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Neutrino Oscillation Physics Potential of the T2K Experiment

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arxiv 1409.7469 v2 pith:OYHG4KEW submitted 2014-09-26 hep-ex

Neutrino Oscillation Physics Potential of the T2K Experiment

K.Abe , J.Adam , H.Aihara , T.Akiri , C.Andreopoulos , S.Aoki , A.Ariga , S.Assylbekov
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D.Autiero M.Barbi G.J.Barker G.Barr P.Bartet-Friburg M.Bass M.Batkiewicz F.Bay V.Berardi B.E.Berger S.Berkman S.Bhadra F.d.M.Blaszczyk A.Blondel C.Bojechko S.Bordoni S.B.Boyd D.Brailsford A.Bravar C.Bronner N.Buchanan R.G.Calland J.Caravaca Rodr'iguez S.L.Cartwright R.Castillo M.G.Catanesi A.Cervera D.Cherdack G.Christodoulou A.Clifton J.Coleman S.J.Coleman G.Collazuol K.Connolly L.Cremonesi A.Dabrowska I.Danko R.Das S.Davis P.de Perio G.De Rosa T.Dealtry S.R.Dennis C.Densham D.Dewhurst F.Di Lodovico S.Di Luise O.Drapier T.Duboyski K.Duffy J.Dumarchez S.Dytman M.Dziewiecki S.Emery-Schrenk A.Ereditato L.Escudero T.Feusels A.J.Finch G.A.Fiorentini M.Friend Y.Fujii Y.Fukuda A.P.Furmanski V.Galymov A.Garcia S.Giffin C.Giganti K.Gilje D.Goeldi T.Golan M.Gonin N.Grant D.Gudin D.R.Hadley L.Haegel A.Haesler M.D.Haigh P.Hamilton D.Hansen T.Hara M.Hartz T.Hasegawa N.C.Hastings T.Hayashino Y.Hayato C.Hearty R.L.Helmer M.Hierholzer J.Hignight A.Hillairet A.Himmel T.Hiraki S.Hirota J.Holeczek S.Horikawa K.Huang A.K.Ichikawa K.Ieki M.Ieva M.Ikeda J.Imber J.Insler T.J.Irvine T.Ishida T.Ishii E.Iwai K.Iwamoto K.Iyogi A.Izmaylov A.Jacob B.Jamieson R.A.Johnson S.Johnson J.H.Jo P.Jonsson C.K.Jung M.Kabirnezhad A.C.Kaboth T.Kajita H.Kakuno J.Kameda Y.Kanazawa D.Karlen I.Karpikov T.Katori E.Kearns M.Khabibullin A.Khotjantsev D.Kielczewska T.Kikawa A.Kilinski J.Kim S.King J.Kisiel P.Kitching T.Kobayashi L.Koch T.Koga A.Kolaceke A.Konaka L.L.Kormos A.Korzenev Y.Koshio W.Kropp H.Kubo Y.Kudenko R.Kurjata T.Kutter J.Lagoda K.Laihem I.Lamont E.Larkin M.Laveder M.Lawe M.Lazos T.Lindner C.Lister R.P.Litchfield A.Longhin J.P.Lopez L.Ludovici L.Magaletti K.Mahn M.Malek S.Manly A.D.Marino J.Marteau J.F.Martin P.Martins S.Martynenko T.Maruyama V.Matveev K.Mavrokoridis E.Mazzucato M.McCarthy N.McCauley K.S.McFarland C.McGrew A.Mefodiev C.Metelko M.Mezzetto P.Mijakowski C.A.Miller A.Minamino O.Mineev A.Missert M.Miura S.Moriyama Th.A.Mueller A.Murakami M.Murdoch S.Murphy J.Myslik T.Nakadaira M.Nakahata K.G.Nakamura K.Nakamura S.Nakayama T.Nakaya K.Nakayoshi C.Nantais C.Nielsen M.Nirkko K.Nishikawa Y.Nishimura J.Nowak H.M.O'Keeffe R.Ohta K.Okumura T.Okusawa W.Oryszczak S.M.Oser T.Ovsyannikova R.A.Owen Y.Oyama V.Palladino J.L.Palomino V.Paolone D.Payne O.Perevozchikov J.D.Perkin Y.Petrov L.Pickard E.S.Pinzon Guerra C.Pistillo P.Plonski E.Poplawska B.Popov M.Posiadala-Zezula J.-M.Poutissou R.Poutissou P.Przewlocki B.Quilain E.Radicioni P.N.Ratoff M.Ravonel M.A.M.Rayner A.Redij M.Reeves E.Reinherz-Aronis C.Riccio P.A.Rodrigues P.Rojas E.Rondio S.Roth A.Rubbia D.Ruterbories R.Sacco K.Sakashita F.S'anchez F.Sato E.Scantamburlo K.Scholberg S.Schoppmann J.Schwehr M.Scott Y.Seiya T.Sekiguchi H.Sekiya D.Sgalaberna R.Shah F.Shaker M.Shiozawa S.Short Y.Shustrov P.Sinclair B.Smith M.Smy J.T.Sobczyk H.Sobel M.Sorel L.Southwell P.Stamoulis J.Steinmann B.Still Y.Suda A.Suzuki K.Suzuki S.Y.Suzuki Y.Suzuki R.Tacik M.Tada S.Takahashi A.Takeda Y.Takeuchi H.K.Tanaka H.A.Tanaka M.M.Tanaka D.Terhorst R.Terri L.F.Thompson A.Thorley S.Tobayama W.Toki T.Tomura Y.Totsuka C.Touramanis T.Tsukamoto M.Tzanov Y.Uchida A.Vacheret M.Vagins G.Vasseur T.Wachala A.V.Waldron K.Wakamatsu C.W.Walter D.Wark W.Warzycha M.O.Wascko A.Weber R.Wendell R.J.Wilkes M.J.Wilking C.Wilkinson Z.Williamson J.R.Wilson R.J.Wilson T.Wongjirad Y.Yamada K.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.Zmuda
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classification hep-ex
keywords deltathetacircneutrinoexperimenthierarchymodeoscillation
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle $\theta_{13}$ have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP violation in neutrinos, non-maximal $\sin^22\theta_{23}$, the octant of $\theta_{23}$, and the mass hierarchy, in addition to the measurements of $\delta_{CP}$, $\sin^2\theta_{23}$, and $\Delta m^2_{32}$, for various combinations of $\nu$-mode and \(\bar{\nu}\)-mode data-taking. With an exposure of $7.8\times10^{21}$~protons-on-target, T2K can achieve 1-$\sigma$ resolution of 0.050(0.054) on $\sin^2\theta_{23}$ and $0.040(0.045)\times10^{-3}~\rm{eV}^2$ on $\Delta m^2_{32}$ for 100\%(50\%) neutrino beam mode running assuming $\sin^2\theta_{23}=0.5$ and $\Delta m^2_{32} = 2.4\times10^{-3}$ eV$^2$. T2K will have sensitivity to the CP-violating phase $\delta_{\rm{CP}}$ at 90\% C.L. or better over a significant range. For example, if $\sin^22\theta_{23}$ is maximal (i.e $\theta_{23}$=$45^\circ$) the range is $-115^\circ<\delta_{\rm{CP}}<-60^\circ$ for normal hierarchy and $+50^\circ<\delta_{\rm{CP}}<+130^\circ$ for inverted hierarchy. When T2K data is combined with data from the NO$\nu$A experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero $\delta_{CP}$ is substantially increased compared to if each experiment is analyzed alone.

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