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October 20, 20250 citationsOpen Access

Direct detection of electromagnetically interacting ultraheavy dark matter

JKJason KumarUniversity of Hawaiʻi at MānoaBMBiprajit MondalIndian Institute of Science BangaloreGMGirish MuralidharaUniversity of Kentucky

Key Points

  • Photon-mediated nuclear interactions in dark matter were constrained up to mass limits of 10^17 GeV.
  • Experiments like XENON1T and PICO-60 provided key insights on millicharge limits for dark matter.
  • New methods for discriminating nuclear and electron recoils have expanded sensitivity ceilings for dark matter detection.
  • The constraints define a significant window between direct detection and neutrino experiment limits for lighter dark matter.

Abstract

At a level too faint for astronomy, particle dark matter may interact with Standard Model states via the photon. We derive limits from direct detection experiments on photon-mediated nuclear interactions up to operator dimension-6, viz. , via a millicharge, charge radius, electric and magnetic dipole moment, and anapole moment, up to dark matter masses 10^17 GeV, where detectors become flux-limited. We derive constraints for XENON1T, XENONnT, LZ, PANDAX-II, PANDAX-4T, DarkSide-50, DEAP-3600, PICO-60, and CDMS-II, and estimate future sensitivities for the multi-deca-tonne scale experiments DarkSide-20k, DARWIN/XLZD, PANDAX-xT, and Argo. Special attention is paid to millicharged dark matter, for which we constrain new parameter space by deriving the ceiling on sensitivity to its electric charge, arising from the nuclear-vs-electron recoil discriminants used in liquid argon and bubble chamber detectors. This result goes beyond ceilings previously identified in liquid xenon and semiconductor detectors from electron recoil vetoes. In particular, the ceiling from PICO-60 closes a large window between direct detection and neutrino experiment limits for dark matter masses below 10^12 GeV.

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Cite This Study

Kumar et al. (2025) studied this question.

synapsesocial.com/papers/68f5fcce8d54a28a75cf1d81https://doi.org/10.48550/arxiv.2509.24938
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