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Improved constraints on neutrino mixing from the T2K experiment with $\mathbf{3.13\times10^{21}}$ protons on target

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Improved constraints on neutrino mixing from the T2K experiment with $\mathbf{3.13\times10^{21}}$ protons on target. / T2K Collaboration ; Dealtry, T.; Doyle, T. A. et al.
In: Physical Review D, Vol. 103, No. 11, 112008, 01.06.2021.

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@article{8fb173ae33784c51a4743c92e69a0648,
title = "Improved constraints on neutrino mixing from the T2K experiment with $\mathbf{3.13\times10^{21}}$ protons on target",
abstract = " The T2K experiment reports updated measurements of neutrino and antineutrino oscillations using both appearance and disappearance channels. This result comes from an exposure of $14.9~(16.4) \times 10^{20}$ protons on target in neutrino (antineutrino) mode. Significant improvements have been made to the neutrino interaction model and far detector reconstruction. An extensive set of simulated data studies have also been performed to quantify the effect interaction model uncertainties have on the T2K oscillation parameter sensitivity. T2K performs multiple oscillation analyses that present both frequentist and Bayesian intervals for the PMNS parameters. For fits including a constraint on \ssqthonethree from reactor data and assuming normal mass ordering T2K measures $\sin^2\theta_{23} = 0.53^{+0.03}_{-0.04}$ and $\Delta{}m^2_{32} = (2.45 \pm 0.07) \times 10^{-3}$ eV$^{2}$c$^{-4}$. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper $\sin^2\theta_{23}$ octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the $2\sigma$ level. ",
keywords = "hep-ex",
author = "{T2K Collaboration} and K. Abe and N. Akhlaq and R. Akutsu and C. Alt and C. Andreopoulos and M. Antonova and S. Aoki and T. Arihara and Y. Asada and Y. Ashida and Atkin, {E. T.} and Y. Awataguchi and Barker, {G. J.} and G. Barr and M. Batkiewicz-Kwasniak and A. Beloshapkin and F. Bench and V. Berardi and L. Berns and S. Bhadra and A. Blanchet and A. Blondel and S. Bolognesi and T. Bonus and B. Bourguille and A. Bravar and Bergu, {D. Bravo} and C. Bronner and S. Bron and A. Bubak and Avanzini, {M. Buizza} and S. Cao and Catanesi, {M. G.} and A. Cervera and D. Cherdack and G. Christodoulou and M. Cicerchia and J. Coleman and G. Collazuol and D. Coplowe and T. Dealtry and Doyle, {T. A.} and Finch, {A. J.} and Kormos, {L. L.} and M. Lawe and J. Nowak and O'Keeffe, {H. M.} and Ratoff, {P. N.} and Walsh, {J. G.}",
year = "2021",
month = jun,
day = "1",
doi = "10.1103/PhysRevD.103.112008",
language = "English",
volume = "103",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "American Physical Society",
number = "11",

}

RIS

TY - JOUR

T1 - Improved constraints on neutrino mixing from the T2K experiment with $\mathbf{3.13\times10^{21}}$ protons on target

AU - T2K Collaboration

AU - Abe, K.

AU - Akhlaq, N.

AU - Akutsu, R.

AU - Alt, C.

AU - Andreopoulos, C.

AU - Antonova, M.

AU - Aoki, S.

AU - Arihara, T.

AU - Asada, Y.

AU - Ashida, Y.

AU - Atkin, E. T.

AU - Awataguchi, Y.

AU - Barker, G. J.

AU - Barr, G.

AU - Batkiewicz-Kwasniak, M.

AU - Beloshapkin, A.

AU - Bench, F.

AU - Berardi, V.

AU - Berns, L.

AU - Bhadra, S.

AU - Blanchet, A.

AU - Blondel, A.

AU - Bolognesi, S.

AU - Bonus, T.

AU - Bourguille, B.

AU - Bravar, A.

AU - Bergu, D. Bravo

AU - Bronner, C.

AU - Bron, S.

AU - Bubak, A.

AU - Avanzini, M. Buizza

AU - Cao, S.

AU - Catanesi, M. G.

AU - Cervera, A.

AU - Cherdack, D.

AU - Christodoulou, G.

AU - Cicerchia, M.

AU - Coleman, J.

AU - Collazuol, G.

AU - Coplowe, D.

AU - Dealtry, T.

AU - Doyle, T. A.

AU - Finch, A. J.

AU - Kormos, L. L.

AU - Lawe, M.

AU - Nowak, J.

AU - O'Keeffe, H. M.

AU - Ratoff, P. N.

AU - Walsh, J. G.

PY - 2021/6/1

Y1 - 2021/6/1

N2 - The T2K experiment reports updated measurements of neutrino and antineutrino oscillations using both appearance and disappearance channels. This result comes from an exposure of $14.9~(16.4) \times 10^{20}$ protons on target in neutrino (antineutrino) mode. Significant improvements have been made to the neutrino interaction model and far detector reconstruction. An extensive set of simulated data studies have also been performed to quantify the effect interaction model uncertainties have on the T2K oscillation parameter sensitivity. T2K performs multiple oscillation analyses that present both frequentist and Bayesian intervals for the PMNS parameters. For fits including a constraint on \ssqthonethree from reactor data and assuming normal mass ordering T2K measures $\sin^2\theta_{23} = 0.53^{+0.03}_{-0.04}$ and $\Delta{}m^2_{32} = (2.45 \pm 0.07) \times 10^{-3}$ eV$^{2}$c$^{-4}$. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper $\sin^2\theta_{23}$ octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the $2\sigma$ level.

AB - The T2K experiment reports updated measurements of neutrino and antineutrino oscillations using both appearance and disappearance channels. This result comes from an exposure of $14.9~(16.4) \times 10^{20}$ protons on target in neutrino (antineutrino) mode. Significant improvements have been made to the neutrino interaction model and far detector reconstruction. An extensive set of simulated data studies have also been performed to quantify the effect interaction model uncertainties have on the T2K oscillation parameter sensitivity. T2K performs multiple oscillation analyses that present both frequentist and Bayesian intervals for the PMNS parameters. For fits including a constraint on \ssqthonethree from reactor data and assuming normal mass ordering T2K measures $\sin^2\theta_{23} = 0.53^{+0.03}_{-0.04}$ and $\Delta{}m^2_{32} = (2.45 \pm 0.07) \times 10^{-3}$ eV$^{2}$c$^{-4}$. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper $\sin^2\theta_{23}$ octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the $2\sigma$ level.

KW - hep-ex

U2 - 10.1103/PhysRevD.103.112008

DO - 10.1103/PhysRevD.103.112008

M3 - Journal article

VL - 103

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

IS - 11

M1 - 112008

ER -