Abstract

The millicharged particle has become an attractive topic to probe physics beyond the Standard Model. In direct detection experiments, the parameter space of millicharged particles can be constrained from the atomic ionization process. In this work, we develop the relativistic impulse approximation (RIA) approach, which can duel with atomic many-body effects effectively, in the atomic ionization process induced by millicharged particles. The formulation of RIA in the atomic ionization induced by millicharged particles is derived, and the numerical calculations are obtained and compared with those from free electron approximation and equivalent photon approximation. Concretely, the atomic ionizations induced by mllicharged dark matter particles and millicharged neutrinos in high-purity germanium (HPGe) and liquid xenon (LXe) detectors are carefully studied in this work. The differential cross sections, reaction event rates in HPGe and LXe detectors, and detecting sensitivities on dark matter particle and neutrino millicharge in next-generation HPGe and LXe based experiments are estimated and calculated to give a comprehensive study. Our results suggested that the next-generation experiments would improve 2-3 orders of magnitude on dark matter particle millicharge δχ than the current best experimental bounds in direct detection experiments. Furthermore, the next-generation experiments would also improve 2-3 times on neutrino millicharge δν than the current experimental bounds.

Highlights

  • The underling nature is still a mystery and can’t be solved in the context of Standard Model

  • We develop the relativistic impulse approximation (RIA) approach, which can duel with atomic many-body effects effectively, in the atomic ionization process induced by millicharged particles

  • Inspired by the previous researches in many-body physics, in this work, we develop the relativistic impulse approximation (RIA) in the atomic ionization process induced by millicharged particles

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Summary

Millicharged particles

This section gives a brief introduction to the millicharged particles. The mechanism giving rise to the millichaged particle and the current experimental bounds for millicharged particles are mainly discussed. Where γμ is the conventional Dirac-γ matrices, and Bμ is the gauge boson in the U (1)Y Standard Model gauge group In these models, the right-handed massive fermion χ is the millicharged particle with mass to be mχ, and its electric charge is related to the millicharge δχ via qχ = δχe. The experimental constrains from accelerators and colliders (COLL [7, 92], SLAC [98], LHC [14], E613 [99], MiniBooNE [100], ArgoNeuT [101]) are presented in this figure as comparisons This figure gives our estimations of detecting sensitivity for millicharged dark matter particles in next-generation LXe based experiments calculated using our RIA approach developed in this work

General pictures for the RIA approach
The RIA approach for the atomic ionization induced by millicharged particles
Some comments
Differential cross section with respect to energy transfer
Numerical results and discussions on millicharged dark matter particles
Differential cross section
Reaction event rate in HPGe and LXe detectors
RIA Results
Numerical results and discussions on millicharged neutrinos
Summary and conclusion
A Free electron approximation
B Equivalent photon approximation
C Dirac-Fock theory
D Supplementary: more figures on reaction event rates in HPGe and LXe detectors
Full Text
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