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      Gravitational waves constraints on post-inflationary phases stiffer than radiation

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          Abstract

          We point out that the existence of post-inflationary phases stiffer than radiation leads to the production of stochastic gravitational waves (GW) backgrounds whose logarithmic energy spectra (in critical units) are typically "blue" at high frequencies. The maximal spectral slope (for present frequencies larger than \(10^{-16}\) Hz) is of order one and it is related to the maximal sound velocity of the stiff plasma governing the evolution of the geometry. The duration of the stiff phase is crucially determined by the backreaction of the GW leaving the horizon during the de Sitter phase and re-entering during the stiff phase. Therefore, the maximal (inflationary) curvature scale has to be fine-tuned to a value smaller than the limits set by the large scale measurements (\(H_{dS}\laq 10^{-6}~M_{P}\)) in order to a have a sufficiently long stiff phase reaching an energy scale of the order of the \(1~{\rm TeV}\) and even lower if we want the stiff phase to touch the hadronic era (corresponding to \(T_{had}\sim 140~{\rm MeV}\)). By looking more positively at our exercise we see that, if an inflationary phase is followed by a stiff phase, there exist an appealing possibility of "graviton reheating" whose effective temperature can be generally quite low.

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          Handbook of Mathematical Functions

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            Reheating after Inflation

            The theory of reheating of the Universe after inflation is developed. The transition from inflation to the hot Universe turns out to be strongly model-dependent and typically consists of several stages. Immediately after inflation the field \(\phi\) begins rapidly rolling towards the minimum of its effective potential. Contrary to some earlier expectations, particle production during this stage does not lead to the appearance of an extra friction term \(\Gamma\dot\phi\) in the equation of motion of the field \(\phi\). Reheating becomes efficient only at the next stage, when the field \(\phi\) rapidly oscillates near the minimum of its effective potential. We have found that typically in the beginning of this stage the classical inflaton field \(\phi\) very rapidly (explosively) decays into \(\phi\)-particles or into other bosons due to broad parametric resonance. This stage cannot be described by the standard elementary approach to reheating based on perturbation theory. The bosons produced at this stage, as well as some part of the classical field \(\phi\) which survives the stage of explosive reheating, should further decay into other particles, which eventually become thermalized. The last stages of decay can be described in terms of perturbation theory. Complete reheating is possible only in those theories where a single massive \(\phi\)-particle can decay into other particles. This imposes strong constraints on the structure of inflationary models. On the other hand, this means that a scalar field can be a cold dark matter candidate even if it is strongly coupled to other fields.
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              Constraints on generalized inflationary cosmologies

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                Author and article information

                Journal
                09 June 1998
                Article
                10.1103/PhysRevD.58.083504
                hep-ph/9806329
                5d740a4f-c47a-4cea-8939-459c969f4c17
                History
                Custom metadata
                Phys.Rev. D58 (1998) 083504
                Accepted for publication in Physical Review D; 30 pages in LaTex style, 6 Encapsulated figures
                hep-ph astro-ph gr-qc hep-th

                General relativity & Quantum cosmology,General astrophysics,High energy & Particle physics

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