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We discuss several low-energy backgrounds to sub-GeV dark matter searches, which arise from high-energy particles of cosmic or radioactive origin that interact with detector materials. We focus on Cherenkov radiation, transition radiation, and luminescence or phonons from electron-hole pair recombination, and show that these processes are an important source of backgrounds at both current and planned detectors. We perform detailed analyses of these backgrounds at several existing and proposed experiments. We find that a large fraction of the observed single-electron events in the SENSEI 2020 run originate from Cherenkov photons generated by high-energy events in the Skipper-CCD, and from recombination photons generated in a phosphorus-doped layer of the same instrument. In a SuperCDMS HVeV 2020 run, Cherenkov photons produced in the sensor holders likely explain the origin of most of the events containing 2 to 6 electrons. At SuperCDMS SNOLAB, Cherenkov radiation from radioactive contaminants in Cirlex could dominate the low-energy backgrounds. For EDELWEISS, Cherenkov or luminescence backgrounds are subdominant to their observed event rate, but could still limit the sensitivity of their future searches. We also point out that Cherenkov radiation, transition radiation, and recombination could be a significant source of backgrounds at future experiments aiming to detect dark-matter via scintillation or phonon signals. The implications of our results for sub-GeV dark-matter searches and for the design of future detectors are significant. In particular, several design strategies to mitigate these backgrounds can be implemented, such as minimizing non-conductive materials near the target, implementing active and passive shielding, and using multiple detectors. Finally, we speculate on the implications of our results for the development of quantum computers and neutrino detectors.
The 2-years MESE IceCube events show a slightly excess in the energy range 10-100 TeV with a maximum local statistical significance of 2.3$sigma$, once a hard astrophysical power-law is assumed. A spectral index smaller than 2.2 is indeed suggested b
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