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The proposed KAON factory at the Triumf Laboratory in Vancouver, Canada provides a unique opportunity for high statistics long baseline neutrino oscillation experiments. Several possibilities are under active consideration. In this paper we…

High Energy Physics - Phenomenology · Physics 2008-02-03 Scott Hayward , Martin Sevior , Nathan Weiss , Dennis Wright

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

In this talk, we show the physics impacts of putting a large Water Cerenkov detector in Korea during the T2K experimental period. The T2K experiment which will start in 2009 plans to use the high intensity conventional neutrino beam from…

High Energy Physics - Phenomenology · Physics 2007-05-23 Naotoshi Okamura

Super-Kamiokande is a 50 kiloton water Cherenkov detector located at the Kamioka Observatory of the Institute for Cosmic Ray Research, University of Tokyo. It was designed to study neutrino oscillations and carry out searches for the decay…

High Energy Physics - Experiment · Physics 2016-11-23 C. W. Walter

A long-baseline neutrino-oscillation experiment using a well-defined neutrino beam is in preparation at KEK. Neutrinos generated at KEK will be detected by the Super-kamiokande detector 250 km away. The design of the neutrino beam line,…

High Energy Physics - Experiment · Physics 2009-09-25 Yuichi Oyama

The three neutrino model has 9 physical parameters, 3 neutrino masses, 3 mixing angles and 3 CP violating phases. Among them, neutrino oscillation experiments can probe 6 parameters: 2 mass squared differences, 3 mixing angles, and 1 CP…

High Energy Physics - Phenomenology · Physics 2009-11-10 Kaoru Hagiwara

Hyper-Kamiokande (HK) is the next generation underground water Cherenkov detector that builds on the highly successful Super-Kamiokande (SK) experiment. The 260,000-ton detector has an 8.4 times larger fiducial volume than its predecessor.…

Hyper-Kamiokande is the next generation underground water Cherenkov detector that builds on the highly successful Super-Kamiokande experiment. The detector which has an 8.4~times larger effective volume than its predecessor will be located…

