Abstract
Dark matter produced from thermal freeze-out is typically restricted to have masses above roughly 1 MeV. However, if the couplings are small, the freeze-in mechanism allows for production of dark matter down to keV masses. We consider dark matter coupled to a dark photon that mixes with the photon and dark matter coupled to photons through an electric or magnetic dipole moment. We discuss contributions to the freeze-in production of such dark matter particles from standard model fermion-antifermion annihilation and plasmon decay. We also derive constraints on such dark matter from the cooling of red giant stars and horizontal branch stars, carefully evaluating the thermal processes as well as the bremsstrahlung process that dominates for masses above the plasma frequency. We find that the parameters needed to obtain the observed relic abundance from freeze-in are excluded below a few tens of keV, depending on the value of the dark gauge coupling constant for the dark photon portal model, and below a few keV, depending on the reheating temperature for dark matter with an electric or magnetic dipole moment. While laboratory probes are unlikely to probe these freeze-in scenarios in general, we show that for dark matter with an electric or magnetic dipole moment and for dark matter masses above the reheating temperature, the couplings needed for freeze-in to produce the observed relic abundance can be probed partially by upcoming direct-detection experiments.
Highlights
In this paper, we consider several models for dark matter down to keV masses for which the relic abundance can be produced from freeze-in [9, 10]
We find that the parameters needed to obtain the observed relic abundance from freeze-in are excluded below a few tens of keV, depending on the value of the dark gauge coupling constant for the dark photon portal model, and below a few keV, depending on the reheating temperature for dark matter with an electric or magnetic dipole moment
We show the stellar constraints for the dark photon portal dark matter for m = 3mχ and for αD = 0.5 and αD = 10−6
Summary
In this work we focus on dark matter interacting with photons, either via kinetic mixing through a heavy dark photon or directly due to an electric or magnetic dipole moment. The dipole moment can be induced by heavy charged particles (a fermion and a scalar) that couple the dark matter to the SM through a loop [37]. We will check this condition below when we compare the parameters needed for freeze-in production to the couplings that would keep the dark matter in chemical equilibrium with the SM bath Another constraint on the dark matter mass comes from the existence of small-scale structure. For dark matter interacting through a dipole moment, the selfinteraction limits are not relevant, since the couplings to the mediator — the photon in this case — are very small.
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