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Improved Search for Muon-Neutrino to Electron-Neutrino Oscillations in MINOS

P. Adamson et al. (MINOS Collaboration)
Phys. Rev. Lett. 107, 181802 – Published 27 October 2011

Abstract

We report the results of a search for νe appearance in a νμ beam in the MINOS long-baseline neutrino experiment. With an improved analysis and an increased exposure of 8.2×1020 protons on the NuMI target at Fermilab, we find that 2sin2(θ23)sin2(2θ13)<0.12(0.20) at 90% confidence level for δ=0 and the normal (inverted) neutrino mass hierarchy, with a best-fit of 2sin2(θ23)sin2(2θ13)=0.0410.031+0.047(0.0790.053+0.071). The θ13=0 hypothesis is disfavored by the MINOS data at the 89% confidence level.

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  • Received 29 July 2011

DOI:https://doi.org/10.1103/PhysRevLett.107.181802

© 2011 American Physical Society

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Vol. 107, Iss. 18 — 28 October 2011

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Images

  • Figure 1
    Figure 1

    (Top) Distribution of the LEM discriminant for events in the Near Detector that pass the preselection requirements. Data (points) and Monte Carlo simulation (histogram) are shown, with the magnitude of the systematic uncertainty indicated by the band. This uncertainty is highly correlated between the ND and FD and thus cancels out to a large degree when we form our FD predictions. (Bottom) Expected background and signal distributions in the Far Detector for sin2(2θ13)=0.1. The signal distribution has been multiplied by 10 for visibility.

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  • Figure 2
    Figure 2

    Reconstructed energy spectra for νe CC candidate events in the Far Detector. The black points indicate the data with statistical error bars shown. The histogram indicates the expected background (unfilled area) together with the contribution of νμνe signal (hatched area) for the best-fit value of sin2(2θ13)=0.041.

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  • Figure 3
    Figure 3

    Allowed ranges and best fits for 2sin2(θ23)sin2(2θ13) as a function of δ. The upper (lower) panel assumes the normal (inverted) neutrino mass hierarchy. The vertical dashed line indicates the CHOOZ 90% C.L. upper limit assuming θ23=π4 and Δm322=2.32×103eV2 [10].

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