Neutrino oscillation physics potential of the T2K experiment

@article{KAbe2014NeutrinoOP,
  title={Neutrino oscillation physics potential of the T2K experiment},
  author={K.Abe and J.Adam and H.Aihara and T.Akiri and C.Andreopoulos and S.Aoki and A.Ariga and S.Assylbekov and D.Autiero and M.Barbi and G.J.Barker and G.Barr and P.Bartet-Friburg and M.Bass and M.Batkiewicz and F.Bay and V.Berardi and B.E.Berger and S.Berkman and S.Bhadra and F.d.M.Blaszczyk and A.Blondel and C.Bojechko and S.Bordoni and S.B.Boyd and D.Brailsford and A.Bravar and C.Bronner and N.Buchanan and R.G.Calland and J.Caravaca Rodr'iguez and S.L.Cartwright and R.Castillo and M.G.Catanesi and A.Cervera and D.Cherdack and G.Christodoulou and A.Clifton and J.Coleman and S.J.Coleman and G.Collazuol and K.Connolly and L.Cremonesi and A.Dabrowska and I.Danko and R.Das and S.Davis and P. Perio and G. Rosa and T.Dealtry and S.R.Dennis and C.Densham and D.Dewhurst and F. Lodovico and S. Luise and O.Drapier and T.Duboyski and K.Duffy and J.Dumarchez and S.Dytman and M.Dziewiecki and S.Emery-Schrenk and A.Ereditato and L.Escudero and T.Feusels and A.J.Finch and G.A.Fiorentini and M.Friend and Y.Fujii and Y.Fukuda and A.P.Furmanski and V.Galymov and A.Garcia and S.Giffin and C.Giganti and K.Gilje and D.Goeldi and T.Golan and M.Gonin and N.Grant and D.Gudin and D.R.Hadley and L.Haegel and A.Haesler and M.D.Haigh and P.Hamilton and D.Hansen and T.Hara and M.Hartz and T.Hasegawa and N.C.Hastings and T.Hayashino and Y.Hayato and C.Hearty and R.L.Helmer and M.Hierholzer and J.Hignight and A.Hillairet and A.Himmel and T.Hiraki and S.Hirota and J.Holeczek and S.Horikawa and K.Huang and A.K.Ichikawa and K.Ieki and M.Ieva and M.Ikeda and J.Imber and J.Insler and T.J.Irvine and T.Ishida and T.Ishii and E.Iwai and K.Iwamoto and K.Iyogi and A.Izmaylov and A.Jacob and B.Jamieson and R.A.Johnson and S.Johnson and J.H.Jo and P.Jonsson and C.K.Jung and M.Kabirnezhad and A.C.Kaboth and T.Kajita and H.Kakuno and J.Kameda and Y.Kanazawa and D.Karlen and I.Karpikov and T.Katori and E.Kearns and M.Khabibullin and A.Khotjantsev and D.Kielczewska and T.Kikawa and A.Kilinski and J.Kim and S.King and J.Kisiel and P.Kitching and T.Kobayashi and L.Koch and T.Koga and A.Kolaceke and A.Konaka and L.L.Kormos and A.Korzenev and Y.Koshio and W.Kropp and H.Kubo and Y.Kudenko and R.Kurjata and T.Kutter and J.Lagoda and K.Laihem and I.Lamont and E.Larkin and M.Laveder and M.Lawe and M.Lazos and T.Lindner and C.Lister and R.P.Litchfield and A.Longhin and J.P.Lopez and L.Ludovici and L.Magaletti and K.Mahn and M.Malek and S.Manly and A.D.Marino and J.Marteau and J.F.Martin and P.Martins and S.Martynenko and T.Maruyama and V.Matveev and K.Mavrokoridis and E.Mazzucato and M.McCarthy and N.McCauley and K.S.McFarland and C.McGrew and A.Mefodiev and C.Metelko and M.Mezzetto and P.Mijakowski and C.A.Miller and A.Minamino and O.Mineev and A.Missert and M.Miura and S.Moriyama and Th.A.Mueller and A.Murakami and M.Murdoch and S.Murphy and J.Myslik and T.Nakadaira and M.Nakahata and K.G.Nakamura and K.Nakamura and S.Nakayama and T.Nakaya and K.Nakayoshi and C.Nantais and C.Nielsen and M.Nirkko and K.Nishikawa and Y.Nishimura and J.Nowak and H.M.O'Keeffe and R.Ohta and K.Okumura and T.Okusawa and W.Oryszczak and S.M.Oser and T.Ovsyannikova and R.A.Owen and Y.Oyama and V.Palladino and J.L.Palomino and V.Paolone and D.Payne and O.Perevozchikov and J.D.Perkin and Y.Petrov and L.Pickard and E. Guerra and C.Pistillo and P.Plonski and E.Poplawska and B.Popov and M.Posiadala-Zezula and J.-M.Poutissou and R.Poutissou and P.Przewlocki and B.Quilain and E.Radicioni and P.N.Ratoff and M.Ravonel and M.A.M.Rayner and A.Redij and M.Reeves and E.Reinherz-Aronis and C.Riccio and P.A.Rodrigues and P.Rojas and E.Rondio and S.Roth and A.Rubbia and D.Ruterbories and R.Sacco and K.Sakashita and F.S'anchez and F.Sato and E.Scantamburlo and K.Scholberg and S.Schoppmann and J.Schwehr and M.Scott and Y.Seiya and T.Sekiguchi and H.Sekiya and D.Sgalaberna and R.Shah and F.Shaker and M.Shiozawa and S.Short and Y.Shustrov and P.Sinclair and B.Smith and M.Smy and J.T.Sobczyk and H.Sobel and M.Sorel and L.Southwell and P.Stamoulis and J.Steinmann and B.Still and Y.Suda and A.Suzuki and K.Suzuki and S.Y.Suzuki and Y.Suzuki and R.Tacik and M.Tada and S.Takahashi and A.Takeda and Y.Takeuchi and H.K.Tanaka and H.A.Tanaka and M.M.Tanaka and D.Terhorst and R.Terri and L.F.Thompson and A.Thorley and S.Tobayama and W.Toki and T.Tomura and Y.Totsuka and C.Touramanis and T.Tsukamoto and M.Tzanov and Y.Uchida and A.Vacheret and M.Vagins and G.Vasseur and T.Wachala and A.V.Waldron and K.Wakamatsu and C.W.Walter and D.Wark and W.Warzycha and M.O.Wascko and A.Weber and R.Wendell and R.J.Wilkes and M.J.Wilking and C.Wilkinson and Z.Williamson and J.R.Wilson and R.J.Wilson and T.Wongjirad and Y.Yamada and K.Yamamoto and C.Yanagisawa and T.Yano and S.Yen and N.Yershov and M.Yokoyama and K.Yoshida and T.Yuan and M.Yu and A.Zalewska and J.Zalipska and L.Zambelli and K.Zaremba and M.Ziembicki and E.D.Zimmerman and M.Zito and J.Zmuda},
  journal={Progress of Theoretical and Experimental Physics},
