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We report an improved measurement of muon anti-neutrino disappearance over a distance of 735km using the MINOS detectors and the Fermilab Main Injector neutrino beam in a muon anti-neutrino enhanced configuration.
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2008
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D. G. Michael et al. (MINOS), Nucl. Instrum. Meth. A 596
2008
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In matter P ( ν μ → ν μ ) P(\nu_{\mu}\rightarrow\nu_{\mu}) and P ( ν ¯ μ → ν ¯ μ ) P(\overline{\nu}_{\mu}\rightarrow\overline{\nu}_{\mu}) can differ by as much as 0.1% due to ν μ ↔ ν e \nu_{\mu}{}\leftrightarrow\nu_{e}{} mixing and ν e \nu_{e}{} and ν ¯ e \overline{\nu}_{e}{} scattering on electrons. This effect is too small to be observed in our experiment
Cited in the paper.
Accounting for flux and cross-sections, the ν μ \nu_{\mu} ( ν ¯ μ \overline{\nu}_{\mu} ) enhanced beam consists of 91.7%(58.1%) ν μ \nu_{\mu} , 7.0%(39.9%) ν ¯ μ \overline{\nu}_{\mu} and 1.3%(2.0%) ν e \nu_{e} + ν ¯ e \overline{\nu}_{e}
Cited in the paper.
S. Kopp, arXiv:physics/0508001
Cited in the paper.
A zero field is expected due to symmetry around the beam axis. We measure a 1 × 10 − 2 mrad 1\times 10^{-2}\,\mathrm{mrad} deflection of the primary proton beam, corresponding to B ⋅ d ℓ = 43 Gm B\cdot\mathrm{d}\ell=43\,\mathrm{Gm}
Cited in the paper.
2011
Later among the works it cites.
K. Abe et al. (T2K) (2012), eprint arXiv:hep-ex/1201.1386
2012
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