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Measurements of neutrino oscillation parameters from the T2K experiment using $3.6\times10^{21}$ protons on target

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Measurements of neutrino oscillation parameters from the T2K experiment using $3.6\times10^{21}$ protons on target. / The T2K Collaboration.
In: European Physical Journal C, Vol. 83, 782, 05.09.2023.

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The T2K Collaboration. Measurements of neutrino oscillation parameters from the T2K experiment using $3.6\times10^{21}$ protons on target. European Physical Journal C. 2023 Sept 5;83:782. doi: 10.1140/epjc/s10052-023-11819-x

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@article{1e1656b4e3a24bebb0e1f1f1e210a993,
title = "Measurements of neutrino oscillation parameters from the T2K experiment using $3.6\times10^{21}$ protons on target",
abstract = " The T2K experiment presents new measurements of neutrino oscillation parameters using $19.7(16.3)\times10^{20}$ protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional $4.7\times10^{20}$ POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on $\sin^2\theta_{13}$ and the impact of priors on the $\delta_\mathrm{CP}$ measurement. Both analyses prefer the normal mass ordering and upper octant of $\sin^2\theta_{23}$ with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on $\sin^2\theta_{13}$ from reactors, $\sin^2\theta_{23}=0.561^{+0.021}_{-0.032}$ using Feldman--Cousins corrected intervals, and $\Delta{}m^2_{32}=2.494_{-0.058}^{+0.041}\times10^{-3}~\mathrm{eV^2}$ using constant $\Delta\chi^{2}$ intervals. The CP-violating phase is constrained to $\delta_\mathrm{CP}=-1.97_{-0.70}^{+0.97}$ using Feldman--Cousins corrected intervals, and $\delta_\mathrm{CP}=0,\pi$ is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than $2\sigma$ credible level using a flat prior in $\delta_\mathrm{CP}$, and just below $2\sigma$ using a flat prior in $\sin\delta_\mathrm{CP}$. When the external constraint on $\sin^2\theta_{13}$ is removed, $\sin^2\theta_{13}=28.0^{+2.8}_{-6.5}\times10^{-3}$, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses. ",
keywords = "hep-ex",
author = "{The T2K Collaboration} and Ram{\'i}rez, {M. A.} and K. Abe and N. Akhlaq and R. Akutsu and Monsalve, {S. Alonso} 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 M. Barbi and Barker, {G. J.} and G. Barr and M. Batkiewicz-Kwasniak 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 S. Bordoni and A. Bravar and C. Bronner and S. Bron and A. Bubak and Avanzini, {M. Buizza} and Caballero, {J. A.} and Calabria, {N. F.} and D. Carabadjac and Catanesi, {M. G.} and A. Cervera and J. Chakrani and D. Cherdack and G. Christodoulou and T. Dealtry and Doyle, {T. A.} and Finch, {A. J.} and Kormos, {L. L.} and James, {M. Lamers} and M. Lawe and O'Keeffe, {H. M.} and Ratoff, {P. N.} and Speers, {A. J.} and Walsh, {J. G.}",
year = "2023",
month = sep,
day = "5",
doi = "10.1140/epjc/s10052-023-11819-x",
language = "English",
volume = "83",
journal = "European Physical Journal C",

}

RIS

TY - JOUR

T1 - Measurements of neutrino oscillation parameters from the T2K experiment using $3.6\times10^{21}$ protons on target

AU - The T2K Collaboration

AU - Ramírez, M. A.

AU - Abe, K.

AU - Akhlaq, N.

AU - Akutsu, R.

AU - Monsalve, S. Alonso

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 - Barbi, M.

AU - Barker, G. J.

AU - Barr, G.

AU - Batkiewicz-Kwasniak, M.

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 - Bordoni, S.

AU - Bravar, A.

AU - Bronner, C.

AU - Bron, S.

AU - Bubak, A.

AU - Avanzini, M. Buizza

AU - Caballero, J. A.

AU - Calabria, N. F.

AU - Carabadjac, D.

AU - Catanesi, M. G.

AU - Cervera, A.

AU - Chakrani, J.

AU - Cherdack, D.

AU - Christodoulou, G.

AU - Dealtry, T.

AU - Doyle, T. A.

AU - Finch, A. J.

AU - Kormos, L. L.

AU - James, M. Lamers

AU - Lawe, M.

AU - O'Keeffe, H. M.

AU - Ratoff, P. N.

AU - Speers, A. J.

AU - Walsh, J. G.

PY - 2023/9/5

Y1 - 2023/9/5

N2 - The T2K experiment presents new measurements of neutrino oscillation parameters using $19.7(16.3)\times10^{20}$ protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional $4.7\times10^{20}$ POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on $\sin^2\theta_{13}$ and the impact of priors on the $\delta_\mathrm{CP}$ measurement. Both analyses prefer the normal mass ordering and upper octant of $\sin^2\theta_{23}$ with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on $\sin^2\theta_{13}$ from reactors, $\sin^2\theta_{23}=0.561^{+0.021}_{-0.032}$ using Feldman--Cousins corrected intervals, and $\Delta{}m^2_{32}=2.494_{-0.058}^{+0.041}\times10^{-3}~\mathrm{eV^2}$ using constant $\Delta\chi^{2}$ intervals. The CP-violating phase is constrained to $\delta_\mathrm{CP}=-1.97_{-0.70}^{+0.97}$ using Feldman--Cousins corrected intervals, and $\delta_\mathrm{CP}=0,\pi$ is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than $2\sigma$ credible level using a flat prior in $\delta_\mathrm{CP}$, and just below $2\sigma$ using a flat prior in $\sin\delta_\mathrm{CP}$. When the external constraint on $\sin^2\theta_{13}$ is removed, $\sin^2\theta_{13}=28.0^{+2.8}_{-6.5}\times10^{-3}$, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.

AB - The T2K experiment presents new measurements of neutrino oscillation parameters using $19.7(16.3)\times10^{20}$ protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional $4.7\times10^{20}$ POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on $\sin^2\theta_{13}$ and the impact of priors on the $\delta_\mathrm{CP}$ measurement. Both analyses prefer the normal mass ordering and upper octant of $\sin^2\theta_{23}$ with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on $\sin^2\theta_{13}$ from reactors, $\sin^2\theta_{23}=0.561^{+0.021}_{-0.032}$ using Feldman--Cousins corrected intervals, and $\Delta{}m^2_{32}=2.494_{-0.058}^{+0.041}\times10^{-3}~\mathrm{eV^2}$ using constant $\Delta\chi^{2}$ intervals. The CP-violating phase is constrained to $\delta_\mathrm{CP}=-1.97_{-0.70}^{+0.97}$ using Feldman--Cousins corrected intervals, and $\delta_\mathrm{CP}=0,\pi$ is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than $2\sigma$ credible level using a flat prior in $\delta_\mathrm{CP}$, and just below $2\sigma$ using a flat prior in $\sin\delta_\mathrm{CP}$. When the external constraint on $\sin^2\theta_{13}$ is removed, $\sin^2\theta_{13}=28.0^{+2.8}_{-6.5}\times10^{-3}$, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.

KW - hep-ex

U2 - 10.1140/epjc/s10052-023-11819-x

DO - 10.1140/epjc/s10052-023-11819-x

M3 - Journal article

VL - 83

JO - European Physical Journal C

JF - European Physical Journal C

M1 - 782

ER -