Updated T2k Measurements Of Muon Neutrino And Antineutrino Disappearance Using 1.5 X 10(21) Protons On Target

K. Abe,J. Amey,C. Andreopoulos,M. Antonova,S. Aoki,A. Ariga,Y. Ashida,D. Autiero,S. Ban,M. Barbi,G. J. Barker,G. Barr,C. Barry,P. Bartet-Friburg,M. Batkiewicz,V. Berardi,S. Berkman,S. Bhadra,S. Bienstock,A. Blondel,S. Bolognesi,S. Bordoni,S. Boyd,D. Brailsford,A. Bravar,C. Bronner,M. Buizza Avanzini,R. G. Calland,T. Campbell,S. V. Cao,S. Cartwright,M. G. Catanesi,A. Cervera,A. Chappell,C. Checchia,D. Cherdack,N. Chikuma,G. Christodoulou,A. Clifton,J. Coleman,G. Collazuol,D. Coplowe,A. Cudd,A. Dabrowska,G. De Rosa,T. Dealtry,P. F. Denner,S. R. Dennis,C. Densham,D. Dewhurst,F. Di Lodovico,S. Dolan,O. Drapier,K. Duffy,J. Dumarchez,P. Dunne,M. Dziewiecki,S. Emery-Schrenk,A. Ereditato,T. Feusels,A.J. Finch,G. A. Fiorentini,M. Friend,Y. Fujii,David H. Fukuda,Y. Fukuda,V. Galymov,A. Garcia,C. Giganti,F. Gizzarelli,T. Golan,M. Gonin,D. R. Hadley,L. Haegel,J. T. Haigh,D. Hansen,J. Harada,M. Hartz,T. Hasegawa,N.C. Hastings,T. Hayashino,Y. Hayato,R. L. Helmer,A. Hillairet,T. Hiraki,A. Hiramoto,S. Hirota,M. Hogan,J. Holeczek,F. Hosomi,K. Huang,A. Ichikawa,M. Ikeda,J. Imber,J. Insler,R. A. Intonti,T. Ishida,T. Ishii,E. Iwai,K. Iwamoto,A. Izmaylov,B. Jamieson,M. Jiang,S. Johnson,P. Jonsson,C. K. Jung,M. Kabirnezhad,A. Kaboth,T. Kajita,H. Kakuno,J. Kameda,D. Karlen,T. Katori,E. Kearns,M. Khabibullin,A. Khotjantsev,H. S. Kim,J. Kim,S. King,J. Kisiel,A. Knight,A. Knox,T. Kobayashi,L. Koch,T. Koga,P. P. Koller,A. Konaka,L. L. Kormos,A. Korzenev,Y. Koshio,K. Kowalik,W. R. Kropp,Y. Kudenko,R. Kurjata,T. Kutter,J. Lagoda,I. Lamont,M. Lamoureux,E. Larkin,P. Lasorak,M. Laveder,M. Lawe,M. Licciardi,T. Lindner,Z. J. Liptak,R. P. Litchfield,X. N. Li,A. Longhin,J. P. Lopez,T. Lou,L. Ludovici,X. Lu,L. Magaletti,K. B. M. Mahn,M. Malek,S. Manly,L. Maret,A. D. Marino,J. F. Martin,P. Martins,S. Martynenko,T. Maruyama,V. Matveev,K. Mavrokoridis,Ma W. Y.,E. Mazzucato,M. McCarthy,N. McCauley,K. S. McFarland,C. McGrew,A. Mefodiev,C. Metelko,M. Mezzetto,P. Mijakowski,A. Minamino,O. Mineev,S. Mine,A. Missert,M. Miura,S. Moriyama,J. Morrison,Th. Mueller,J. Myslik,T. Nakadaira,M. Nakahata,K. G. Nakamura,K. Nakamura,Y. Nakanishi,S. Nakayama,T. Nakaya,K. Nakayoshi,C. Nantais,C. Nielsen,M. Nirkko,K. Nishikawa,Y. Nishimura,P. Novella,J. Nowak,H. M. O’Keeffe,K. Okumura,T. Okusawa,W. Oryszczak,S. M. Oser,T. Ovsyannikova,R. A. Owen,Y. Oyama,V. Palladino,J. L. Palomino,V. Paolone,N. D. Patel,P. Paudyal,M. Pavin,D. Payne,J. D. Perkin,Y. Petrov,L. Pickard,L. Pickering,E. S. Pinzon Guerra,C. Pistillo,B. Popov,M. Posiadala-Zezula,J.