Abstract:We consider models for inflation with a stable inflaton. Reheating is achieved through scattering processes such as φφ → hh, where h is the Standard Model Higgs boson. We consider the reheating process in detail and show that for a relatively large coupling (needed for the late annihilations of the inflaton during freeze-out), reheating is almost instantaneous leading to a relatively high reheating temperature. The process φφ ↔ hh brings the inflaton back into equilibrium, leading to a well studied scalar sing… Show more
“…In the case of the weak scale gravitino, the thermal production cross section is independent of the temperature and therefore constant in time, implying a gravitino abundance proportional to T RH . However, when the particle production cross section depends strongly on temperature, σ ∼ T n with n ≥ 6, the abundance depends on the maximum temperature attained during the reheating process [17][18][19][21][22][23][24][25][26][27][28][29][30][31][32] (see also [33] for a pedagogical introduction on the subject). Thus, the details of the reheating process between T max and T RH become important.…”
We consider the production of dark matter during the process of reheating after inflation. The relic density of dark matter from freeze-in depends on both the energy density and energy distribution of the inflaton scattering or decay products composing the radiation bath. We compare the perturbative and non-perturbative calculations of the energy density in radiation. We also consider the (likely) possibility that the final state scalar products are unstable. Assuming either thermal or non-thermal energy distribution functions, we compare the resulting relic density based on these different approaches. We show that the present-day cold dark matter density can be obtained through freeze-in from preheating for a large range of dark matter masses.
“…In the case of the weak scale gravitino, the thermal production cross section is independent of the temperature and therefore constant in time, implying a gravitino abundance proportional to T RH . However, when the particle production cross section depends strongly on temperature, σ ∼ T n with n ≥ 6, the abundance depends on the maximum temperature attained during the reheating process [17][18][19][21][22][23][24][25][26][27][28][29][30][31][32] (see also [33] for a pedagogical introduction on the subject). Thus, the details of the reheating process between T max and T RH become important.…”
We consider the production of dark matter during the process of reheating after inflation. The relic density of dark matter from freeze-in depends on both the energy density and energy distribution of the inflaton scattering or decay products composing the radiation bath. We compare the perturbative and non-perturbative calculations of the energy density in radiation. We also consider the (likely) possibility that the final state scalar products are unstable. Assuming either thermal or non-thermal energy distribution functions, we compare the resulting relic density based on these different approaches. We show that the present-day cold dark matter density can be obtained through freeze-in from preheating for a large range of dark matter masses.
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