| dc.contributor.author | Sivaram, C | |
| dc.date.accessioned | 2008-12-02T14:09:48Z | |
| dc.date.available | 2008-12-02T14:09:48Z | |
| dc.date.issued | 1987-12 | |
| dc.identifier.citation | International Journal of Theoretical Physics, Vol. 26, No. 12, pp. 1127 - 113 | en |
| dc.identifier.issn | 0020-7748 | |
| dc.identifier.uri | http://hdl.handle.net/2248/4042 | |
| dc.description | Restricted Access | |
| dc.description.abstract | Unification 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.iso | en | en |
| dc.publisher | Springer | en |
| dc.relation.uri | http://www.springerlink.com/content/t4237h3876660417/ | en |
| dc.subject | Unification of gravity | en |
| dc.subject | GUTs | en |
| dc.subject | Universe | en |
| dc.title | At what energy does gravity unite with grand unified theories in the early universe? | en |
| dc.type | Article | en |