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Related papers: Plans for super-beams in Japan

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I discuss why and how powerful is the two-detector setting in neutrino oscillation experiments. I cover three concrete examples: (1) reactor \theta_{13} experiments, (2) T2KK, Tokai-to-Kamioka-Korea two-detector complex for measuring CP…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hisakazu Minakata

The T2K neutrino oscillation experiment will start in 2009. In this experiment the center of the neutrino beam from J-PARC at Tokai village will go through underground beneath Super-Kamiokande, reach the sea level east of Korean shore, and…

High Energy Physics - Phenomenology · Physics 2010-11-11 Kaoru Hagiwara , Naotoshi Okamura , Ken-ichi Senda

The concept of a very long baseline neutrino experiment with quasi monochromatic neutrino beam and very large area underground detector is discussed. The detector could be placed in the existing 20 km tunnel at IHEP, Protvino. The High…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Ammosov , V. Garkusha , A. Ivanilov , V. Kabachenko , E. Melnikov , F. Novoskoltsev , A. Soldatov , A. Zaitsev

Hyper-Kamiokande is a large infrastructure for particle and astroparticle physics being built in Japan and aiming to start operations by the end of 2027 whose objective is to address the most important questions in science today, for…

High Energy Physics - Experiment · Physics 2025-06-23 Kamiokande Collaboration

Long-baseline neutrino oscillation experiments, in particular Deep Underground Neutrino Experiment (DUNE) and Tokai to Hyper-Kamiokande (T2HK), will lead the effort in the precision determination of the as yet unknown parameters of the…

High Energy Physics - Phenomenology · Physics 2017-08-30 Peter Ballett , Stephen F. King , Silvia Pascoli , Nick W. Prouse , TseChun Wang

The T2K experiment is a second generation long baseline neutrino oscillation experiment designed as a sensitive search for nu_e appearance. The T2K near neutrino detector complex is located 280 meters from the pion production target and…

Instrumentation and Detectors · Physics 2017-06-01 Yury Kudenko

The Tokai to Kamioka (T2K) long-baseline neutrino experiment consists of a muon neutrino beam, produced at the J-PARC accelerator, a near detector complex and a large 295km distant far detector. The present work utilizes the T2K event…

High Energy Physics - Experiment · Physics 2015-02-25 T2K Collaboration

The T2K long-baseline neutrino-oscillationexperiment was started in January 2010 for the purpose of physics data-taking. Until the massive earthquake on March 11, 2011 in Japan, $1.43\times 10^{20}$ pot data were accumulated. In this data,…

High Energy Physics - Experiment · Physics 2019-08-14 Yuichi Oyama

We study the feasibility of a long baseline neutrino experiment from CERN to Gran Sasso LNGS Laboratories using the CERN PS accelerator. Baseline and neutrino energy spectrum are suitable to explore a region of the (Dm2, Sin2(theta))…

High Energy Physics - Experiment · Physics 2007-05-23 P. F. Loverre , R. Santacesaria , F. R. Spada

Recent neutrino oscillation results have shown that the existing long baseline experiments have some sensitivity to the effects of CP violation in the neutrino sector. This sensitivity is currently statistically limited, but the next…

Instrumentation and Detectors · Physics 2019-08-21 Mark Scott

On the strength of a double Nobel prize winning experiment (Super)Kamiokande and an extremely successful long baseline neutrino programme, the third generation Water Cherenkov detector, Hyper-Kamiokande, is being developed by an…

