Measurements of neutrino oscillation parameters from the T2K experiment using 3.6 x 1021 protons on target
K. Abe,N. Akhlaq,R. Akutsu,A. Ali,S. Alonso Monsalve,C. Alt,C. Andreopoulos,M. Antonova,S. Aoki,T. Arihara,Y. Asada,Y. Ashida,E. T. Atkin,M. Barbi,G. J. Barker,G. Barr,D. Barrow,M. Batkiewicz-Kwasniak,F. Bench,V. Berardi,L. Berns,S. Bhadra,A. Blanchet,A. Blondel,S. Bolognesi,T. Bonus,S. Bordoni,S. B. Boyd,A. Bravar,C. Bronner,S. Bron,A. Bubak,M. Buizza Avanzini,J. A. Caballero,N. F. Calabria,S. Cao,D. Carabadjac,A. J. Carter,S. L. Cartwright,M. G. Catanesi,A. Cervera,J. Chakrani,D. Cherdack,P. S. Chong,G. Christodoulou,A. Chvirova,M. Cicerchia,J. Coleman,G. Collazuol,L. Cook,A. Cudd,C. Dalmazzone,T. Daret,Yu. I. Davydov,A. De Roeck,G. De Rosa,T. Dealtry,C. C. Delogu,C. Densham,A. Dergacheva,F. Di Lodovico,S. Dolan,D. Douqa,T. A. Doyle,O. Drapier,J. Dumarchez,P. Dunne,K. Dygnarowicz,A. Eguchi,S. Emery-Schrenk,G. Erofeev,A. Ershova,G. Eurin,D. Fedorova,S. Fedotov,M. Feltre,A. J. Finch,G. A. Fiorentini Aguirre,G. Fiorillo,M. D. Fitton,J. M. Franco Patino,M. Friend,Y. Fujii,Y. Fukuda,K. Fusshoeller,L. Giannessi,C. Giganti,V. Glagolev,M. Gonin,J. Gonzalez Rosa,E. A. G. Goodman,A. Gorin,M. Grassi,M. Guigue,D. R. Hadley,J. T. Haigh,P. Hamacher-Baumann,D. A. Harris,M. Hartz,T. Hasegawa,S. Hassani,N. C. Hastings,Y. Hayato,D. Henaff,A. Hiramoto,M. Hogan,J. Holeczek,A. Holin,T. Holvey,N. T. Hong Van,T. Honjo,F. Iacob,A. K. Ichikawa,M. Ikeda,T. Ishida,M. Ishitsuka,H. T. Israel,K. Iwamoto,A. Izmaylov,N. Izumi,M. Jakkapu,B. Jamieson,S. J. Jenkins,C. Jesus-Valls,J. J. Jiang,P. Jonsson,S. Joshi,C. K. Jung,P. B. Jurj,M. Kabirnezhad,A. C. Kaboth,T. Kajita,H. Kakuno,J. Kameda,S. P. Kasetti,Y. Kataoka,Y. Katayama,T. Katori,M. Kawaue,E. Kearns,M. Khabibullin,A. Khotjantsev,T. Kikawa,H. Kikutani,S. King,V. Kiseeva,J. Kisiel,T. Kobata,H. Kobayashi,T. Kobayashi,L. Koch,S. Kodama,A. Konaka,L. L. Kormos,Y. Koshio,A. Kostin,T. Koto,K. Kowalik,Y. Kudenko,Y. Kudo,S. Kuribayashi,R. Kurjata,T. Kutter,M. Kuze,M. La Commara,L. Labarga,K. Lachner,J. Lagoda,S. M. Lakshmi,M. Lamers James,M. Lamoureux,A. Langella,J. -F. Laporte,D. Last,N. Latham,M. Laveder,L. Lavitola,M. Lawe,Y. Lee,C. Lin,S. -K. Lin,R. P. Litchfield,S. L. Liu,W. Li,A. Longhin,K. R. Long,A. Lopez Moreno,L. Ludovici,X. Lu,T. Lux,L. N. Machado,L. Magaletti,K. Mahn,M. Malek,M. Mandal,S. Manly,A. D. Marino,L. Marti-Magro,D. G. R. Martin,M. Martini,J. F. Martin,T. Maruyama,T. Matsubara,V. Matveev,C. Mauger,K. Mavrokoridis,E. Mazzucato,N. McCauley,J. McElwee,K. S. McFarland,C. McGrew,J. McKean,A. Mefodiev,G. D. Megias,P. Mehta,L. Mellet,C. Metelko,M. Mezzetto,E. Miller,A. Minamino,O. Mineev,S. Mine,M. Miura,L. Molina