Instrumentation and Detectors · Physics 2020-09-03 Kamiokande Collaboration , K. Abe , P. Adrich , H. Aihara , R. Akutsu , I. Alekseev , A. Ali , F. Ameli , L. H. V. Anthony , A. Araya , Y. Asaoka , V. Aushev , I. Bandac , M. Barbi , G. Barr , M. Batkiewicz-Kwasniak , M. Bellato , V. Berardi , L. Bernard , E. Bernardini , L. Berns , S. Bhadra , J. Bian , A. Blanchet , A. Blondel , A. Boiano , S. Bolognesi , L. Bonavera , S. Borjabad , T. Boschi , D. Bose , S . B. Boyd , C. Bozza , A. Bravar , C. Bronner , A. Bubak , A. Buchowicz , M. Buizza Avanzini , F. S. Cafagna , N. F. Calabria , J. M. Calvo-Mozota , S. Cao , M. G. Catanesi , S. Chakraborty , J. H. Choi , S. Choubey , M. Cicerchia , J. Coleman , G. Collazuol , S. Cuen-Rochin , M. Danilov , E. De la Fuente , P. de Perio , G. De Rosa , T. Dealtry , C. J. Densham , A. Dergacheva , N. Deshmukh , M. M. Devi , F. Di Lodovico , P. Di Meo , I. Di Palma , T. A. Doyle , E. Drakopoulou , O. Drapier , J. Dumarchez , L. Eklund , S. El Hedri , J. Ellis , S. Emery , A. Esmaili , S. Fedotov , J. Feng , E. Fernández-Martinez , P. Ferrario , B. Ferrazzi , A. Finch , C. Finley , G. Fiorillo , M. Fitton , M. Friend , Y. Fujii , Y. Fukuda , G. Galinski , J. Gao , C. Garde , A. Garfagnini , S. Garode , L. Gialanella , C. Giganti , J. J. Gomez-Cadenas , M. Gonin , J. González-Nuevo , A. Gorin , R. Gornea , F. Gramegna , M. Grassi , G. Grella , M. Guigue , D. R. Hadley , M. Harada , M. Hartz , S. Hassani , N. C. Hastings , Y. Hayato , K. Hiraide , K. Hoshina , K. Hultqvist , F. Iacob , A. K. Ichikawa , W. Idrissi Ibnsalih , M. Ikeda , M. Inomoto , A. Ioannisian , T. Ishida , K. Ishidoshiro , H. Ishino , M. Ishitsuka , H. Ito , S. Ito , Y. Itow , K. Iwamoto , N. Izumi , S. Izumiyama , M. Jakkapu , B. Jamieson , J. S. Jang , H. S. Jo , P. Jonsson , K. K. Joo , T. Kajita , H. Kakuno , J. Kameda , Y. Kano , D. Karlen , Y. Kataoka , A. Kato , T. Katori , N. Kazarian , M. Khabibullin , A. Khotjantsev , T. Kikawa , J. Y. Kim , S. B. Kim , S. King , T. Kinoshita , J. Kisiel , A. Klekotko , T. Kobayashi , L. Koerich , N. Kolev , A. Konaka , L. L. Kormos , Y. Koshio , Y. Kotsar , K. A. Kouzakov , K. L. Kowalik , L. Kravchuk , A. P. Kryukov , Y. Kudenko , T. Kumita , R. Kurjata , T. Kutter , M. Kuze , K. Kwak , M. La Commara , L. Labarga , J. Lagoda , M. Lamoureux , M. Laveder , L. Lavitola , J. Lee , R. Leitner , V. Lezaun , I. T. Lim , T. Lindner , R. P. Litchfield , K. R. Long , A. Longhin , P. Loverre , X. Lu , L. Ludovici , Y. Maekawa , L. Magaletti , K. Magar , Y. Makida , M. Malek , M. Malinský , T. Marchi , C. Mariani , A. Marinelli , K. Martens , Ll. Marti , J. F. Martin , D. Martin , J. Marzec , T. Matsubara , R. Matsumoto , N. McCauley , A. Medhi , P. Mehta , L. Mellet , H. Menjo , M. Mezzetto , J. Migenda , P. Migliozzi , S. Miki , A. Minamino , S. Mine , O. Mineev , A. Mitra , M. Miura , R. Moharana , C. M. Mollo , T. Mondal , M. Mongelli , F. Monrabal , D. H. Moon , C. S. Moon , S. Moriyama , T. Mueller , Y. Nagao , T. Nakadaira , K. Nakagiri , M. Nakahata , S. Nakai , Y. Nakajima , K. Nakamura , KI. Nakamura , H. Nakamura , Y. Nakano , T. Nakaya , S. Nakayama , K. Nakayoshi , L. Nascimento Machado , C. E. R. Naseby , B. Navarro-Garcia , M. Needham , K. Niewczas , Y. Nishimura , F. Nova , J. C. Nugent , H. Nunokawa , W. Obrebski , J. P. Ochoa-Ricoux , E. O'Connor , N. Ogawa , T. Ogitsu , K. Okamoto , H. M. O'Keeffe , K. Okumura , Y. Onishchuk , F. Orozco-Luna , A. Oshlianskyi , N. Ospina , M. Ostrowski , E. O'Sullivan , Y. Oyama , H. Ozaki , M. Y. Pac , P. Paganini , V. Palladino , M. Pari , J. Pasternak , C. Pastore , G. Pastuszak , D. A. Patel , M. Pavin , D. Payne , C. Peña-Garay , C. Pidcott , S. Playfer , B. W. Pointon , A. Popov , B. Popov , K. Porwit , M. Posiadala-Zezula , G. Pronost , N. W. Prouse , B. Quilain , A. A. Quiroga , E. Radicioni , B. Radics , P. J. Rajda , M. Rescigno , G. Ricciardi , B. Richards , E. Rondio , B. Roskovec , S. Roth , C. Rott , A. Rubbia , A. C. Ruggeri , S. Russo , A. Rychter , D. Ryu , K. Sakashita , S. Samani , F. Sánchez , M. L. Sánchez , S. Sano , J. D. Santos , G. Santucci , P. Sarmah , K. Sato , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , J. W. Seo , D. Sgalaberna , A. Shaykina , I. Shimizu , C. D. Shin , M. Shinoki , M. Shiozawa , N. Skrobova , K. Skwarczynski , M. B. Smy , J. Sobczyk , H. W. Sobel , F. J. P. Soler , Y. Sonoda , R. Spina , B. Spisso , P. Spradlin , K. L. Stankevich , L. Stawarz , S. M. Stellacci , A. I. Studenikin , S. L. Suárez Gómez , T. Suganuma , S. Suvorov , Y. Suwa , A. T. Suzuki , S. Suzuki , Y. Suzuki , D. Svirida , M. Taani , M. Tada , A. Takeda , Y. Takemoto , A. Takenaka , A. Taketa , Y. Takeuchi , H. Tanaka , H. I. Tanaka , M. Tanaka , T. Tashiro , M. Thiesse , L. F. Thompson , A. K. Tomatani-Sánchez , G. Tortone , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. R. Vagins , S. Valder , V. Valentino , G. Vasseur , A. Vijayvargi , W. G. S. Vinning , D. Vivolo , R. B. Vogelaar , M. M. Vyalkov , T. Wachala , J. Walker , D. Wark , M. O. Wascko , R. A. Wendell , J. R. Wilson , S. Wronka , J. Xia , Y. Yamaguchi , K. Yamamoto , T. Yano , N. Yershov , M. Yokoyama , J. Yoo , I. Yu , T. Zakrzewski , B. Zaldivar , J. Zalipska , K. Zaremba , G. Zarnecki , M. Ziembicki , K. Zietara , M. Zito , S. Zsoldos

