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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

We study physics potential of placing a far detector in the east coast of Korea, where the off-axis beam from J-PARC at Tokai village for the T2K project has significant intensity at a few GeV range. In particular we examine the capability…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaoru Hagiwara , Naotoshi Okamura , Ken-ichi Senda

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

The ``baseline setup'' for a possible, beyond T2K, next generation long baseline experiment along the J-PARC neutrino beam produced at Tokai, assumes two very large deep-underground Water Cerenkov imaging detectors of about 300 kton…

High Energy Physics - Phenomenology · Physics 2008-01-29 A. Meregaglia , A. Rubbia

T2K is a long baseline high intensity neutrino oscillation experiment employing an off-axis design to search for the as yet unobserved appearance of \nu_e neutrinos in a \nu_{\mu} beam. The neutrino beam originates at the J-PARC facility in…

High Energy Physics - Experiment · Physics 2019-08-14 Mark Hartz

Oki Island is located between Japan and Korea along the Tokai-To-Kamioka (T2K) baseline. The distance from J-PARC to Oki Island is about 653km, which is twice that of the T2K experiment (L=295km). When the off-axis angle of the neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-11 Kaoru Hagiwara , Takayuki Kiwanami , Naotoshi Okamura , Ken-ichi Senda

If the atmospheric neutrino oscillation amplitude, sin^2 2theta_atm is not maximal, there is a two fold ambiguity in the neutrino parameter space: sin^2 theta_atm>0.5 or sin^2 theta_atm<0.5. In this article, we study the impact of this…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaoru Hagiwara , Naotoshi Okamura

T2K is a long-baseline neutrino oscillation experiment taking data since 2010. A neutrino beam is produced at the J-PARC accelerator in Japan and is sampled at a Near Detector complex 280 m from the neutrino production point and at the far…

High Energy Physics - Experiment · Physics 2022-09-21 L. Haegel

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

The Tokai to Kamioka (T2K) experiment uses a beam of muon neutrinos, produced at the J-PARC facility on the east coast of Japan, to study neutrino oscillations driven by the $\Delta m_{\textrm{atm}}^{2}$ mass splitting. A suite of near…

High Energy Physics - Experiment · Physics 2015-01-20 Martin David Haigh

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

The T2K (Tokai to Kamioka) experiment is a long-baseline accelerator neutrino oscillation experiment. Intense muon neutrino and antineutrino beams are produced at the J-PARC accelerator complex situated in Tokai. After 280 metres the beam…

High Energy Physics - Experiment · Physics 2018-05-11 Marcela Batkiewicz

Tokai-to-Kamioka T2K is a long baseline neutrino oscillation experiment, looking for sub-dominant muon neutrino to electron neutrino oscillations. One of the primary aims of the T2K experiment is to narrow down the current limit on the…

High Energy Physics - Experiment · Physics 2010-06-08 Melissa George

We explore the possibility of simultaneous determination of neutrino mass hierarchy and the CP violating phase by using two identical detectors placed at different baseline distances. We focus on a possible experimental setup using neutrino…

High Energy Physics - Phenomenology · Physics 2010-04-06 Masaki Ishitsuka , Takaaki Kajita , Hisakazu Minakata , Hiroshi Nunokawa

T2K is a long-baseline neutrino oscillation experiment, in which a muon neutrino beam is produced at J-PARC and detected 295 km away at the Super-Kamiokande detector. The T2K experiment observed electron-neutrino appearance in 2012. This…

High Energy Physics - Experiment · Physics 2015-08-26 M. Ravonel Salzgeber

T2K is a neutrino oscillation experiment with a 295 km long baseline between the far detector, Super-Kamiokande, and a suite of near detectors to study $\nu_\mu/\bar{\nu}_\mu$ disappearance and $\nu_e/\bar{\nu}_e$ appearance in a…

High Energy Physics - Experiment · Physics 2024-05-13 T. Nosek

T2K is a long-baseline neutrino oscillation experiment using a $\nu_{\mu}$ beam produced at the J-PARC facility. Neutrinos are detected at a Near Detector complex (ND280) and at the Far Detector (Super-Kamiokande). The most recent…

