Abstract

We propose a simple mechanism of light dark matter (DM) production from the decay of the oscillating inflaton condensation. If the reheating temperature after inflation is higher than the inflaton mass, which is of the same order of the momentum of the DM at the time of the production, the DM momentum can be suppressed compared to the temperature of the thermal plasma if the interaction of the DM is weak enough. Consequently, the DM can be cold enough to avoid the observational constraints on the warm DM, like the Lyman-α bound even if the DM mass is small. We study the bosonic and fermionic DM production from the inflaton decay, taking into account the effect of the stimulated emission and Pauli blocking, respectively. In both cases, the DM can be cold and abundant enough to be a viable candidate of the DM. We also apply our mechanism to the production of isocurvature-problem-free axion DM and Dirac sea DM of right-handed neutrino consistent the seesaw relation for the active neutrino masses.

Highlights

  • Throughout this paper we will use a Boltzmann equation, which governs the evolution of the distribution function of the dark matter (DM) particle, to describe the DM production from the inflaton decay

  • Universe to discuss the DM abundance produced by the decay of a scalar field φ

  • We discuss some relations between the Boltzmann equation and resonance parameter, which is introduced for a microscopic picture

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Summary

Basic formalisms

Throughout this paper we will use a Boltzmann equation, which governs the evolution of the distribution function of the DM particle, to describe the DM production from the inflaton decay. Universe to discuss the DM abundance produced by the decay of a scalar field φ (which is identified as the inflaton). ~k the DM production is via the two-body decay of the inflaton, φ → χχ In such a case, the collision term is given by h i (0). For more discussion about the particle production in the framework of the quantum field theory, as well as the relation between the parametric resonance and the Bose-enhancement factor, see [41]. Such effects are suppressed when the amplitude of φ is small enough; the higher order terms are suppressed by powers of q and are negligible when q 1 [47]

Cold DM from inflaton decay
DM production in a narrow resonance regime
This leads to
DASER production of isocurvature free axion DM
Dirac sea DM of right handed neutrino
MN c
TG bound
Reheating from evaporating inflaton
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