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Electron Neutrino and Antineutrino Appearance in the Full MINOS Data Sample

P. Adamson et al. (MINOS Collaboration)
Phys. Rev. Lett. 110, 171801 – Published 22 April 2013

Abstract

We report on νe and ν¯e appearance in νμ and ν¯μ beams using the full MINOS data sample. The comparison of these νe and ν¯e appearance data at a 735 km baseline with θ13 measurements by reactor experiments probes δ, the θ23 octant degeneracy, and the mass hierarchy. This analysis is the first use of this technique and includes the first accelerator long-baseline search for ν¯μν¯e. Our data disfavor 31% (5%) of the three-parameter space defined by δ, the octant of the θ23, and the mass hierarchy at the 68% (90%) C.L. We measure a value of 2sin2(2θ13)sin2(θ23) that is consistent with reactor experiments.

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  • Received 22 January 2013

DOI:https://doi.org/10.1103/PhysRevLett.110.171801

© 2013 American Physical Society

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Vol. 110, Iss. 17 — 26 April 2013

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  • Figure 1
    Figure 1

    Distributions of αLEM. The plots in the left column correspond to the ν beam mode. The plots in the right column correspond to the ν¯ beam mode. The top row shows the distributions for ND selected events with a band about the simulation representing the systematic uncertainty. The bottom row shows the distributions for the predicted FD background and signal multiplied by 10 with 2sin2(2θ13)sin2(θ23)=0.1, δ=0, and a normal mass hierarchy.

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  • Figure 2
    Figure 2

    The reconstructed energy distributions for three αLEM ranges. The events with energy greater than 5 GeV are combined into a single bin for the fits. The vertical bars through the data points denote statistical uncertainties. The signal predictions assume sin2(2θ13)=0.051, Δm322>0, δ=0, and θ23=π/4. The plots in the left column correspond to data collected in the ν beam mode. The plots in the right column correspond to data collected in the ν¯ beam mode.

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  • Figure 3
    Figure 3

    The 68% and 90% confidence intervals of allowed values for 2sin2(2θ13)sin2(θ23) as a function of δ for the two mass hierarchies.

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  • Figure 4
    Figure 4

    The resulting values of the likelihood L, shown here as 2ΔlnL, from a fit of δ to our data using constraints from reactor experiments [8, 9, 10], assuming various values of the mass hierarchy and the sign of θ23π/4. The difference is taken with respect to the best-fitting solution. Values above the horizontal dashed lines are disfavored at either 68% or 90% C.L.

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