Abstract

Light non-relativistic components of the galactic dark matter halo elude direct detection constraints because they lack the kinetic energy to create an observable recoil. However, cosmic-rays can upscatter dark matter to significant energies, giving direct detection experiments access to previously unreachable regions of parameter-space at very low dark matter mass. In this work we extend the cosmic-ray dark matter formalism to models of inelastic dark matter and show that previously inaccessible regions of the mass-splitting parameter space can be probed. Conventional direct detection of non-relativistic halo dark matter is limited to mass splittings of $\delta\sim10~\mathrm{keV}$ and is highly mass dependent. We find that including the effect of cosmic-ray upscattering can extend the reach to mass splittings of $\delta\sim100~\mathrm{MeV}$ and maintain that reach at much lower dark matter mass.

Highlights

  • Until recent years low-mass dark matter (DM) was relatively unconstrained by direct detection experiments

  • Two useful strategies, which have been the subject of several recent studies, are the Migdal effect [18,23,32,33,34,35,36,37,38,39,40] and cosmic-ray boosted dark matter (CRDM) [19,41,42,43,44]

  • III we present the recoil spectrum arising from the inelastic scattering of CR-upscattered inelastic DM (CRIDM), and comment on the distinguishability of the scenarios under consideration

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Summary

INTRODUCTION

Until recent years low-mass dark matter (DM) was relatively unconstrained by direct detection experiments. Two useful strategies, which have been the subject of several recent studies, are the Migdal effect [18,23,32,33,34,35,36,37,38,39,40] and cosmic-ray boosted dark matter (CRDM) [19,41,42,43,44] These studies have all focused on elastic nuclear scattering. When energetic cosmic rays (mostly protons) scatter off nonrelativistic DM particles in the halo, they can produce a small population of relativistic DM If these relativistic DM particles scatter at a direct detection experiment, the deposited energy can be well above threshold. V, we conclude with a discussion of our results and future avenues

COSMIC-RAY UPSCATTERING OF INELASTIC DM
Decay of excited DM
DETECTION OF CRIDM
EXPERIMENTAL BOUNDS ON CRIDM
Findings
CONCLUSION
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