-M. Poutissou,R. Poutissou,A. Pritchard,P. Przewlocki,B. Quilain,T. Radermacher,E. Radicioni,P. N. Ratoff,M. Ravonel,M. A. Rayner,A. Redij,E. Reinherz-Aronis,C. Riccio,E. Rondio,B. Rossi,S. Roth,A. Rubbia,A. C. Ruggeri,A. Rychter,K. Sakashita,Francisca Javiela Munoz Sanchez,E. Scantamburlo,K. Scholberg,J. Schwehr,M. Scott,Y. Seiya,T. Sekiguchi,H. Sekiya,D. Sgalaberna,R. Shah,A. Shaikhiev,F. Shaker,D. Shaw,M. Shiozawa,T. Shirahige,S. Short,M. Smy,J. Sobczyk,H. W. Sobel,M. Sorel,L. Southwell,J. Steinmann,T. Stewart,P. Stowell,Y. Suda,S. Suvorov,A. Suzuki,S. Suzuki,Y. Suzuki,R. Tacik,M. Tada,A. Takeda,Y. Takeuchi,R. Tamura,H. Tanaka,H. A. Tanaka,D. Terhorst,R. Terri,T. Thakore,L.F. Thompson,S. Tobayama,W. H. Toki,T. Tomura,C. Touramanis,T. Tsukamoto,M. Tzanov,Y. Uchida,M. Vagins,Z. Vallari,G. Vasseur,C. Vilela,T. Vladisavljevic,T. Wachala,C. W. Walter,D. Wark,M. O. Wascko,A. Weber,R. Wendell,R. J. Wilkes,M. J. Wilking,C. Wilkinson,J. R. Wilson,R. J. Wilson,C. Wret,Y. Yamada,Kazuhiro Yamamoto,M. Yamamoto,C. Yanagisawa,T. Yano,S. Yen,N. Yershov,M. Yokoyama,K. Yoshida,T. Yuan,M. Yu,A. Zalewska,J. Zalipska,L. Zambelli,K. Zaremba,M. Ziembicki,E. D. Zimmerman,M. Zito, Żmuda

PHYSICAL REVIEW D(2017)

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摘要
We report measurements by the T2K experiment of the parameters theta(23) and Delta m(32)(2) governing the disappearance of muon neutrinos and antineutrinos in the three-flavor neutrino oscillation model. Utilizing the ability of the experiment to run with either a mainly neutrino or a mainly antineutrino beam, the parameters are measured separately for neutrinos and antineutrinos. Using 7.482 x 10(20) POT in neutrino running mode and 7.471 x 10(20) POT in antineutrino mode, T2K obtained sin(2) (theta(23)) = 0.51(-0.07)(+0.08) and Delta (m) over bar (2)(32) = (+0.15)(-2.53) -0.13 x 10(-3) eV(2)/c(4) for neutrinos, and sin(2) ((theta) over bar (23)) = 0.42(-0.07)(+0.25) and Delta(m) over bar (2)(32) = 2.55(-0.27)(+0.33) x 10(-3) eV(2)/c(4) for antineutrinos (assuming normal mass ordering). No significant differences between the values of the parameters describing the disappearance of muon neutrinos and antineutrinos were observed.
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关键词
antineutrino disappearance,muon neutrino,protons
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