Cold and Nonthermal Production After a Bounce That Reheats Gently

Not every bounce reheats the universe to extreme temperatures. If the post-bounce reheating temperature is low, thermal production of the heavy particles that baryogenesis usually relies on is shut off, and the asymmetry must be made cold or nonthermally. This paper computes the trade-off. Thermally, a reheating temperature T_reh permits heavy-neutrino production only up to masses near 3 T_reh, so T_reh = 1e9 GeV caps thermal leptogenesis at 3.0e+09 GeV, below its usual minimum scale. Nonthermally, decays of a heavy field of mass 1e13 GeV with branching ratio 0.1 produce eta = 3.74e-12 at T_reh = 1e9 GeV and 3.74e-09 at 1e12 GeV, for reference CP asymmetry 1e-6 and efficiency 0.1; matching the observed eta at the reference parameters requires T_reh near 1.63e+11 GeV. Low-temperature bounces are therefore not excluded from baryogenesis, but they must use nonthermal production and they pay for it in parameter tuning. Computed from stated assumptions, not measured.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-11
DOI
https://doi.org/10.5281/zenodo.24142519
Primary Topic
Particle physics theoretical and experimental studies
Type
article
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article

Cold and Nonthermal Production After a Bounce That Reheats Gently

William Alexander Aldred
Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
article

Cold and Nonthermal Production After a Bounce That Reheats Gently

William Alexander Aldred
article en

Abstract

Not every bounce reheats the universe to extreme temperatures. If the post-bounce reheating temperature is low, thermal production of the heavy particles that baryogenesis usually relies on is shut off, and the asymmetry must be made cold or nonthermally. This paper computes the trade-off. Thermally, a reheating temperature T_reh permits heavy-neutrino production only up to masses near 3 T_reh, so T_reh = 1e9 GeV caps thermal leptogenesis at 3.0e+09 GeV, below its usual minimum scale. Nonthermally, decays of a heavy field of mass 1e13 GeV with branching ratio 0.1 produce eta = 3.74e-12 at T_reh = 1e9 GeV and 3.74e-09 at 1e12 GeV, for reference CP asymmetry 1e-6 and efficiency 0.1; matching the observed eta at the reference parameters requires T_reh near 1.63e+11 GeV. Low-temperature bounces are therefore not excluded from baryogenesis, but they must use nonthermal production and they pay for it in parameter tuning. Computed from stated assumptions, not measured.

Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
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