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Updated T2K measurements of muon neutrino and antineutrino disappearance using 1.5e21 protons on target

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arxiv 1704.06409 v2 pith:VDVJK4ET submitted 2017-04-21 hep-ex

K. Abe , J. Amey , C. Andreopoulos , M. Antonova , S. Aoki , A. Ariga , Y. Ashida , D. Autiero
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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.B. Boyd D. Brailsford A. Bravar C. Bronner M. Buizza Avanzini R.G. Calland T. Campbell S. Cao S.L. 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.E. Duffy J. Dumarchez P. Dunne M. Dziewiecki S. Emery-Schrenk A. Ereditato T. Feusels A.J. Finch G.A. Fiorentini M. Friend Y. Fujii D. 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.K. 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.C. Kaboth T. Kajita H. Kakuno J. Kameda D. Karlen T. Katori E. Kearns M. Khabibullin A. Khotjantsev H. 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. 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. Li A. Longhin J.P. Lopez T. Lou L. Ludovici X. Lu L. Magaletti K. Mahn M. Malek S. Manly L. Maret A.D. Marino J.F. Martin P. Martins S. Martynenko T. Maruyama V. Matveev K. Mavrokoridis W.Y. Ma 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.A. Mueller J. Myslik T. Nakadaira M. Nakahata K.G. Nakamura K. Nakamura K.D. 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 F. Sánchez 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.T. Sobczyk H. Sobel M. Sorel L. Southwell J. Steinmann T. Stewart P. Stowell Y. Suda S. Suvorov A. Suzuki S.Y. Suzuki Y. Suzuki R. Tacik M. Tada A. Takeda Y. Takeuchi R. Tamura H.K. Tanaka H.A. Tanaka D. Terhorst R. Terri T. Thakore L.F. Thompson S. Tobayama W. 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 K. 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 J. Żmuda
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classification hep-ex
keywords antineutrinosneutrinoneutrinostimesantineutrinodeltadisappearancemuon
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abstract

We report measurements by the T2K experiment of the parameters $\theta_{23}$ and $\Delta m^{2}_{32}$ 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 $7.482 \times 10^{20}$ POT in neutrino running mode and $7.471 \times 10^{20}$ POT in antineutrino mode, T2K obtained, $\sin^{2}(\theta_{23})=0.51^{+0.08}_{-0.07}$ and $\Delta m^{2}_{32} = 2.53^{+0.15}_{-0.13} \times 10^{-3}$eV$^{2}$/c$^{4}$ for neutrinos, and $\sin^{2}({\overline{\theta}}_{23})=0.42^{+0.25}_{-0.07}$ and ${\Delta\overline{m}^2}_{32} = 2.55^{+0.33}_{-0.27} \times 10^{-3}$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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