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Combined Analysis of Neutrino and Antineutrino Oscillations at T2K

K. Abe et al. (T2K Collaboration)
Phys. Rev. Lett. 118, 151801 – Published 10 April 2017
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Abstract

T2K reports its first results in the search for CP violation in neutrino oscillations using appearance and disappearance channels for neutrino- and antineutrino-mode beams. The data include all runs from January 2010 to May 2016 and comprise 7.482×1020 protons on target in neutrino mode, which yielded in the far detector 32 e-like and 135μ-like events, and 7.471×1020 protons on target in antineutrino mode, which yielded 4 e-like and 66μ-like events. Reactor measurements of sin22θ13 have been used as an additional constraint. The one-dimensional confidence interval at 90% for the phase δCP spans the range (3.13, 0.39) for normal mass ordering. The CP conservation hypothesis (δCP=0, π) is excluded at 90% C.L.

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  • Received 3 January 2017

DOI:https://doi.org/10.1103/PhysRevLett.118.151801

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.

Published by the American Physical Society

Physics Subject Headings (PhySH)

  1. Research Areas
  1. Properties
Particles & Fields

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See Also

Measurement of the Neutrino Mixing Angle θ23 in NOvA

P. Adamson et al. (NOvA Collaboration)
Phys. Rev. Lett. 118, 151802 (2017)

Article Text

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Issue

Vol. 118, Iss. 15 — 14 April 2017

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Images

  • Figure 1
    Figure 1

    The leptonic CP asymmetry, ACP=[P(νμνe)P(ν¯μν¯e)]/[P(νμνe)+P(ν¯μν¯e)], as a function of energy for maximal CP-violation hypotheses (top) and the νμ (ν¯μ) and νe+ν¯e components of the unoscillated neutrino flux in neutrino and antineutrino modes (bottom).

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  • Figure 2
    Figure 2

    The FGD2 data, prefit predictions and postfit predictions binned in pμ (left) and cosθμ (right) for the neutrino mode CC0π (top), antineutrino mode CC 1-track μ+ (middle) and antineutrino mode CC 1-track μ (bottom) categories. The overflow bins are integrated out to 10000MeV/c for pμ and 1.0 for cosθμ respectively.

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  • Figure 3
    Figure 3

    The reconstructed lepton momentum and angle relative to the beam at the far detector for the ν¯e sample signal (left) and background (right) expectation with the data overlaid (blue points).

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  • Figure 4
    Figure 4

    The reconstructed neutrino energy at the far detector for the νe (left) and ν¯e (right) candidate samples is shown together with the expected distribution without oscillation (blue histogram) and the best fit (red histogram).

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  • Figure 5
    Figure 5

    The 68% (90%) constant 2ΔlnL confidence regions for the sin2θ23|Δm322| plane assuming normal ordering, alongside NOνA [43], MINOS+[44], SK [45], and IceCube [46] confidence regions.

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  • Figure 6
    Figure 6

    The 68% (90%) constant 2ΔlnL confidence regions in the δCPsin2θ13 plane are shown by the dashed (continuous) lines, computed independently for the normal (black) and inverted (yellow) mass ordering. The best-fit point is shown by a star for each mass-ordering hypothesis. The 68% confidence region from reactor experiments on sin2θ13 is shown by the yellow vertical band.

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  • Figure 7
    Figure 7

    2ΔlnL as a function of δCP for the normal (black) and inverted (yellow) mass ordering. The vertical lines show the corresponding allowed 90% confidence intervals, calculated using the Feldman-Cousins method. sin2θ13 is marginalized using the reactor measurement as prior probability.

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