Abstract

We consider the prospects for testing the dark matter interpretation of the DAMA/LIBRA signal with the Super-Kamiokande experiment. The DAMA/LIBRA signal favors dark matter with low mass and high scattering cross section. We show that these characteristics imply that the scattering cross section that enters the DAMA/LIBRA event rate determines the annihilation rate probed by Super-Kamiokande. Current limits from Super-Kamiokande through-going events do not test the DAMA/LIBRA favored region. We show, however, that upcoming analyses including fully-contained events with sensitivity to dark matter masses from 5 to 10 GeV may corroborate the DAMA/LIBRA signal. We conclude by considering three specific dark matter candidates, neutralinos, WIMPless dark matter, and mirror dark matter, which illustrate the various model-dependent assumptions entering our analysis.

Highlights

  • Have been proposed to explain DAMA: neutralinos [19], WIMPless dark matter [12, 21, 22], and mirror dark matter [23]

  • In the low-mass region of interest, the dominant contribution to neutrino production via dark matter annihilation is from the Sun [28], and we will focus on the Sun below, the Earth may provide an interesting signal

  • It has been shown [28,29,30] that if σv ∼ 10−26 cm3 s−1, as required for the thermal relic density of dark matter to be in the observed range, for the range of parameters used in this work the Sun is in equilibrium, and

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Summary

Relating Super-Kamiokande to DAMA

Super-K may indirectly detect dark matter by finding evidence for dark matter annihilation in the Sun or Earth’s core to standard model (SM) particles that decay to neutrinos. √ where C is the capture rate, τ ≃ 4.5 Gyr is the age of the solar system, and a = σv /(4 2V ), with σ the total dark matter annihilation cross section and V the effective volume of WIMPs in the Sun (V = 5.7 × 1030 cm3(1 GeV/mX )3/2 [27, 28, 31]) It has been shown [28,29,30] that if σv ∼ 10−26 cm s−1, as required for the thermal relic density of dark matter to be in the observed range, for the range of parameters used in this work the Sun is in equilibrium Super-K bounds the νμ-flux from dark matter annihilation in the Sun. Since the total annihilation rate is equal to the capture rate, this permits Super-K to bound the dark matter-nucleon scattering cross section using eq (2.2), assuming ρX = 0.3 GeV cm−3 and a Maxwellian velocity distribution with v ∼ 220 km/s. We will see that consideration of the full Super-K event sample may provide marked improvements, and extend Super-K’s sensitivity to low masses and the DAMA regions

Projection of Super-K sensitivity
Prospects for various Dark Matter candidates
Findings
Summary
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