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Reheating Temperature and Inflaton Mass Bounds from Thermalization After Inflation

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arxiv hep-ph/9909467 v4 pith:3ENPM7CL submitted 1999-09-22 hep-ph astro-ph

classification hep-phastro-ph
keywords inflatonthermalizationdecayinflationreheatingtemperaturebeforebound
verification ladder T0 review T1 audit T2 compute T3 formal
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We consider the conditions for the decay products of perturbative inflaton decay to thermalize. The importance of considering the full spectrum of inflaton decay products in the thermalization process is emphasized. It is shown that the delay between the end of inflaton decay and thermalization allows the thermal gravitino upper bound on the reheating temperature to be raised from 10^{8} GeV to as much as 10^{12} GeV in realistic inflation models. Requiring that thermalization occurs before nucleosynthesis imposes an upper bound on the inflaton mass as a function of the reheating temperature, m_{S} < 10^{10} (T_{R}/1 GeV)^{7/9} GeV. It is also shown that even in realistic inflation models with relatively large reheating temperatures, it is non-trivial to have thermalization before the electroweak phase transition temperature. Therefore the thermal history of the Universe is very sensitive to details of the inflation model.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Post-inflationary enhancement of adiabatic perturbations in modular cosmology

    astro-ph.CO 2025-07 conditional novelty 6.0 of 10

    In modular inflation models, entropic perturbations frozen during inflation are converted into curvature perturbations after inflation, producing an enhanced power spectrum while preserving the spectral index ns.

  2. Tachyonic Encore: A universal shift of inflationary observables

    hep-th 2026-06 unverdicted novelty 5.0 of 10

    A light axion spectator induces post-inflation tachyonic phases that produce a nearly scale-invariant boost to the curvature power spectrum and alter key inflationary observables in a largely potential-independent manner.

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