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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 of Super-Kamiokande. One of the main goals of…

Instrumentation and Detectors · Physics 2015-01-20 Kamiokande Working Group , K. Abe , H. Aihara , C. Andreopoulos , I. Anghel , A. Ariga , T. Ariga , R. Asfandiyarov , M. Askins , 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

In this paper we quantify the trade-off between setups optimized to be ancillary to Phase II Superbeams or Neutrino Factories and experiments tuned for maximal sensitivity to the subdominant terms of the neutrino transition probability at…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Migliozzi , F. Terranova

We discuss the minimum requirements for a neutrino beta beam if theta_13 is discovered by an upcoming reactor experiment, such as Double Chooz or Daya Bay. We require that both neutrino mass hierarchy and leptonic CP violation can be…

High Energy Physics - Phenomenology · Physics 2009-11-13 Walter Winter

We explore as clearly as possible the features of neutrino oscillation which are relevant for measurements of the CP violating Kobayashi-Maskawa phase delta and the sign of \Delta m^2_{13}. We focus on the so called low-energy option and…

High Energy Physics - Phenomenology · Physics 2010-02-03 Hisakazu Minakata , Hiroshi Nunokawa

This article describes a new experimental method for accelerator based neutrino experiments called neutrino tagging. The method consists in exploiting the neutrino production mechanism, the $\pi^{\pm}\to\mu^{\pm}\nu_\mu$ decay, to…

High Energy Physics - Experiment · Physics 2022-06-02 Mathieu Perrin-Terrin

In this article we investigate the prospects for probing the strength of the possible non-standard neutrino interactions (NSI) in long baseline neutrino oscillation experiments. We find that these experiments are sensitive to NSI couplings…

High Energy Physics - Phenomenology · Physics 2016-04-06 Katri Huitu , Timo J. Kärkkäinen , Jukka Maalampi , Sampsa Vihonen

Over the past few decades, outstanding progress in the neutrino experiment frontier has greatly advanced our understanding of the flavor oscillations of active neutrinos. The remaining key questions such as the neutrino mass ordering, the…

High Energy Physics - Phenomenology · Physics 2025-09-25 Sudipta Das

This research continues to focus on the idea using cyclotronic antineutrino source for purposes of neutrino physics. Long baseline experiments suffer from degeneracies and correlations between $\Theta_{23}$, $\delta_{\rm CP}$ and the mass…

High Energy Physics - Phenomenology · Physics 2019-03-19 M. V. Smirnov , Zh. J. Hu , S. J. Li , J. J. Ling

The primary goal of the Long-Baseline Neutrino Experiment (LBNE) is to measure the neutrino mixing matrix parameters. The design, optimized to search for CP violation and to determine the neutrino mass hierarchy, includes a large…

High Energy Physics - Experiment · Physics 2013-10-28 Matthew Bass , Daniel Cherdack , Robert J. Wilson

A brief review of the experimental status of neutrino mixing. The model of neutrino oscillations has now been established with high confidence, with many of the model parameters measured to an accuracy of a few per cent. However, some…

High Energy Physics - Experiment · Physics 2011-07-21 Justin Evans

In a recent work by two of us, we have studied, how CP violation discovery potential can be improved at long baseline neutrino experiments (LBNE/DUNE), by combining with its ND (near detector) and reactor experiments. In this work, we…

High Energy Physics - Phenomenology · Physics 2016-03-07 Kalpana Bora , Gayatri Ghosh , Debajyoti Dutta

We present a systematic procedure to establish a connection between complex neutrino mass matrix textures and experimental observables, including the Dirac CP phase. In addition, we illustrate how future experimental measurements affect the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Walter Winter

Recently, the reactor mixing angle $\theta_{13}$ has been measured precisely by Daya Bay, RENO and T2K experiments with a moderately large value. However, the standard form of neutrino mixing patterns such as bimaximal, tri-bimaximal,…

High Energy Physics - Phenomenology · Physics 2015-09-02 Sruthilaya M. , Soumya C. , K. N. Deepthi , R. Mohanta

Assuming 3-$\nu$ mixing, massive Majorana neutrinos and neutrinoless double-beta (\betabeta-) decay generated only by the (V-A) charged current weak interaction via the exchange of the three Majorana neutrinos, we briefly review the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Pascoli , S. T. Petcov , T. Schwetz

In view of recent measurements of the mixing angle \theta_{13} a possibility to determine the difference of two CP Majorana phases of the neutrino mixing matrix from the study of neutrinoless double-beta decay is investigated. We show that…

High Energy Physics - Phenomenology · Physics 2015-06-11 F. Simkovic , S. M. Bilenky , Amand Faessler , Th. Gutsche

The physics potential of beta beams is investigated from low to very high gamma values and it is compared to superbeams and neutrino factories. The gamma factor and the baseline are treated as continuous variables in the optimization of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Huber , M. Lindner , M. Rolinec , W. Winter

We examine the prospects of probing nonstandard interactions (NSI) of neutrinos in the e-tau sector with upcoming long-baseline nu_mu -> nu_e oscillation experiments. First conjectured decades ago, neutrino NSI remain of great interest,…

High Energy Physics - Phenomenology · Physics 2012-07-31 Alexander Friedland , Ian M. Shoemaker

The opportunities which are offered by a next generation and multi-purpose fixed-target experiment exploiting the proton and lead LHC beams extracted by a bent crystal are outlined. In particular, such an experiment can greatly complement…

Beam neutrino oscillation experiments typically employ only one detector at a certain baseline, apart from the near detector that measures the unoscillated neutrino flux at the source. Lately, there have been discussions of having detectors…

High Energy Physics - Phenomenology · Physics 2019-07-03 Minseok Cho , YeolLin ChoeJo , Hye-Sung Lee , Young-Min Lee , Sushant K. Raut

We consider the nu_mu to nu_e oscillation measurements that would be possible at upgraded 1 GeV and multi-GeV conventional neutrino sources driven by future megawatt-scale proton drivers. If these neutrino superbeams are used together with…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Barger