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A Long Baseline Neutrino Oscillation Experiment Using J-PARC Neutrino Beam and Hyper-Kamiokande

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arxiv 1412.4673 v2 pith:3Q75CN3K submitted 2014-12-15 physics.ins-det hep-exhep-ph

Hyper-Kamiokande Working Group: K. Abe , H. Aihara , C. Andreopoulos , I. Anghel , A. Ariga , T. Ariga , R. Asfandiyarov , M. Askins
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J. J. Back P. Ballett M. Barbi G. J. Barker G. Barr F. Bay P. Beltrame V. Berardi M. Bergevin S. Berkman T. Berry S. Bhadra F. d. M. Blaszczyk A. Blondel S. Bolognesi S. B. Boyd A. Bravar C. Bronner F. S. Cafagna G. Carminati S. L. Cartwright M. G. Catanesi K. Choi J. H. Choi G. Collazuol G. Cowan L. Cremonesi G. Davies G. De Rosa C. Densham J. Detwiler D. Dewhurst F. Di Lodovico S. Di Luise O. Drapier S. Emery A. Ereditato P. Fernandez T. Feusels A. Finch M. Fitton M. Friend Y. Fujii Y. Fukuda D. Fukuda V. Galymov K. Ganezer M. Gonin P. Gumplinger D. R. Hadley L. Haegel A. Haesler Y. Haga B. Hartfiel M. Hartz Y. Hayato M. Hierholzer J. Hill A. Himmel S. Hirota S. Horiuchi K. Huang A. K. Ichikawa T. Iijima M. Ikeda J. Imber K. Inoue J. Insler R. A. Intonti T. Irvine T. Ishida H. Ishino M. Ishitsuka Y. Itow A. Izmaylov B. Jamieson H. I. Jang M. Jiang K. K. Joo C. K. Jung A. Kaboth T. Kajita J. Kameda Y. Karadhzov T. Katori E. Kearns M. Khabibullin A. Khotjantsev J. Y. Kim S. B. Kim Y. Kishimoto T. Kobayashi M. Koga A. Konaka L. L. Kormos A. Korzenev Y. Koshio W. R. Kropp Y. Kudenko T. Kutter M. Kuze L. Labarga J. Lagoda M. Laveder M. Lawe J. G. Learned I. T. Lim T. Lindner A. Longhin L. Ludovici W. Ma L. Magaletti K. Mahn M. Malek C. Mariani L. Marti J. F. Martin C. Martin P. P. J. Martins E. Mazzucato N. McCauley K. S. McFarland C. McGrew M. Mezzetto H. Minakata A. Minamino S. Mine O. Mineev M. Miura J. Monroe T. Mori S. Moriyama T. Mueller F. Muheim M. Nakahata K. Nakamura T. Nakaya S. Nakayama M. Needham T. Nicholls M. Nirkko Y. Nishimura E. Noah J. Nowak H. Nunokawa H. M. O'Keeffe Y. Okajima K. Okumura S. M. Oser E. O'Sullivan R. A. Owen Y. Oyama J. Perez M. Y. Pac V. Palladino J. L. Palomino V. Paolone D. Payne O. Perevozchikov J. D. Perkin C. Pistillo S. Playfer M. Posiadala-Zezula J.-M. Poutissou B. Quilain M. Quinto E. Radicioni P. N. Ratoff M. Ravonel M. Rayner A. Redij F. Retiere C. Riccio E. Richard E. Rondio H. J. Rose M. Ross-Lonergan C. Rott S. D. Rountree A. Rubbia R. Sacco M. Sakuda M. C. Sanchez E. Scantamburlo K. Scholberg M. Scott Y. Seiya T. Sekiguchi H. Sekiya A. Shaikhiev I. Shimizu M. Shiozawa S. Short G. Sinnis M. B. Smy J. Sobczyk H. W. Sobel T. Stewart J. L. Stone Y. Suda Y. Suzuki A. T. Suzuki R. Svoboda R. Tacik A. Takeda A. Taketa Y. Takeuchi H. A. Tanaka H. K. M. Tanaka H. Tanaka R. Terri L. F. Thompson M. Thorpe S. Tobayama N. Tolich T. Tomura C. Touramanis T. Tsukamoto M. Tzanov Y. Uchida M. R. Vagins G. Vasseur R. B. Vogelaar C. W. Walter D. Wark M. O. Wascko A. Weber R. Wendell R. J. Wilkes M. J. Wilking J. R. Wilson T. Xin K. Yamamoto C. Yanagisawa T. Yano S. Yen N. Yershov M. Yokoyama M. Zito
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classification physics.ins-dethep-exhep-ph
keywords neutrinobeamhyper-kamiokandeprotondeltaexperimentj-parcbaseline
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abstract

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 of Super-Kamiokande. One of the main goals of Hyper-Kamiokande is the study of $CP$ asymmetry in the lepton sector using accelerator neutrino and anti-neutrino beams. In this document, the physics potential of a long baseline neutrino experiment using the Hyper-Kamiokande detector and a neutrino beam from the J-PARC proton synchrotron is presented. The analysis has been updated from the previous Letter of Intent [K. Abe et al., arXiv:1109.3262 [hep-ex]], based on the experience gained from the ongoing T2K experiment. With a total exposure of 7.5 MW $\times$ 10$^7$ sec integrated proton beam power (corresponding to $1.56\times10^{22}$ protons on target with a 30 GeV proton beam) to a $2.5$-degree off-axis neutrino beam produced by the J-PARC proton synchrotron, it is expected that the $CP$ phase $\delta_{CP}$ can be determined to better than 19 degrees for all possible values of $\delta_{CP}$, and $CP$ violation can be established with a statistical significance of more than $3\,\sigma$ ($5\,\sigma$) for $76%$ ($58%$) of the $\delta_{CP}$ parameter space.

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