Instrumentation and Detectors · Physics 2018-11-30 Hyper-Kamiokande Proto-Collaboration , : , K. Abe , Ke. Abe , H. Aihara , A. Aimi , R. Akutsu , C. Andreopoulos , I. Anghel , L. H. V. Anthony , M. Antonova , Y. Ashida , V. Aushev , M. Barbi , G. J. Barker , G. Barr , P. Beltrame , V. Berardi , M. Bergevin , S. Berkman , L. Berns , T. Berry , S. Bhadra , D. Bravo-Berguño , F. d. M. Blaszczyk , A. Blondel , S. Bolognesi , S. B. Boyd , A. Bravar , C. Bronner , M. Buizza Avanzini , F. S. Cafagna , A. Cole , R. Calland , S. Cao , S. L. Cartwright , M. G. Catanesi , C. Checchia , Z. Chen-Wishart , J. H. Choi , K. Choi , J. Coleman , G. Collazuol , G. Cowan , L. Cremonesi , T. Dealtry , G. De Rosa , C. Densham , D. Dewhurst , E. L. Drakopoulou , F. Di Lodovico , O. Drapier , J. Dumarchez , P. Dunne , M. Dziewiecki , S. Emery , A. Esmaili , A. Evangelisti , E. Fernandez-Martinez , T. Feusels , A. Finch , A. Fiorentini , G. Fiorillo , M. Fitton , K. Frankiewicz , M. Friend , Y. Fujii , Y. Fukuda , D. Fukuda , K. Ganezer , C. Giganti , M. Gonin , N. Grant , P. Gumplinger , D. R. Hadley , B. Hartfiel , M. Hartz , Y. Hayato , K. Hayrapetyan , J. Hill , S. Hirota , S. Horiuchi , A. K. Ichikawa , T. Iijima , M. Ikeda , J. Imber , K. Inoue , J. Insler , R. A. Intonti , A. Ioannisian , T. Ishida , H. Ishino , M. Ishitsuka , Y. Itow , K. Iwamoto , A. Izmaylov , B. Jamieson , H. I. Jang , J. S. Jang , S. H. Jeon , M. Jiang , P. Jonsson , K. K. Joo , A. Kaboth , C. Kachulis , T. Kajita , J. Kameda , Y. Kataoka , T. Katori , K. Kayrapetyan , E. Kearns , M. Khabibullin , A. Khotjantsev , J. H. Kim , J. Y. Kim , S. B. Kim , S. Y. Kim , S. King , Y. Kishimoto , T. Kobayashi , M. Koga , A. Konaka , L. L. Kormos , Y. Koshio , A. Korzenev , K. L. Kowalik , W. R. Kropp , Y. Kudenko , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , P. J. J. Lasorak , M. Laveder , M. Lawe , J. G. Learned , I. T. Lim , T. Lindner , R. P. Litchfield , A. Longhin , P. Loverre , T. Lou , L. Ludovici , W. Ma , L. Magaletti , K. Mahn , M. Malek , L. Maret , C. Mariani , K. Martens , Ll. Marti , J. F. Martin , J. Marzec , S. Matsuno , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , P. Mermod , C. Metelko , M. Mezzetto , J. Migenda , P. Mijakowski , H. Minakata , A. Minamino , S. Mine , O. Mineev , A. Mitra , M. Miura , T. Mochizuki , J. Monroe , D. H. Moon , S. Moriyama , T. Mueller , F. Muheim , K. Murase , F. Muto , M. Nakahata , Y. Nakajima , K. Nakamura , T. Nakaya , S. Nakayama , C. Nantais , M. Needham , T. Nicholls , Y. Nishimura , E. Noah , F. Nova , J. Nowak , H. Nunokawa , Y. Obayashi , H. M. O'Keeffe , Y. Okajima , K. Okumura , Yu. Onishchuk , E. O'Sullivan , L. O'Sullivan , T. Ovsiannikova , R. A. Owen , Y. Oyama , M. Y. Pac , V. Palladino , J. L. Palomino , V. Paolone , W. Parker , S. Parsa , D. Payne , J. D. Perkin , C. Pidcott , E. Pinzon Guerra , S. Playfer , B. Popov , M. Posiadala-Zezula , J. M. Poutissou , A. Pritchard , N. W. Prouse , G. Pronost , P. Przewlocki , B. Quilain , E. Radicioni , P. N. Ratoff , F. Retiere , C. Riccio , B. Richards , E. Rondio , H. J. Rose , C. Rott , S. D. Rountree , A. C. Ruggeri , A. Rychter , R. Sacco , M. Sakuda , M. C. Sanchez , E. Scantamburlo , M. Scott , S. M. Sedgwick , Y. Seiya , T. Sekiguchi , H. Sekiya , S. H. Seo , D. Sgalaberna , R. Shah , A. Shaikhiev , I. Shimizu , M. Shiozawa , Y. Shitov , S. Short , C. Simpson , G. Sinnis , M. B. Smy , S. Snow , J. Sobczyk , H. W. Sobel , Y. Sonoda , R. Spina , T. Stewart , J. L. Stone , Y. Suda , Y. Suwa , Y. Suzuki , A. T. Suzuki , R. Svoboda , M. Taani , R. Tacik , A. Takeda , A. Takenaka , A. Taketa , Y. Takeuchi , V. Takhistov , H. A. Tanaka , H. K. M. Tanaka , H. Tanaka , R. Terri , M. Thiesse , L. F. Thompson , M. Thorpe , S. Tobayama , C. Touramanis , T. Towstego , T. Tsukamoto , K. M. Tsui , M. Tzanov , Y. Uchida , M. R. Vagins , G. Vasseur , C. Vilela , R. B. Vogelaar , J. Walding , J. Walker , M. Ward , 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 , D. N. Yeum , M. Yokoyama , T. Yoshida , I. Yu , M. Yu , J. Zalipska , K. Zaremba , M. Ziembicki , M. Zito , S. Zsoldos

