language.isoen_USen_US
dc.titleWeyl-invariant Kaluza-Klein theory and the teleparallel equivalent of Weyl-invariant general relativityen_US
dc.typeArticleen_US

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