Phys. Rev. D 71, 043003 (2005) [11 pages]

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

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Edmund J. Copeland1, Mohammad R. Garousi2, M. Sami3, and Shinji Tsujikawa4
1Department of Physics and Astronomy, University of Sussex, Falmer, Brighton BN1 9QJ, United Kingdom
2Department of Physics, Ferdowsi University, P.O. Box 1436, Mashhad, Iran and Institute for Studies in Theoretical Physics and Mathematics IPM, P.O. Box 19395-5531, Tehran, Iran
3IUCAA, Post Bag 4, Ganeshkhind, Pune 411 007, India
4Department of Physics, Gunma National College of Technology, Gunma 371-8530, Japan

Received 25 November 2004; published 10 February 2005

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/V3/2. 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.


©2005 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevD.71.043003
DOI: 10.1103/PhysRevD.71.043003
PACS: 98.70.Vc, 98.80.Cq

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