Indirect searches for realistic sub-GeV Dark Matter models

TL;DR

This paper investigates indirect detection methods for sub-GeV dark matter models, analyzing current constraints and future prospects with upcoming MeV gamma-ray telescopes, focusing on secondary emissions like inverse Compton scattering.

Contribution

It provides a detailed analysis of indirect detection signals for two realistic sub-GeV dark matter models, including current constraints and future detection prospects with the COSI telescope.

Findings

Current observations constrain annihilation cross-section to below 10^{-27} cm^3/s.

Secondary photons often dominate the indirect detection signals.

Upcoming instruments like COSI can probe new parameter space.

Abstract

Indirect searches for Dark Matter (DM) particles with mass in the MeV -- GeV scale have received significant attention lately. Pair-annihilations of such DM particles in the Galaxy can give rise to (at the same time) MeV to GeV $\gamma$-rays via prompt emission, sub-GeV $e^\pm$ in cosmic-rays, as well as a broad photon spectrum ranging from $X$-rays to soft $\gamma$-rays, produced by the DM induced $e^\pm$ via inverse Compton scattering, bremsstrahlung and in-flight annihilation processes (collectively called `secondary emissions'). We focus on two representative realistic sub-GeV DM models, namely, the vector-portal kinetic-mixing model and the higgs-portal model, and perform a detailed study of the indirect detection constraints from existing $X$-rays, $\gamma$-rays and cosmic-ray observations, based on all of the above-mentioned signals. We also estimate the future prospects from the upcoming MeV photon telescope COSI, including all possible types of prompt and secondary emission signals. We compare our results with the constraints and (or) projections from cosmological and terrestrial observations. We find that, for both the sub-GeV DM models, the current observations constrain the annihilation cross-section at the level of $\langle \sigma v \rangle \lesssim 10^{-27} {\rm cm}^3/{\rm s}$, or lower for some specific mass ranges or under optimistic assumptions. Moreover, new unconstrained DM parameter space can be probed at the upcoming instruments like COSI, thanks to the inclusion of secondary photons which in many cases provide the dominant signal.