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  • Open Access

Search for heavy neutrinos with the T2K near detector ND280

K. Abe et al. (T2K Collaboration)
Phys. Rev. D 100, 052006 – Published 10 September 2019

Abstract

This paper reports on the search for heavy neutrinos with masses in the range 140<MN<493MeV/c2 using the off-axis near detector ND280 of the T2K experiment. These particles can be produced from kaon decays in the standard neutrino beam and then subsequently decay in ND280. The decay modes under consideration are Nα±π and Nα+βν()(α,β=e,μ). A search for such events has been made using the Time Projection Chambers of ND280, where the background has been reduced to less than two events in the current dataset in all channels. No excess has been observed in the signal region. A combined Bayesian statistical approach has been applied to extract upper limits on the mixing elements of heavy neutrinos to electron-, muon- and tau- flavored currents (Ue2, Uμ2, Uτ2) as a function of the heavy neutrino mass, e.g., Ue2<109 at 90% C.L. for a mass of 390MeV/c2. These constraints are competitive with previous experiments.

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  • Received 5 April 2019

DOI:https://doi.org/10.1103/PhysRevD.100.052006

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. 100, Iss. 5 — 1 September 2019

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Images

  • Figure 1
    Figure 1

    An exploded view of the ND280 off-axis near detector labeling each subdetector. Adapted from [10].

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  • Figure 2
    Figure 2

    Expected flux of heavy neutrinos crossing the ND280 TPCs from K±μ±N and K±e±N for several values of MN, with the T2K beam in neutrino-mode and for Ue2=Uμ2=1. The black dotted curve corresponds to the limiting case of a massless neutrino (N=ν); the one for Keν is not drawn as it is a few orders of magnitude lower due to helicity suppression.

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  • Figure 3
    Figure 3

    Schematic of all the possible production and decay mode combinations for heavy neutrinos with 140<MN<493MeV/c2. The colored bars show the allowed kinematic regions for each decay mode, with the corresponding mixing element in the right column. A total of 40 production/decay mode combinations are possible.

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  • Figure 4
    Figure 4

    Heavy neutrino signal selection efficiency in neutrino mode as a function of heavy neutrino mass for some of the decay modes. Error bars include both statistical and systematic uncertainties.

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  • Figure 5
    Figure 5

    90% upper limits on the mixing element Ue2 as a function of heavy neutrino mass using the single-channel approach, considering only the contribution from K±e±N,Ne±π, with the three methods A, B and C. The limits are compared to the ones of PS191 experiment [6, 7].

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  • Figure 6
    Figure 6

    90% upper limits on the mixing elements Ue2 (top), Uμ2 (middle), Uτ2 (bottom) as a function of heavy neutrino mass, obtained with the combined approach. The blue dashed lines corresponds to the results of the single-channel approach (method C). The blue solid lines are obtained after marginalization over the two other mixing elements. In the top plot, the additional blue dotted line corresponds to the case where profiling is used (Uμ2=Uτ2=0), as explained in the main text. The limits are compared to the ones of other experiments: PS191 [6, 7], E949 [5], CHARM [27].

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  • Figure 7
    Figure 7

    2D contours in the Ue2Uμ2 plane, after profiling over Uτ2 (Uτ2=0). Each line corresponds to a different heavy neutrino mass hypothesis.

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It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

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