Bueno,S. Moriyama,S. Moriyama,P. Morrison,Th. A. Mueller,D. Munford,L. Munteanu,K. Nagai,Y. Nagai,T. Nakadaira,K. Nakagiri,M. Nakahata,Y. Nakajima,A. Nakamura,H. Nakamura,K. Nakamura,K. D. Nakamura,Y. Nakano,S. Nakayama,T. Nakaya,K. Nakayoshi,C. E. R. Naseby,T. V. Ngoc,V. Q. Nguyen,K. Niewczas,S. Nishimori,Y. Nishimura,K. Nishizaki,T. Nosek,F. Nova,P. Novella,J. C. Nugent,H. M. O'Keeffe,L. O'Sullivan,T. Odagawa,T. Ogawa,R. Okada,W. Okinaga,K. Okumura,T. Okusawa,N. Ospina,R. A. Owen,Y. Oyama,V. Palladino,V. Paolone,M. Pari,J. Parlone,S. Parsa,J. Pasternak,M. Pavin,D. Payne,G. C. Penn,D. Pershey,L. Pickering,C. Pidcott,G. Pintaudi,C. Pistillo,B. Popov,K. Porwit,M. Posiadala-Zezula,Y. S. Prabhu,F. Pupilli,B. Quilain,T. Radermacher,E. Radicioni,B. Radics,M. A. Ramirez,P. N. Ratoff,M. Reh,C. Riccio,E. Rondio,S. Roth,N. Roy,A. Rubbia,A. C. Ruggeri,C. A. Ruggles,A. Rychter,K. Sakashita,F. Sanchez,G. Santucci,C. M. Schloesser,K. Scholberg,M. Scott,Y. Seiya,T. Sekiguchi,H. Sekiya,D. Sgalaberna,A. Shaikhiev,F. Shaker,A. Shaykina,M. Shiozawa,W. Shorrock,A. Shvartsman,N. Skrobova,K. Skwarczynski,D. Smyczek,M. Smy,J. T. Sobczyk,H. Sobel,F. J. P. Soler,Y. Sonoda,A. J. Speers,R. Spina,I. A. Suslov,S. Suvorov,A. Suzuki,S. Y. Suzuki,Y. Suzuki,A. A. Sztuc,M. Tada,S. Tairafune,S. Takayasu,A. Takeda,Y. Takeuchi,K. Takifuji,H. K. Tanaka,Y. Tanihara,M. Tani,A. Teklu,V. V. Tereshchenko,N. Teshima,N. Thamm,L. F. Thompson,W. Toki,C. Touramanis,T. Towstego,K. M. Tsui,T. Tsukamoto,M. Tzanov,Y. Uchida,M. Vagins,D. Vargas,M. Varghese,G. Vasseur,C. Vilela,E. Villa,W. G. S. Vinning,U. Virginet,T. Vladisavljevic,T. Wachala,J. G. Walsh,Y. Wang,L. Wan,D. Wark,M. O. Wascko,A. Weber,R. Wendell,M. J. Wilking,C. Wilkinson,J. R. Wilson,K. Wood,C. Wret,J. Xia,Y. -H. Xu,K. Yamamoto,T. Yamamoto,C. Yanagisawa,G. Yang,T. Yano,K. Yasutome,N. Yershov,U. Yevarouskaya,M. Yokoyama,Y. Yoshimoto,N. Yoshimura,M. Yu,R. Zaki,A. Zalewska,J. Zalipska,K. Zaremba,G. Zarnecki,X. Zhao,T. Zhu,M. Ziembicki,E. D. Zimmerman,M. Zito,S. Zsoldos
EUROPEAN PHYSICAL JOURNAL C（2023）
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摘要
The T2K experiment presents new measurements of neutrino oscillation parameters using 19.7(16.3) x 10(20) protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional 4.7 x 10(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(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(-0.032)(+0.021) using Feldman-Cousins corrected intervals, and Delta m(32)(2) = 2.494(-0.058)(+0.041) x 10(-3) eV(2) using constant Delta chi(2) intervals. The CP-violating phase is constrained to delta(CP) = -1.97(-0.70)(+0.97) using Feldman-Cousins corrected intervals, and delta(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(CP), and just below 2 sigma using a flat prior in sin delta(CP). When the external constraint on sin(2) nu(13) is removed, sin(2) theta(13) = 28.0(-6.5)(+2.8) x 10(-3), in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