High Energy Physics - Experiment · Physics 2018-04-02 Claudio Giganti

T2K is a long baseline neutrino experiment which exploits a neutrino and antineutrino beam at JPARC to perform precision measurements of neutrino oscillation parameters $\Delta {\rm m}^2_{\rm 32}$, $\sin^2 \theta_{23}$ (besides the…

High Energy Physics - Experiment · Physics 2022-07-15 Ajmi Ali

The T2K (Tokai to Kamioka) experiment is a second generation long baseline neutrino oscillation experiment located in Japan. The main goal is to probe the $\theta_{13}$ neutrino mixing parameter by looking for $\nu_{\mu}\to\nu_e$…

High Energy Physics - Experiment · Physics 2019-08-14 Alexander Izmaylov

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 a {\nu}_{\mu} beam. It also aims to make a…

Instrumentation and Detectors · Physics 2019-08-14 T2K Collaboration , K. Abe , N. Abgrall , H. Aihara , Y. Ajima , J. B. Albert , D. Allan , P. -A. Amaudruz , C. Andreopoulos , B. Andrieu , M. D. Anerella , C. Angelsen , S. Aoki , O. Araoka , J. Argyriades , A. Ariga , T. Ariga , S. Assylbekov , J. P. A. M. de André , D. Autiero , A. Badertscher , O. Ballester , M. Barbi , G. J. Barker , P. Baron , G. Barr , L. Bartoszek , M. Batkiewicz , F. Bay , S. Bentham , V. Berardi , B. E. Berger , H. Berns , I. Bertram , M. Besnier , J. Beucher , D. Beznosko , S. Bhadra , P. Birney , D. Bishop , E. Blackmore , F. d. M. Blaszczyk , J. Blocki , A. Blondel , A. Bodek , C. Bojechko , J. Bouchez , T. Boussuge , S. B. Boyd , M. Boyer , N. Braam , R. Bradford , A. Bravar , K. Briggs , J. D. Brinson , C. Bronner , D. G. Brook-Roberge , M. Bryant , N. Buchanan , H. Budd , M. Cadabeschi , R. G. Calland , D. Calvet , J. Caravaca Rodríguez , J. Carroll , S. L. Cartwright , A. Carver , R. Castillo , M. G. Catanesi , C. Cavata , A. Cazes , A. Cervera , J. P. Charrier , C. Chavez , S. Choi , S. Chollet , G. Christodoulou , P. Colas , J. Coleman , W. Coleman , G. Collazuol , K. Connolly , P. Cooke , A. Curioni , A. Dabrowska , I. Danko , R. Das , G. S. Davies , S. Davis , M. Day , X. De La Broise , P. de Perio , G. De Rosa , T. Dealtry , A. Debraine , E. Delagnes , A. Delbart , C. Densham , F. Di Lodovico , S. Di Luise , P. Dinh Tran , J. Dobson , J. Doornbos , U. Dore , O. Drapier , F. Druillole , F. Dufour , J. Dumarchez , T. Durkin , S. Dytman , M. Dziewiecki , M. Dziomba , B. Ellison , S. Emery , A. Ereditato , J. E. Escallier , L. Escudero , L. S. Esposito , W. Faszer , M. Fechner , A. Ferrero , A. Finch , C. Fisher , M. Fitton , R. Flight , D. Forbush , E. Frank , K. Fransham , Y. Fujii , Y. Fukuda , M. Gallop , V. Galymov , G. L. Ganetis , F. C. Gannaway , A. Gaudin , J. Gaweda , A. Gendotti , M. George , S. Giffin , C. Giganti , K. Gilje , I. Giomataris , J. Giraud , A. K. Ghosh , T. Golan , M. Goldhaber , J. J. Gomez-Cadenas , S. Gomi , M. Gonin , M. Goyette , A. Grant , N. Grant , F. Grañena , S. Greenwood , P. Gumplinger , P. Guzowski , M. D. Haigh , K. Hamano , C. Hansen , T. Hara , P. F. Harrison , B. Hartfiel , M. Hartz , T. Haruyama , R. Hasanen , T. Hasegawa , N. C. Hastings , S. Hastings , A. Hatzikoutelis , K. Hayashi , Y. Hayato , T. D. J. Haycock , C. Hearty , R. L. Helmer , R. Henderson , S. Herlant , N. Higashi , J. Hignight , K. Hiraide , E. Hirose , J. Holeczek , N. Honkanen , S. Horikawa , A. Hyndman , A. K. Ichikawa , K. Ieki , M. Ieva , M. Iida , M. Ikeda , J. Ilic , J. Imber , T. Ishida , C. Ishihara , T. Ishii , S. J. Ives , M. Iwasaki , K. Iyogi , A. Izmaylov , B. Jamieson , R. A. Johnson , K. K. Joo , G. Jover-Manas , C. K. Jung , H. Kaji , T. Kajita , H. Kakuno , J. Kameda , K. Kaneyuki , D. Karlen , K. Kasami , V. Kasey , I. Kato , H. Kawamuko , E. Kearns , L. Kellet , M. Khabibullin , M. Khaleeq , N. Khan , A. Khotjantsev , D. Kielczewska , T. Kikawa , J. Y. Kim , S. -B. Kim , N. Kimura , B. Kirby , J. Kisiel , P. Kitching , T. Kobayashi , G. Kogan , S. Koike , T. Komorowski , A. Konaka , L. L. Kormos , A. Korzenev , K. Koseki , Y. Koshio , Y. Kouzuma , K. Kowalik , V. Kravtsov , I. Kreslo , W. Kropp , H. Kubo , J. Kubota , Y. Kudenko , N. Kulkarni , L. Kurchaninov , Y. Kurimoto , R. Kurjata , Y. Kurosawa , T. Kutter , J. Lagoda , K. Laihem , R. Langstaff , M. Laveder , T. B. Lawson , P. T. Le , A. Le Coguie , M. Le Ross , K. P. Lee , M. Lenckowski , C. Licciardi , I. T. Lim , T. Lindner , R. P. Litchfield , A. Longhin , G. D. Lopez , P. Lu , L. Ludovici , T. Lux , M. Macaire , L. Magaletti , K. Mahn , Y. Makida , C. J. Malafis , M. Malek , S. Manly , A. Marchionni , C. Mark , A. D. Marino , A. J. Marone , J. Marteau , J. F. Martin , T. Maruyama , T. Maryon , J. Marzec , P. Masliah , E. L. Mathie , C. Matsumura , K. Matsuoka , V. Matveev , K. Mavrokoridis , E. Mazzucato , N. McCauley , K. S. McFarland , C. McGrew , T. McLachlan , I. Mercer , M. Messina , W. Metcalf , C. Metelko , M. Mezzetto , P. Mijakowski , C. A. Miller , A. Minamino , O. Mineev , S. Mine , R. E. Minvielle , G. Mituka , M. Miura , K. Mizouchi , J. -P. Mols , L. Monfregola , E. Monmarthe , F. Moreau , B. Morgan , S. Moriyama , D. Morris , A. Muir , A. Murakami , J. F. Muratore , M. Murdoch , S. Murphy , J. Myslik , G. Nagashima , T. Nakadaira , M. Nakahata , T. Nakamoto , K. Nakamura , S. Nakayama , T. Nakaya , D. Naples , B. Nelson , T. C. Nicholls , K. Nishikawa , H. Nishino , K. Nitta , F. Nizery , J. A. Nowak , M. Noy , Y. Obayashi , T. Ogitsu , H. Ohhata , T. Okamura , K. Okumura , T. Okusawa , C. Ohlmann , K. Olchanski , R. Openshaw , S. M. Oser , M. Otani , R. A. Owen , Y. Oyama , T. Ozaki , M. Y. Pac , V. Palladino , V. Paolone , P. Paul , D. Payne , G. F. Pearce , C. Pearson , J. D. Perkin , M. Pfleger , F. Pierre , D. Pierrepont , P. Plonski , P. Poffenberger , E. Poplawska , B. Popov , M. Posiadala , J. -M. 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Zalipska , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , J. Zmuda
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