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New limits on heavy sterile neutrino mixing in B8 decay obtained with the Borexino detector

G. Bellini et al. (Borexino Collaboration)
Phys. Rev. D 88, 072010 – Published 29 October 2013

Abstract

If heavy neutrinos with mass mνH2me are produced in the Sun via the decay B8Be8+e++νH in a side branch of the pp chain, they would undergo the observable decay into an electron, a positron and a light neutrino νHνL+e++e. In the present work Borexino data are used to set a bound on the existence of such decays. We constrain the mixing of a heavy neutrino with mass 1.5MeVmνH14MeV to be |UeH|2(1034×106), respectively. These are tighter limits on the mixing parameters than obtained in previous experiments at nuclear reactors and accelerators.

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  • Received 27 May 2013

DOI:https://doi.org/10.1103/PhysRevD.88.072010

© 2013 American Physical Society

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Vol. 88, Iss. 7 — 1 October 2013

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Images

  • Figure 1
    Figure 1

    Feynman graphs describing the appearance B8Be8+e++νH (a) and decay νHνe+e++e (b),(c) of a heavy neutrino. The invisible decay mode νHνeνiν˜i is shown also (d).

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  • Figure 2
    Figure 2

    Energy spectra of the events surviving incremental selection cuts. From top to bottom: (1) raw spectrum; (2) 2 ms postmuon veto cut; (3) 20 s after muons crossing the SSS cut; (4) FV cut. See text for details.

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  • Figure 3
    Figure 3

    The expected spectra of signals due to νHνL+e++e decay for different neutrino masses mνH=4, 8, 10, 12 MeV and mixing parameter |UeH|2=1.0×105.

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  • Figure 4
    Figure 4

    The Borexino spectrum in the (4.8–12.8) MeV range. 1, optimal fit; 2, (ν,e) scattering of B8 neutrino [LMA MSW BPS06(GS98)]; 3, 15 Be11 decays; 4, the detector response function for the decay of neutrino with mνH=8MeV and |UeH|2=8×106. The inset shows the dependence of L on |UeH|4 for mνH=8MeV.

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  • Figure 5
    Figure 5

    Limits on the mixing parameter |UeH|2 as a function of neutrino mass mν (90% C.L.). 1: Present work excludes values of |UeH|2 and mν inside region 1. 2: Upper limits from reactor experiments on the search for νHνL+e++e decay due to W-exchange mode [26]. 3: Upper limits from πe+ν decay [28].

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  • Figure 6
    Figure 6

    The Borexino constraints (region 1) and limits on |UeH|2 versus mνH in the mass range (0.01–100) MeV from different experiments (see text).

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