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Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 protons on target

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Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 protons on target. / T2K Collaboration.
In: Physical Review D, Vol. 103, No. 11, 112008, 01.06.2021.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

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T2K Collaboration. Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 protons on target. Physical Review D. 2021 Jun 1;103(11):112008. doi: 10.1103/PhysRevD.103.112008

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T2K Collaboration. / Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 protons on target. In: Physical Review D. 2021 ; Vol. 103, No. 11.

Bibtex

@article{283341ff7c5945e4b3a1692912990976,
title = "Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 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)×1020 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 Pontecorvo-Maki-Nakagawa-Sakata parameters. For fits including a constraint on sin2θ13 from reactor data and assuming normal mass ordering T2K measures sin2θ23=0.53-0.04+0.03 and Δm322=(2.45±0.07)×10-3 eV2 c-4. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper sin2θ23 octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the 2σ level. ",
author = "{T2K Collaboration} and K. Abe and N. Akhlaq and R. Akutsu and A. Ali and C. Alt and C. Andreopoulos and M. Antonova and S. Aoki and T. Arihara and Y. Asada and Y. Ashida and E.T. Atkin and D. Barrow and S.B. Boyd and S.L. Cartwright and L. Cook and T. Dealtry and S. Dolan and T.A. Doyle and A.J. Finch and E.A.G. Goodman and C.K. Jung and S. King and L.L. Kormos and M. Lawe and S.-K. Lin and S.L. Liu and X. Lu and Y. Nakajima and Y. Nakano and J. Nowak and H.M. O'Keeffe and K. Okumura and R.A. Owen and L. Pickering and A. Pritchard and P.N. Ratoff and M. Scott and S.Y. Suzuki and Y. Takeuchi and L.F. Thompson and J. Walker and J.G. Walsh and Y. Wang and L. Wan and C. Wilkinson and J.R. Wilson and J. Xia and Y.-H. Xu and M. Yu",
year = "2021",
month = jun,
day = "1",
doi = "10.1103/PhysRevD.103.112008",
language = "English",
volume = "103",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "11",

}

RIS

TY - JOUR

T1 - Improved constraints on neutrino mixing from the T2K experiment with 3.13×1021 protons on target

AU - T2K Collaboration

AU - Abe, K.

AU - Akhlaq, N.

AU - Akutsu, R.

AU - Ali, A.

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 - Barrow, D.

AU - Boyd, S.B.

AU - Cartwright, S.L.

AU - Cook, L.

AU - Dealtry, T.

AU - Dolan, S.

AU - Doyle, T.A.

AU - Finch, A.J.

AU - Goodman, E.A.G.

AU - Jung, C.K.

AU - King, S.

AU - Kormos, L.L.

AU - Lawe, M.

AU - Lin, S.-K.

AU - Liu, S.L.

AU - Lu, X.

AU - Nakajima, Y.

AU - Nakano, Y.

AU - Nowak, J.

AU - O'Keeffe, H.M.

AU - Okumura, K.

AU - Owen, R.A.

AU - Pickering, L.

AU - Pritchard, A.

AU - Ratoff, P.N.

AU - Scott, M.

AU - Suzuki, S.Y.

AU - Takeuchi, Y.

AU - Thompson, L.F.

AU - Walker, J.

AU - Walsh, J.G.

AU - Wang, Y.

AU - Wan, L.

AU - Wilkinson, C.

AU - Wilson, J.R.

AU - Xia, J.

AU - Xu, Y.-H.

AU - Yu, M.

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)×1020 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 Pontecorvo-Maki-Nakagawa-Sakata parameters. For fits including a constraint on sin2θ13 from reactor data and assuming normal mass ordering T2K measures sin2θ23=0.53-0.04+0.03 and Δm322=(2.45±0.07)×10-3 eV2 c-4. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper sin2θ23 octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the 2σ 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)×1020 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 Pontecorvo-Maki-Nakagawa-Sakata parameters. For fits including a constraint on sin2θ13 from reactor data and assuming normal mass ordering T2K measures sin2θ23=0.53-0.04+0.03 and Δm322=(2.45±0.07)×10-3 eV2 c-4. The Bayesian analyses show a weak preference for normal mass ordering (89% posterior probability) and the upper sin2θ23 octant (80% posterior probability), with a uniform prior probability assumed in both cases. The T2K data exclude CP conservation in neutrino oscillations at the 2σ level.

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 - 1550-7998

IS - 11

M1 - 112008

ER -