T2K measurements of muon neutrino and antineutrino disappearance using $3.13\times 10^{21}$ protons on target

Phys. Rev. D 103, 011101 (2021) We report measurements by the T2K experiment of the parameters $\theta_{23}$ and $\Delta m^2_{32}$ which govern the disappearance of muon neutrinos and antineutrinos in the three-flavor PMNS neutrino oscillation model at T2K's neutrino energy and propagation dist...

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Hauptverfasser: Abe, K, Alt, C, Antonova, M, Ashida, Y, Atkin, E. T, Awataguchi, Y, Barr, G, Beloshapkin, A, Bourguille, B, BravoBerguno, D, Bronner, C, Cartwright, S. L, Catanesi, M. G, Christodoulou, G, Coleman, J, Coplowe, D, Cudd, A, DeRosa, G, Delogu, C. C, Dennis, S. R, DiLodovico, F, Doyle, T. A, Francois, C, Friend, M, Fukuda, R, Guigue, M, Hadley, D. R, Hamacher-Baumann, P, HongVan, N. T, Ishitsuka, M, Izumi, N, Jamieson, B, Jesus-Valls, C, Jonsson, P, Jurj, P. B, De Rosa, G, Dergacheva, A, Di Lodovico, F, Van, N. T. Hong, Katayama, Y, Khabibullin, M, Kobata, T, Koch, L, Kostin, A, Lagoda, J, Lamoureux, M, Lawe, M, Lux, T, Manly, S, Maret, L, Maruyama, T, McGrew, C, Mineev, O, Mueller, Th. A, Nakahata, M, Nakano, Y, Nakayama, S, Niewczas, K, Nova, F, Nowak, J, O'Keeffe, H. M, Odagawa, T, Pasternak, J, Penn, G. C, Pickering, L, Pidcott, C, Pintaudi, G, Pistillo, C, Porwit, K, Radermacher, T, Radicioni, E, Ratoff, P. N, Rychter, A, Sakashita, K, Santucci, G, Scholberg, K, Scott, M, Sekiguchi, T, Shaykina, A, Shiozawa, M, Shvartsman, A, Skwarczynski, K, Sobczyk, J. T, Soler, F. J. P, Suzuki, A, Takeda, A, Towstego, T, Tzanov, M, Valder, S, Vasseur, G, Walker, J, Walsh, J. G, Wendell, R, Wilking, M. J, Xia, J, Yano, T, Yershov, N, Yoshimoto, Y, Zarnecki, G, Zito, M
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Zusammenfassung:Phys. Rev. D 103, 011101 (2021) We report measurements by the T2K experiment of the parameters $\theta_{23}$ and $\Delta m^2_{32}$ which govern the disappearance of muon neutrinos and antineutrinos in the three-flavor PMNS neutrino oscillation model at T2K's neutrino energy and propagation distance. Utilizing the ability of the experiment to run with either a mainly neutrino or a mainly antineutrino beam, muon-like events from each beam mode are used to measure these parameters separately for neutrino and antineutrino oscillations. Data taken from $1.49 \times 10^{21}$ protons on target (POT) in neutrino mode and $1.64 \times 10^{21}$ POT in antineutrino mode are used. The best-fit values obtained by T2K were $\sin^2\left(\theta_{23}\right)=0.51^{+0.06}_{-0.07} \left(0.43^{+0.21}_{-0.05}\right)$ and $\Delta m^2_{32}=2.47^{+0.08}_{-0.09} \left(2.50^{+0.18}_{-0.13}\right)$\evmass for neutrinos (antineutrinos). No significant differences between the values of the parameters describing the disappearance of muon neutrinos and antineutrinos were observed. An analysis using an effective two-flavor neutrino oscillation model where the sine of the mixing angle is allowed to take non-physical values larger than 1 is also performed to check the consistency of our data with the three-flavor model. Our data were found to be consistent with a physical value for the mixing angle.
DOI:10.48550/arxiv.2008.07921