Scalar-Tensor Models of Normal and Phantom Dark Energy Auteur(s): Gannouji Radouane, Polarski D., Ranquet Andre, Starobinsky A.A. (Article) Publié: Journal Of Cosmology And Astroparticle Physics, vol. 0609 p.016 (2006) Texte intégral en Openaccess : Ref HAL: in2p3-00115596_v1 Ref Arxiv: astro-ph/0606287 DOI: 10.1088/1475-7516/2006/09/016 WoS: 000242449600016 Ref. & Cit.: NASA ADS Exporter : BibTex | endNote 197 Citations Résumé: We consider the viability of dark energy (DE) models in the framework of the scalar-tensor theory of gravity, including the possibility to have a phantom DE at small redshifts $z$ as admitted by supernova luminosity-distance data. For small $z$, the generic solution for these models is constructed in the form of a power series in $z$ without any approximation. Necessary constraints for DE to be phantom today and to cross the phantom divide line $p=-\rho$ at small $z$ are presented. Considering the Solar System constraints, we find for the post-Newtonian parameters that $\gamma_{PN}<1$ and $\gamma_{PN,0}\approx 1$ for the model to be viable, and $\beta_{PN,0}>1$ (but very close to 1) if the model has a significantly phantom DE today. However, prospects to establish the phantom behaviour of DE are much better with cosmological data than with Solar System experiments. Earlier obtained results for a $\Lambda$-dominated universe with the vanishing scalar field potential are extended to a more general DE equation of state confirming that the cosmological evolution of these models rule them out. Models of currently fantom DE which are viable for small $z$ can be easily constructed with a constant potential; however, they generically become singular at some higher $z$. With a growing potential, viable models exist up to an arbitrary high redshift. Commentaires: 30 pages, 4 figures; Matches the published version containing an expanded discussion of various points |