What is needed of a tachyon if it is to be the dark energy?
| dc.contributor.author | Copeland, E. J. | |
| dc.contributor.author | Garousi, M. R. | |
| dc.contributor.author | Sami, M. | |
| dc.contributor.author | et al. | |
| dc.date.accessioned | 2012-03-09T06:26:02Z | |
| dc.date.available | 2012-03-09T06:26:02Z | |
| dc.date.issued | 2011-07-06 | |
| dc.description.abstract | We study a dark energy scenario in the presence of a tachyon field φ with potential V (φ) and a barotropic perfect fluid. The cosmological dynamics crucially depends on the asymptotic behavior of the quantity λ = −MpVφ/V 3/2 . If λ is a constant, which corresponds to an inverse square potential V (φ) ∝ φ−2 , there exists one stable critical point that gives an acceleration of the universe at late times. When λ → 0 asymptotically, we can have a viable dark energy scenario in which the system approaches an “instantaneous” critical point that dynamically changes with λ. If |λ| approaches infinity asymptotically, the universe does not exhibit an acceleration at late times. In this case, however, we find an interesting possibility that a transient acceleration occurs in a regime where |λ| is smaller than of order unity. | en_US |
| dc.identifier.uri | http://hdl.handle.net/11007/992 | |
| dc.language.iso | en | en_US |
| dc.relation.ispartofseries | IUCAA Preprints;54/04 | |
| dc.subject | Dark energy | en_US |
| dc.subject | Tachyon | en_US |
| dc.title | What is needed of a tachyon if it is to be the dark energy? | en_US |
| dc.type | Article | en_US |