Abstract

We provide a detailed study of gravitational reheating in quintessential inflation generalizing previous analyses only available for the standard case when inflation is followed by an era dominated by the energy density of radiation. Quintessential inflation assumes a common origin for inflation and the dark energy of the Universe. In this scenario reheating can occur through gravitational particle production during the inflation-kination transition. We calculate numerically the amount of the radiation energy density, and determine the temperature Tβˆ—T_* at which radiation starts dominating over kination. The value of Tβˆ—T_* is controlled by the Hubble parameter H0H_0 during inflation and the transition time Ξ”t\Delta t, scaling as H02[ln⁑(1/H0Ξ”t)]3/4H_0^2 [\ln(1/H_0\Delta t)]^{3/4} for H0Ξ”tβ‰ͺ1H_0 \Delta t \ll1 and H02(H0Ξ”t)βˆ’cH_0^2 (H_0 \Delta t)^{-c} for H0Ξ”t≫1H_0\Delta t \gg 1. The model-dependent parameter cc is found to be around 0.5 in two different parametrizations for the transition between inflation and kination.Comment: 12 pages, 5 figure

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    Last time updated on 01/04/2019