2015
DOI: 10.1016/j.astropartphys.2014.07.006
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Search for neutrino emission from relic dark matter in the sun with the Baikal NT200 detector

Abstract: We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels bb, W + W − and τ + τ − we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes … Show more

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Cited by 38 publications
(45 citation statements)
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“…In Fig. 7 we plot the flux as a function of the dark matter mass (neutrino flux in the left panel, muon flux in the right panel) and compare it with the experimental limits from Baikal [73]. Figure 7: Neutrino (left) and muon (right) fluxes as a function of dark matter mass (red curve).…”
Section: Indirect Detectionmentioning
confidence: 98%
“…In Fig. 7 we plot the flux as a function of the dark matter mass (neutrino flux in the left panel, muon flux in the right panel) and compare it with the experimental limits from Baikal [73]. Figure 7: Neutrino (left) and muon (right) fluxes as a function of dark matter mass (red curve).…”
Section: Indirect Detectionmentioning
confidence: 98%
“…Since then, this is one of the existing strategies to indirectly detect DM, which is in turn complementary to DM direct searches, given that in both cases the signal would be proportional to the DM elastic scattering cross section. Indeed, numerous studies have evaluated the prospects of detection of the potential high-energy neutrino flux and of that of neutrinos in the O(10-100) MeV range [72][73][74][75] using neutrino detectors/telescopes [76][77][78][79][80][81][82][83][84][85][86][87][88][89]. All these works have focused on DM-nucleon interactions.…”
Section: Introductionmentioning
confidence: 99%
“…These were derived for other Z models than the one considered here, so we have reanalyzed the ATLAS data to constrain the purely kinetically mixed Z , as described in appendix E. In figure 5(a) we show the limits on σBR for Z → e + e − and Z → µ + µ − , where BR denotes the branching ratio for Z to decay into these final states. Assuming that there are no invisible decays, the predicted values of σBR for models with 2 Stronger limits on SD scattering on protons in the sun have been obtained by neutrino detection experiments [21,22]. These depend upon the efficiency of getting neutrinos from the decays of final state particles from χχ annihilation.…”
Section: Collider Constraintsmentioning
confidence: 99%