What is needed of a tachyon if it is to be the dark energy?

dc.contributor.authorCopeland, E. J.
dc.contributor.authorGarousi, M. R.
dc.contributor.authorSami, M.
dc.contributor.authoret al.
dc.date.accessioned2012-03-09T06:26:02Z
dc.date.available2012-03-09T06:26:02Z
dc.date.issued2011-07-06
dc.description.abstractWe 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.urihttp://hdl.handle.net/11007/992
dc.language.isoenen_US
dc.relation.ispartofseriesIUCAA Preprints;54/04
dc.subjectDark energyen_US
dc.subjectTachyonen_US
dc.titleWhat is needed of a tachyon if it is to be the dark energy?en_US
dc.typeArticleen_US

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