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 |