Abstract

We search for nuclear recoil signals of dark matter models with a light mediator in PandaX-II, a direct detection experiment in the China Jinping underground laboratory. Using data collected in 2016 and 2017 runs, corresponding to a total exposure of 54ton day, we set upper limits on the zero-momentum dark matter-nucleon cross section. These limits have a strong dependence on the mediator mass when it is comparable to or below the typical momentum transfer. We apply our results to constrain self-interacting dark matter models with a light mediator mixing with standard model particles, and set strong limits on the model parameter space for the dark matter mass ranging from 5GeV to 10TeV.

Highlights

  • We search for nuclear recoil signals of dark matter models with a light mediator in PandaX-II, a direct detection experiment in the China Jinping underground laboratory

  • We apply our results to constrain self-interacting dark matter models with a light mediator mixing with standard model particles, and set strong limits on the model parameter space for the dark matter mass ranging from 5 GeV to 10 TeV

  • In this Letter, we report upper limits on the dark matter (DM)-nucleon scattering cross section induced by a light mediator and interpret them to constrain the self-interacting DM (SIDM) models proposed in Ref. [4]

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Summary

Published by the American Physical Society

Signal event in direct detection can be enhanced towards low recoil energies, a smoking-gun signature of SIDM [4,6,7,18]. Z v≥vmin d3vvfðv; tÞ; ð2Þ where ρ is the local DM density which we set to be 0.3 GeV=cm, mχ is the DM particle mass, fðv; tÞ is the time-dependent DM velocity distribution relative to the detector, and vmin is the minimum DM velocity that results in a recoil energy E This analysis uses the same data sets as the recent WIMP search (unblind) in PandaX-II [22], consisting of 80 live days of exposure in 2016 and 77 live days of exposure in 2017, the largest published data set of its kind to date. We plot PandaX-II detection efficiency as a function of S1 (magenta) It is nearly a constant over the range of 10–45 PE, but is reduced dramatically for S1 < 10 PE, where the event rate of the light-mediator model is maximized.

Detection efficiency
CMB excluded
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