  year={2014},
  volume={2015}
}
  • K.Abe, J.Adam, +342 authors J.Zmuda
  • Published 2014
  • Physics
  • Progress of Theoretical and Experimental Physics
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… Expand
Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6E20 protons on target
We report on measurements of neutrino oscillation using data from the T2K long-baseline neutrino experiment collected between 2010 and 2013. In an analysis of muon neutrino disappearance alone, weExpand
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This talk presented the first muon anti-neutrino disappearance analysis using data from the T2K anti-neutrino data taken in 2014 and up to March 12, 2015. The preliminary measured oscillationExpand
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Hyper-Kamiokande will be a next generation underground water Cherenkov detector with a total (fiducial) mass of 0.99 (0.56) million metric tons, approximately 20 (25) times larger than that ofExpand
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The longstanding discrepancy between bubble chamber measurements of $$\nu _\mu $$νμ-induced single pion production channels has led to large uncertainties in pion production cross section parametersExpand
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A bstractWe investigate invisible decays of the third neutrino mass eigenstate in future accelerator neutrino experiments using muon-decay beams such as MuOn-decay MEdium baseline NeuTrino beamExpand
Measurement of neutrino oscillation parameters using neutrino and antineutrino data of the T2K experiment
This thesis presents a measurement of the neutrino oscillation parameters with the T2K experiment. A simultaneous analysis of ND280 and Super-Kamiokande data is performed to measure sin^2 θ_23,Expand
Sensitivities to charged-current nonstandard neutrino interactions at DUNE
We investigate the effects of charged-current (CC) nonstandard neutrino interactions (NSIs) at the source and at the detector in the simulated data for the planned Deep Underground NeutrinoExpand
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A bstractWe study the impact of one light sterile neutrino on the prospective data expected to come from the two presently running long-baseline experiments T2K and NOvA when they will accumulateExpand
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References

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The T2K Experiment
The T2K experiment is a long-baseline neutrino oscillation experiment. Its main goal is to measure the last unknown lepton sector mixing angle {\theta}_{13} by observing {\nu}_e appearance in aExpand
Evidence for oscillation of atmospheric neutrinos
We present an analysis of atmospheric neutrino data from a 33.0 kton yr (535-day) exposure of the Super-Kamiokande detector. The data exhibit a zenith angle dependent deficit of muon neutrinos whichExpand
Evidence of electron neutrino appearance in a muon neutrino beam
The T2K collaboration reports evidence for electron neutrino appearance at the atmospheric mass splitting, |\Delta m_{32}^2|=2.4x10^{-3} eV^2. An excess of electron neutrino interactions overExpand
Measurement of neutrino oscillation by the K2K experiment
We present measurements of {nu}{sub {mu}} disappearance in K2K, the KEK to Kamioka long-baseline neutrino oscillation experiment. One-hundred and twelve beam-originated neutrino events are observedExpand
Combined analysis of all three phases of solar neutrino data from the Sudbury Neutrino Observatory
We report results from a combined analysis of solar neutrino data from all phases of the Sudbury Neutrino Observatory. By exploiting particle identification information obtained from the proportionalExpand
Measurement of atmospheric neutrino oscillation parameters by Super-Kamiokande I
We present a combined analysis of fully-contained, partially-contained and upward-going muon atmospheric neutrino data from a 1489 d exposure of the Super-Kamiokande detector. The data samples spanExpand
Observation of a first ντ candidate event in the OPERA experiment in the CNGS beam
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Observation of electron neutrino appearance in a muon neutrino beam.
  • K Abe, J. Adam, +336 authors J. Żmuda
  • Physics, Medicine
  • Physical review letters
  • 2014
TLDR
The T2K experiment has observed electron neutrino appearance in a muon neutrinos beam produced 295 km from the Super-Kamiokande detector with a peak energy of 0.6 GeV, corresponding to a significance of 7.3σ. Expand
First muon-neutrino disappearance study with an off-axis beam
We report a measurement of muon-neutrino disappearance in the T2K experiment. The 295-km muon-neutrino beam from Tokai to Kamioka is the first implementation of the off-axis technique in aExpand
Solar neutrino results in Super-Kamiokande-III
The results of the third phase of the Super-Kamiokande solar neutrino measurement are presented and compared to the first and second phase results. With improved detector calibrations, a fullExpand
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