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Indirect search for dark matter from the Galactic Center and halo with the Super-Kamiokande detector

K. Abe et al. (The Super-Kamiokande Collaboration)
Phys. Rev. D 102, 072002 – Published 9 October 2020
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Abstract

We present a search for an excess of neutrino interactions due to dark matter in the form of weakly interacting massive particles (WIMPs) annihilating in the Galactic center or halo based on the data set of Super-Kamiokande-I, -II, -III and -IV taken from 1996 to 2016. We model the neutrino flux, energy, and flavor distributions assuming WIMP self-annihilation is dominant to νν¯, μ+μ, bb¯, or W+W. The excess is in comparison to atmospheric neutrino interactions which are modeled in detail and fit to data. Limits on the self-annihilation cross section σAV are derived for WIMP masses in the range 1 GeV to 10 TeV, reaching as low as 9.6×1023cm3s1 for 5 GeV WIMPs in bb¯ mode and 1.2×1024cm3s1 for 1 GeV WIMPs in νν¯ mode. The obtained sensitivity of the Super-Kamiokande detector to WIMP masses below several tens of GeV is the best among similar indirect searches to date.

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  • Received 12 May 2020
  • Accepted 9 September 2020

DOI:https://doi.org/10.1103/PhysRevD.102.072002

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

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Issue

Vol. 102, Iss. 7 — 1 October 2020

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Images

  • Figure 1
    Figure 1

    Differential muon neutrino energy spectra for a WIMP mass of 100 GeV after taking into account neutrino oscillations throughout the Galaxy. Fluxes have been calculated based on DarkSUSY [27, 28] and Eqs. (1) and (2).

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  • Figure 2
    Figure 2

    Dark matter density (ρ) as a function of distance (r) from the GC for different DM density distribution profiles: Moore [17], NFW [15], and Kravtsov [16]. The vertical gray line indicates the solar system position, Rsc=8.5kpc. The normalizations are chosen to match the local density of DM expected at the position of the solar system from the local rotation curves, for NFW ρ(Rsc)=0.3GeVcm3 (0.27 for Moore, 0.37 for Kravtsov) [9].

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  • Figure 3
    Figure 3

    Intensity of annihilation products versus angular distance from the Galactic center for various DM halo profiles.

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  • Figure 4
    Figure 4

    Illustration of the DM annihilation signal for Mχ=5GeV/c2 (blue solid line) and Mχ=50GeV/c2 (blue dotted line) into a pair of bb¯ quarks. The samples used in the fit are presented. SK data (black points with errors), the “best-fit” atmospheric MC after oscillations (red solid), and the DM-induced neutrino signals are shown with respect to the direction of the Galactic center (cosθGC=1 corresponds to the direction of the GC). The signal normalization corresponds to the 90% C.L. upper limit for the given WIMP mass hypothesis, but has been multiplied by 10 for visibility. In the fitting procedure, the angular distributions shown in the figure are also binned in lepton momentum.

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  • Figure 5
    Figure 5

    Fitted number of DM-induced neutrinos of all flavors from annihilation into bb¯, μ+μ, W+W, and νν¯ as a function of the WIMP mass. Also shown are the expected sensitivities for the zero-signal case.

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  • Figure 6
    Figure 6

    Upper limit on the fitted number of DM-induced neutrinos of all flavors from annihilation into bb¯, μ+μ, W+W, and νν¯ as a function of the mass of the DM particles. The expected (median) limit assuming no signal is shown by the dashed line and the region containing 68.3% (95.5%) of the expected limits is shown by the green (yellow) band.

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  • Figure 7
    Figure 7

    Local p-value for the fitted number of WIMP-induced neutrinos for bb¯, μ+μ, W+W, and νν¯ annihilation channels as a function of the mass of the DM particles. Results based on data are shown as solid thick lines with points. For comparison, the expected values assuming different σAV are also shown.

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  • Figure 8
    Figure 8

    Upper limits at 90% C.L. on the σAV versus WIMP mass (the region above the lines is excluded), for dark matter annihilating through νν¯, bb¯, W+W, and μ+μ into neutrinos, assuming the NFW halo profile. SK limits, obtained in the combined fit and corresponding to a total livetime of 5325.8 (5629.1) live-days for FC and PC (UP-μ) events, are compared with published results from IceCube (1005 live-days) [44] and ANTARES (3170 live-days) [45].

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  • Figure 9
    Figure 9

    The on-source/off-source regions defined in equatorial coordinates.

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  • Figure 10
    Figure 10

    Observed asymmetry between the number of neutrino events in the on- and off-source regions across the event subcategories for the NFW halo model. Errors on the points are statistical.

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  • Figure 11
    Figure 11

    Upper limits at 90% C.L. on the DM self-annihilation cross section σAV as a function of Mχ for the bb¯ (blue), W+W (maroon), μ+μ (purple), and νν¯ (orange) annihilation channels as obtained in the on-source/off-source analysis. The influence of the halo model choice is shown as bands around the results for the benchmark NFW profile.

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  • Figure 12
    Figure 12

    Upper limits at 90% C.L. on the DM self-annihilation cross section σAV as a function of Mχ for the combined fit (solid) and on-source off-source (dashed) analyses for the bb¯ (blue), W+W (maroon), μ+μ (purple), and νν¯ (orange) annihilation channels assuming the NFW profile.

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