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Measurements of neutrino oscillation parameters from the T2K experiment using 3.6×1021 protons on target.
Abe, K; Akhlaq, N; Akutsu, R; Ali, A; Alonso Monsalve, S; Alt, C; Andreopoulos, C; Antonova, M; Aoki, S; Arihara, T; Asada, Y; Ashida, Y; Atkin, E T; Barbi, M; Barker, G J; Barr, G; Barrow, D; Batkiewicz-Kwasniak, M; Bench, F; Berardi, V; Berns, L; Bhadra, S; Blanchet, A; Blondel, A; Bolognesi, S; Bonus, T; Bordoni, S; Boyd, S B; Bravar, A; Bronner, C; Bron, S; Bubak, A; Buizza Avanzini, M; Caballero, J A; Calabria, N F; Cao, S; Carabadjac, D; Carter, A J; Cartwright, S L; Catanesi, M G; Cervera, A; Chakrani, J; Cherdack, D; Chong, P S; Christodoulou, G; Chvirova, A; Cicerchia, M; Coleman, J; Collazuol, G; Cook, L.
Afiliação
  • Abe K; Kamioka Observatory, Institute for Cosmic Ray Research, University of Tokyo, Kamioka, Japan.
  • Akhlaq N; School of Physics and Astronomy, Queen Mary University of London, London, UK.
  • Akutsu R; High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki Japan.
  • Ali A; TRIUMF, Vancouver, BC Canada.
  • Alonso Monsalve S; Department of Physics, University of Winnipeg, Winnipeg, MB Canada.
  • Alt C; Institute for Particle Physics and Astrophysics, ETH Zurich, Zurich, Switzerland.
  • Andreopoulos C; Institute for Particle Physics and Astrophysics, ETH Zurich, Zurich, Switzerland.
  • Antonova M; Department of Physics, University of Liverpool, Liverpool, UK.
  • Aoki S; IFIC (CSIC and University of Valencia), Valencia, Spain.
  • Arihara T; Kobe University, Kobe, Japan.
  • Asada Y; Department of Physics, Tokyo Metropolitan University, Tokyo, Japan.
  • Ashida Y; Department of Physics, Yokohama National University, Yokohama, Japan.
  • Atkin ET; Department of Physics, Kyoto University, Kyoto, Japan.
  • Barbi M; Department of Physics, Imperial College London, London, UK.
  • Barker GJ; Department of Physics, University of Regina, Regina, Saskatchewan Canada.
  • Barr G; Department of Physics, University of Warwick, Coventry, UK.
  • Barrow D; Department of Physics, Oxford University, Oxford, UK.
  • Batkiewicz-Kwasniak M; Department of Physics, Oxford University, Oxford, UK.
  • Bench F; H. Niewodniczanski Institute of Nuclear Physics PAN, Cracow, Poland.
  • Berardi V; Department of Physics, University of Liverpool, Liverpool, UK.
  • Berns L; Dipartimento Interuniversitario di Fisica, INFN Sezione di Bari and Università e Politecnico di Bari, Bari, Italy.
  • Bhadra S; Department of Physics, Faculty of Science, Tohoku University, Sendai, Miyagi Japan.
  • Blanchet A; Department of Physics and Astronomy, York University, Toronto, ON Canada.
  • Blondel A; Section de Physique, DPNC, University of Geneva, Geneva, Switzerland.
  • Bolognesi S; Section de Physique, DPNC, University of Geneva, Geneva, Switzerland.
  • Bonus T; Laboratoire de Physique Nucléaire et de Hautes Energies (LPNHE), Sorbonne Université, Université Paris Diderot, CNRS/IN2P3, Paris, France.
  • Bordoni S; IRFU, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France.
  • Boyd SB; Faculty of Physics and Astronomy, Wroclaw University, Wroclaw, Poland.
  • Bravar A; Section de Physique, DPNC, University of Geneva, Geneva, Switzerland.
  • Bronner C; Department of Physics, University of Warwick, Coventry, UK.
  • Bron S; Section de Physique, DPNC, University of Geneva, Geneva, Switzerland.
  • Bubak A; Kamioka Observatory, Institute for Cosmic Ray Research, University of Tokyo, Kamioka, Japan.
  • Buizza Avanzini M; TRIUMF, Vancouver, BC Canada.
  • Caballero JA; Institute of Physics, University of Silesia, Katowice, Poland.
  • Calabria NF; Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France.
  • Cao S; Departamento de Física Atómica, Molecular y Nuclear, Universidad de Sevilla, 41080 Sevilla, Spain.
  • Carabadjac D; Dipartimento Interuniversitario di Fisica, INFN Sezione di Bari and Università e Politecnico di Bari, Bari, Italy.
  • Carter AJ; Institute For Interdisciplinary Research in Science and Education (IFIRSE), ICISE, Quy Nhon, Vietnam.
  • Cartwright SL; Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France.
  • Catanesi MG; Université Paris-Saclay, Gif-sur-Yvette, France.
  • Cervera A; Department of Physics, Royal Holloway University of London, Egham, Surrey UK.
  • Chakrani J; Department of Physics and Astronomy, University of Sheffield, Sheffield, UK.
  • Cherdack D; Dipartimento Interuniversitario di Fisica, INFN Sezione di Bari and Università e Politecnico di Bari, Bari, Italy.
  • Chong PS; IFIC (CSIC and University of Valencia), Valencia, Spain.
  • Christodoulou G; Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France.
  • Chvirova A; Department of Physics, University of Houston, Houston, TX USA.
  • Cicerchia M; Department of Physics and Astronomy, University of Pennsylvania, Philadelphia, PA 19104 USA.
  • Coleman J; CERN European Organization for Nuclear Research, 1211 Geneva 23, Switzerland.
  • Collazuol G; Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia.
  • Cook L; Dipartimento di Fisica, INFN Sezione di Padova and Università di Padova, Padua, Italy.
Eur Phys J C Part Fields ; 83(9): 782, 2023.
Article em En | MEDLINE | ID: mdl-37680254
ABSTRACT
The T2K experiment presents new measurements of neutrino oscillation parameters using 19.7(16.3)×1020 protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional 4.7×1020 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 sin2θ13 and the impact of priors on the δCP measurement. Both analyses prefer the normal mass ordering and upper octant of sin2θ23 with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on sin2θ13 from reactors, sin2θ23=0.561-0.032+0.021 using Feldman-Cousins corrected intervals, and Δm322=2.494-0.058+0.041×10-3eV2 using constant Δχ2 intervals. The CP-violating phase is constrained to δCP=-1.97-0.70+0.97 using Feldman-Cousins corrected intervals, and δCP=0,π is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than 2σ credible level using a flat prior in δCP, and just below 2σ using a flat prior in sinδCP. When the external constraint on sin2θ13 is removed, sin2θ13=28.0-6.5+2.8×10-3, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article