What is needed of a tachyon if it is to be the dark energy?
| dc.creator | Copeland, Edmund J. | |
| dc.creator | Garousi, Mohammad R. | |
| dc.creator | Sami, M. | |
| dc.creator | Tsujikawa, Shinji | |
| dc.date | 2004-11-22 | |
| dc.date | 2005-01-28 | |
| dc.date.accessioned | 2026-07-07T10:30:06Z | |
| dc.date.available | 2026-07-07T10:30:06Z | |
| dc.description | 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 $λ=-M_pV_ϕ/V^{3/2}$. If $λ$ is a constant, which corresponds to an inverse square potential $V(ϕ) \propto ϕ^{-2}$, there exists one stable critical point that gives an acceleration of the universe at late times. When $λ\to 0$ 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. | |
| dc.description | 11 pages and 3 figures, minor clarifications added; final version to appear in PRD | |
| dc.identifier | https://arxiv.org/abs/hep-th/0411192 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0411192 | |
| dc.identifier | Phys.Rev.D71:043003,2005 | |
| dc.identifier | doi:10.1103/PhysRevD.71.043003 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/178032 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | Astrophysics | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | What is needed of a tachyon if it is to be the dark energy? | |
| dc.type | text |