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Production of massive particles during reheating

8 Pith papers cite this work. Polarity classification is still indexing.

8 Pith papers citing it
abstract

What is commonly called the reheat temperature, $T_{RH}$, is not the maximum temperature obtained after inflation. The maximum temperature is, in fact, much larger than $T_{RH}$. As an application of this we consider the production of massive stable dark-matter particles of mass $M_X$ during reheating, and show that their abundance is suppressed as a power of $T_{RH}/M_X$ rather than $\exp(-M_X/T_{RH})$. We find that particles of mass as large as $2\times 10^3$ times the reheat temperature may be produced in interesting abundance. In addition to dark matter, our analysis is relevant for baryogenesis if the baryon asymmetry is produced by the baryon (or lepton) number violating decays of superheavy bosons, and also for relic ultra-high energy cosmic rays if decays of superheavy particles are responsible for the highest energy cosmic rays.

citation-role summary

background 4

citation-polarity summary

years

2026 8

verdicts

UNVERDICTED 8

roles

background 4

polarities

background 4

representative citing papers

Asymmetric Reheating of Dark QED

hep-ph · 2026-05-10 · unverdicted · novelty 6.0

Asymmetric reheating in Dark QED produces dark matter via a new channel where DM particles annihilate while still being created by inflaton decay, with the hidden-to-visible temperature ratio tied to the square root of the Yukawa coupling ratio.

Gravitational Waves from Matter Perturbations of Spectator Scalar Fields

hep-ph · 2026-04-06 · unverdicted · novelty 5.0

A spectator scalar field with strong portal coupling to the inflaton sources a stochastic gravitational wave background reaching Ω_GW h² ∼ 10^{-11} at frequencies 10^7-10^8 Hz for benchmark parameters σ/λ ≃ 10^4 and T_reh = 2×10^{14} GeV.

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Showing 8 of 8 citing papers.