Pre-thermalized gravitational waves

A bstract We investigate a novel gravitational wave (GW) production mechanism from gravitons generated during the pre-thermal phase of cosmic reheating, where the energy density is dominated by non-thermalized inflaton decay products, dubbed reheatons . We consider multiple production channels, including: i ) pure inflaton-inflaton annihilation, ii ) graviton Bremsstrahlung from inflaton decay, iii ) scatterings between an inflaton and a reheaton, and iv ) scatterings among reheatons. To determine the resulting GW spectrum, we solve the Boltzmann equation to obtain the graviton phase-space distribution for each channel. We find that the third channel, iii ), dominates due to the large occupation number of reheatons at highly-energetic states during the pre-thermalization phase. Notably, in scenarios with a low inflaton mass, the GW spectrum could fall within the sensitivity range of future experiments such as the Einstein Telescope, the Cosmic Explorer, the Big Bang Observer, and ultimate DECIGO.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-08-18
DOI
https://doi.org/10.1007/jhep08(2025)125
Citations
3
Primary Topic
Cosmology and Gravitation Theories
Type
article
Field-Weighted Citation Impact
3.46
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article

Pre-thermalized gravitational waves

Nicolás Bernal, Yong Xu, Xun-Jie Xu, Quan-feng Wu
3 citations
Journal of High Energy Physics
Cosmology and Gravitation Theories
3.46
article

Pre-thermalized gravitational waves

Nicolás Bernal, Yong Xu, Xun-Jie Xu, Quan-feng Wu
article en
3 citations

Abstract

A bstract We investigate a novel gravitational wave (GW) production mechanism from gravitons generated during the pre-thermal phase of cosmic reheating, where the energy density is dominated by non-thermalized inflaton decay products, dubbed reheatons . We consider multiple production channels, including: i ) pure inflaton-inflaton annihilation, ii ) graviton Bremsstrahlung from inflaton decay, iii ) scatterings between an inflaton and a reheaton, and iv ) scatterings among reheatons. To determine the resulting GW spectrum, we solve the Boltzmann equation to obtain the graviton phase-space distribution for each channel. We find that the third channel, iii ), dominates due to the large occupation number of reheatons at highly-energetic states during the pre-thermalization phase. Notably, in scenarios with a low inflaton mass, the GW spectrum could fall within the sensitivity range of future experiments such as the Einstein Telescope, the Cosmic Explorer, the Big Bang Observer, and ultimate DECIGO.

Journal of High Energy PhysicsVol. 2025(8)
Chinese Academy of Sciences (CN), New York University (US)
Openalex Percentile: Top 7%
Cosmology and Gravitation Theories
3.46
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