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Neutrinos exhibit an interesting phenomenon called 'neutrino oscillation', in which a neutrino changes its flavor after traveling some flight length. Many experiments measured the mixing angles and mass differences, but the angle…

High Energy Physics - Experiment · Physics 2013-03-07 Masahiro Kuze

There is broad consensus in the worldwide physics community as to the need for a new reactor-neutrino experiment to measure or limit the neutrino mixing angle $\theta_{13}$. The Double Chooz Experiment, planned for operation in the years…

High Energy Physics - Experiment · Physics 2009-11-11 Daniel M. Kaplan

The next generation of long baseline neutrino experiments will aim at determining the value of the unknown mixing angle, theta_{13}, the type of neutrino mass hierarchy and the presence of CP-violation in the lepton sector. Beta-beams and…

High Energy Physics - Phenomenology · Physics 2009-06-19 J. Bernabeu , C. Espinoza , C. Orme , S. Palomares-Ruiz , S. Pascoli

Numbers of accelerator and reactor neutrino oscillation experiments aiming to search finite value of $\theta_{13}$ are starting within a few years. T2K experiment is a next generation long baseline neutrino experiment starts on 2009, in…

High Energy Physics - Experiment · Physics 2008-07-28 Y. Obayashi

The Double Chooz Reactor Neutrino Experiment in France plans to quickly measure the neutrino mixing angle theta-13, or limit it to sin^2 2-theta_13 less than 0.025. The physics reach, experimental site, detector structures, scintillator,…

High Energy Physics - Experiment · Physics 2007-05-23 Maury Goodman Thierry Lasserre

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. Poutissou , R. Poutissou , R. Preece , P. Przewlocki , W. Qian , J. L. Raaf , E. Radicioni , K. Ramos , P. Ratoff , T. M. Raufer , M. Ravonel , M. Raymond , F. Retiere , D. Richards , J. -L. Ritou , A. Robert , P. A. Rodrigues , E. Rondio , M. Roney , M. Rooney , D. Ross , B. Rossi , S. Roth , A. Rubbia , D. Ruterbories , R. Sacco , S. Sadler , K. Sakashita , F. Sanchez , A. Sarrat , K. Sasaki , P. Schaack , J. Schmidt , K. Scholberg , J. Schwehr , M. Scott , D. I. Scully , Y. Seiya , T. Sekiguchi , H. Sekiya , G. Sheffer , M. Shibata , Y. Shimizu , M. Shiozawa , S. Short , M. Siyad , D. Smith , R. J. Smith , M. Smy , J. Sobczyk , H. Sobel , S. Sooriyakumaran , M. Sorel , J. Spitz , A. Stahl , P. Stamoulis , O. Star , J. Statter , L. Stawnyczy , J. Steinmann , J. Steffens , B. Still , M. Stodulski , J. Stone , C. Strabel , T. Strauss , R. Sulej , P. Sutcliffe , A. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Y. Suzuki , Y. Suzuki , J. Swierblewski , T. Szeglowski , M. Szeptycka , R. Tacik , M. Tada , A. S. Tadepalli , M. Taguchi , S. Takahashi , A. Takeda , Y. Takenaga , Y. Takeuchi , H. A. Tanaka , K. Tanaka , M. Tanaka , M. M. Tanaka , N. Tanimoto , K. Tashiro , I. J. Taylor , A. Terashima , D. Terhorst , R. Terri , L. F. Thompson , A. Thorley , M. Thorpe , W. Toki , T. Tomaru , Y. Totsuka , C. Touramanis , T. Tsukamoto , V. Tvaskis , M. Tzanov , Y. Uchida , K. Ueno , M. Usseglio , A. Vacheret , M. Vagins , J. F. Van Schalkwyk , J. -C. Vanel , G. Vasseur , O. Veledar , P. Vincent , T. Wachala , A. V. Waldron , C. W. Walter , P. J. Wanderer , M. A. Ward , G. P. Ward , D. Wark , D. Warner , M. O. Wascko , A. Weber , R. Wendell , J. Wendland , N. West , L. H. Whitehead , G. Wikström , R. J. Wilkes , M. J. Wilking , Z. Williamson , J. R. Wilson , R. J. Wilson , K. Wong , T. Wongjirad , S. Yamada , Y. Yamada , A. Yamamoto , K. Yamamoto , Y. Yamanoi , H. Yamaoka , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , A. Zalewska , J. Zalipska , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , J. Zmuda