The Tokai-to-Kamioka-and-Korea (T2KK) neutrino oscillation experiment under examination can have a high sensitivity to determine the neutrino mass hierarchy for a combination of relatively large (\sim 3.0^circ) off-axis angle beam at…

High Energy Physics - Phenomenology · Physics 2009-07-22 Kaoru Hagiwara , Naotoshi Okamura

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

Hyper-Kamiokande (Hyper-K) is a next-generation long baseline neutrino experiment. One of its primary physics goals is to measure neutrino oscillation parameters precisely, including the Dirac CP violating phase. As conventional $\nu_{\mu}$…

High Energy Physics - Experiment · Physics 2025-05-19 T. Mondal , N. W. Prouse , P. de Perio , M. Hartz , D. Bose

Hyper-Kamiokande, scheduled to begin construction as soon as 2020, is a next generation underground water Cherenkov detector, based on the highly successful Super-Kamiokande experiment. It will serve as a far detector, 295 km away, of a…

Instrumentation and Detectors · Physics 2020-01-08 Stephane Zsoldos

Hyper-Kamiokande (HK) is a next generation large water Cherenkov detector to be built in Japan, based on the highly successful Super-Kamiokande detector. HK will offer a broad science program such as neutrino oscillation studies, proton…

High Energy Physics - Experiment · Physics 2019-08-14 Masashi Yokoyama

We have shown in a previous paper that two identical detectors with each fiducial mass of 0.27 megaton water, one in Kamioka and the other in Korea, which receive the (anti-) muon neutrino beam of 4 MW power from J-PARC facility have…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takaaki Kajita , Hisakazu Minakata , Shoei Nakayama , Hiroshi Nunokawa

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

We revisit the sensitivity study of the Tokai-to-Kamioka-and-Korea (T2KK) and Tokai-to-Kamioka-and-Oki (T2KO) proposals where a water Cerenkov detector with the 100 kton fiducial volume is placed in Korea ($L = 1000$ km) and Oki island ($L…

High Energy Physics - Phenomenology · Physics 2017-03-09 Kaoru Hagiwara , Pyungwon Ko , Naotoshi Okamura , Yoshitaro Takaesu

T2K is a long-baseline neutrino oscillation experiment, in which a muon-neutrino beam is directed over a 295 km baseline from the J-PARC facility to the Super-Kamiokande detector. This allows neutrino oscillation to be studied in two…

High Energy Physics - Experiment · Physics 2019-08-14 Kirsty Duffy

It has been pointed out that the mixing of an eV-scale sterile neutrino with active flavors can lead to loss of sensitivity to the $\theta_{23}$ octant (sign of $\sin^2\theta_{23}-1/2$) in long baseline experiments, because the main…

High Energy Physics - Phenomenology · Physics 2020-04-22 Naoyuki Haba , Yukihiro Mimura , Toshifumi Yamada

The discovery potentials of non-standard physics (NSP) which might be possessed by neutrinos are examined by taking a concrete setting of Tokai-to-Kamioka-Korea (T2KK) two detector complex which receives neutrino superbeam from J-PARC. We…

High Energy Physics - Phenomenology · Physics 2008-01-17 Nei Cipriano Ribeiro , Takaaki Kajita , Pyungwon Ko , Hisakazu Minakata , Shoei Nakayama , Hiroshi Nunokawa

A variety of new physics scenarios allow for neutrinos to up-scatter into a heavy neutral lepton state. For a range of couplings and neutrino energies, the heavy neutrino may travel some distance before decaying to visible final states.…

High Energy Physics - Phenomenology · Physics 2022-10-31 Mack Atkinson , Pilar Coloma , Ivan Martinez-Soler , Noemi Rocco , Ian M. Shoemaker