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  • Open Access

Constraints on neutrino lifetime from the Sudbury Neutrino Observatory

B. Aharmim et al. (SNO Collaboration)
Phys. Rev. D 99, 032013 – Published 25 February 2019

Abstract

The long baseline between Earth and the Sun makes solar neutrinos an excellent test beam for exploring possible neutrino decay. The signature of such decay would be an energy-dependent distortion of the traditional survival probability which can be fit for using well-developed and high-precision analysis methods. Here a model including neutrino decay is fit to all three phases of B8 solar neutrino data taken by the Sudbury Neutrino Observatory (SNO). This fit constrains the lifetime of neutrino mass state ν2 to be >8.08×105s/eV at 90% confidence. An analysis combining this SNO result with those from other solar neutrino experiments results in a combined limit for the lifetime of mass state ν2 of >1.92×103s/eV at 90% confidence.

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  • Received 3 December 2018

DOI:https://doi.org/10.1103/PhysRevD.99.032013

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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Vol. 99, Iss. 3 — 1 February 2019

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Images

  • Figure 1
    Figure 1

    The SNO detector [19].

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  • Figure 2
    Figure 2

    The fraction of solar neutrino flux that, due to the MSW effect, is mass state ν2 is shown here in a solid line. The cross-section-weighted B8 energy spectrum is shown with a dashed line to guide the eye. The ν2 state dominates over the energy range where B8 neutrinos can be detected.

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  • Figure 3
    Figure 3

    Shown here in dashed lines are survival probability of electron neutrinos Pee and the oscillation probability Pea for various values of mass state ν2 lifetime (k2), demonstrating the energy-dependent distortion being fit for. Both k1 and k3 are fixed to infinity in these plots. Existing limits are near k2=104s/eV. The solid line shows the survival probability with no neutrino decay (k2=).

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  • Figure 4
    Figure 4

    Shown here are the central values and widths of the pull distributions for the signal-only (top, 250 datasets) and all-backgrounds (bottom, two sets of 14 datasets) test cases. Expected magnitude of fluctuations in the central value are shown with gray dashed lines, while gray boxes show the expected fluctuation in pull widths.

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  • Figure 5
    Figure 5

    Shown here is the likelihood scan of the mass state ν2 lifetime k2. This is shown both with systematic parameters fixed and after incorporating systematic uncertainties using a shift-and-refit method.

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  • Figure 6
    Figure 6

    Shown here is the combined likelihood profile including the SNO result from this analysis and flux constraints from other solar experiments as described in Sec. 5b.

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