The pattern of oscillation parameters emerging from current experimental data can be further elucidated by the observation of matter effects. In contrast to planned experiments with conventional neutrino beams, atmospheric neutrinos offer…

High Energy Physics - Phenomenology · Physics 2011-09-13 T. Tabarelli de Fatis

Searches for mass-3 component in the electron neutrino flavor state $\sin{\theta}_{13}$ and for sterile neutrinos can be carried out in the same small mixing angle antineutrino oscillation experiment at a reactor. As an example we consider…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Kopeikin , L. Mikaelyan , V. Sinev

We discuss the potential to determine leading oscillation parameters, the value and the sign of \Delta m^2_{31}, as well as the magnitude of \sin^2 2\theta_{13} using a conventional wide band neutrino beam pointing to water or ice Cherenkov…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. Dick , M. Freund , P. Huber , M. Lindner

We study the physics potential of future long-baseline neutrino oscillation experiments at large $\theta_{13}$, focusing especially on systematic uncertainties. We discuss superbeams, \bbeams, and neutrino factories, and for the first time…

High Energy Physics - Phenomenology · Physics 2013-03-14 Pilar Coloma , Patrick Huber , Joachim Kopp , Walter Winter

We discuss reactor measurement of \theta_{12} which has a potential of reaching the ultimate sensitivity which surpasses all the methods so far proposed. The key is to place a detector at an appropriate baseline distance from the reactor…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Minakata , H. Nunokawa , W. J. C. Teves , R. Zukanovich Funchal

We review the potential of long and intermediate baseline reactor neutrino experiments in measuring the mass and mixing parameters. The KamLAND experiment can measure the solar mass squared difference very precisely. However it is not at…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sandhya Choubey

After the first measurement of the coherent elastic neutrino nucleus scattering (CENNS) by the COHERENT Collaboration, it is expected that new experiments will confirm the observation. Such measurements will allow to put stronger…

High Energy Physics - Phenomenology · Physics 2018-08-01 B. C. Cañas , E. A. Garcés , O. G. Miranda , A. Parada

Leptonic \textit{CP} violation search, neutrino mass hierarchy determination, and the precision measurement of oscillation parameters for a unitary test of the leptonic mixing matrix are among the major targets of the ongoing and future…

High Energy Physics - Phenomenology · Physics 2021-07-07 S. Cao , A. Nath , T. V. Ngoc , P. T. Quyen , N. T. Hong Van , Ng. K. Francis

We investigate how the data from various future neutrino oscillation experiments will constrain the physics parameters for a three active neutrino mixing model. The investigations properly account for the degeneracies and ambiguities…

High Energy Physics - Experiment · Physics 2009-09-09 Kendall B. M. Mahn , Michael H. Shaevitz

Neutrinos are elementary particles in the standard model of particle physics. There are 3 flavors of neutrinos that oscillate among themselves. Their oscillation can be described by a 3$\times$3 unitary matrix, containing three mixing…

High Energy Physics - Experiment · Physics 2015-06-19 Haoqi Lu

This presentation describes a precision result of the neutrino mixing parameter, $\sin^2 2\theta_{13}$, and the first direct measurement of the antineutrino mass-squared difference $\sin^2(\Delta_{ee}) \equiv \cos^2 \theta_{12} \sin^2…

High Energy Physics - Experiment · Physics 2019-08-13 Bei-Zhen Hu

The recent measurement of the reactor angle as $\sin^2 2\theta_{13} = 0.092 \pm 0.016(stat) \pm 0.005(syst)$ come from the Daya Bay collaboration. Evidence of nonzero \theta_{13} was also there at T2K, MINOS and Double Chooz experiments. We…

High Energy Physics - Phenomenology · Physics 2012-05-23 Swarup Kumar Majee

The RENO experiment recently reported the disappearance of reactor electron antineutrinos consistent with neutrino oscillations, with a significance of 4.9 standard deviations. The published ratio of observed to expected number of…

A lithium-based radiochemical detector is aimed primarily to detect neutrinos from CNO cycle what will provide a direct proof of its existence and will be a stringent test of the theory of stellar evolution. Another task which can be solved…

High Energy Physics - Phenomenology · Physics 2007-05-23 Anatoly Kopylov , Valery Petukhov
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