Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/4042
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dc.contributor.authorSivaram, C-
dc.date.accessioned2008-12-02T14:09:48Z-
dc.date.available2008-12-02T14:09:48Z-
dc.date.issued1987-12-
dc.identifier.citationInternational Journal of Theoretical Physics, Vol. 26, No. 12, pp. 1127 - 113en
dc.identifier.issn0020-7748-
dc.identifier.urihttp://hdl.handle.net/2248/4042-
dc.descriptionRestricted Access-
dc.description.abstractUnification of gravity with GUTs is usually expected at the Planck energy E pl≈10/sup19 GeV. However, the vastly different values of the two couplings at E Pl ( α GUT« 1, α grav≈ 1) would make such unity (at E Pl) implausible unless there is a drastic change in the behavior of either gravity or GUTs around E Pl. We picture gravity and GUTs to be unified at energies >EPl with a single dimensionless coupling constant ( α U « 1) and described by a scale-invariant action quadratic in the Weyl curvature (with Yang-Mills fields). Breaking of scale invariance at E Pl then separates the interactions into gravity, now described by a Hilbert action with a dimensional G and GUTs woth a dimensionless α GUT and YM action. Problems with Klein-Kaluza unification of gravity with GUTs are also discussed in this context.en
dc.language.isoenen
dc.publisherSpringeren
dc.relation.urihttp://www.springerlink.com/content/t4237h3876660417/en
dc.subjectUnification of gravityen
dc.subjectGUTsen
dc.subjectUniverseen
dc.titleAt what energy does gravity unite with grand unified theories in the early universe?en
dc.typeArticleen
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