Having a far detector in Korea for the J-PARC neutrino beam in addition to one at Kamioka has been shown to be a powerful way to lift neutrino parameter ($\Delta m^2$ and mixing angles) degeneracies. In this talk, I report the sensitivity…

High Energy Physics - Phenomenology · Physics 2008-01-29 N. Cipriano Ribeiro , T. Kajita , P. Ko , H. Minakata , S. Nakayama , H. Nunokawa

The Japan Proton Accelerator Research Complex (J-PARC) currently delivers a 1 MW, 3 GeV proton beam to the Materials and Life Science Experimental Facility (MLF). Power is expected to increase to 1.3 MW, driven by the needs of…

The Hyper-Kamiokande (HK) experiment centres around a proposed next-generation underground water Cherenkov detector that will be nearly 20 times larger than the highly successful Super-Kamiokande experiment and use significantly improved…

High Energy Physics - Experiment · Physics 2019-08-14 Jost Migenda

In this talk I compare the physics potential of possible future neutrino oscillation experiments from CERN to a Mt scale water Cerenkov detector at Frejus (MEMPHYS) and of the T2HK proposal in Japan, where for the CERN experiments an SPL…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Schwetz

New results from the K2K (KEK to Kamioka) long-baseline neutrino-oscillation experiment is presented.

High Energy Physics - Experiment · Physics 2007-05-23 Yuichi Oyama

We study physics potential of Very Long Base-Line (VLBL) Neutrino-Oscillation Experiments with the High Intensity Proton Accelerator, which will be completed by the year 2007 in Tokai-village, Japan. As a target, a 100 kton-level…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mayumi Aoki

The K2K (KEK to Kamioka) long-baseline neutrino-oscillation experiment was successfully started in early 1999. A total intensity of 7.20 x 10^18 protons on target, which is about 7% of the goal of the experiment, was accumulated in 39.4…

High Energy Physics - Experiment · Physics 2007-05-23 Yuichi Oyama

We study physics possibility of Very Long Base-Line (VLBL) Neutrino-Oscillation Experiments with the High Intensity Proton Accelerator, which will be completed by the year 2007 in Tokai-village, Japan. As a target, a 100 kton-level…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Okamura

Future neutrino projects in Europe will follow two distinct time lines. On the medium term, they will be dominated by the CERN-Gran Sasso long-baseline project, with two experiments OPERA and ICARUS, mainly concentrated on $\tau$…

High Energy Physics - Experiment · Physics 2017-08-23 Mario Campanelli