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Two neutrino mixing angles have been measured, and much of the neutrino community is turning its attention to the unmeasured mixing angle, $\quq$, whose best limit comes from the reactor neutrino experiment CHOOZ.\cite{bib:chooz} New two…

High Energy Physics - Experiment · Physics 2007-06-06 Maury Goodman

Till 2010 we had three unknown parameters of neutrino oscillation: the third mixing angle {\theta}_(13), the sign of the larger mass difference {\Delta}m^(2)_(31) and the CP violating phase {\delta}. Thanks to a number of consistent…

High Energy Physics - Phenomenology · Physics 2015-06-16 D. P. Roy

This article represents quantitative numerical analysis to find the sensitivity for the mass ordering and octant of atmospheric mixing angle $\theta_{23}$ within 3$\sigma$ range of oscillation parameters, in the context of three long base…

High Energy Physics - Phenomenology · Physics 2017-06-21 Mandip Singh

This article presents the status of the art of the T2K experiment and the measurements prospects for the incoming years. After a brief description of the experiment, the most recent results will be illustrated. The observation of the…

High Energy Physics - Experiment · Physics 2016-09-08 M. G. Catanesi

In view of the evaluation of the physics goals of a large Liquid Argon TPC, evolving from the ICARUS technology, we have studied the possibility of performing precision measurements on atmospheric neutrinos. For this purpose we have…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Battistoni , A. Ferrari , C. Rubbia , P. R. Sala , F. Vissani

One of the most robust relationships predicted by binary tetrahedral ($T^{'}$) flavor symmetry relates the reactor neutrino angle $\theta_{13}$ to the atmospheric neutrino angle $\theta_{23}$, independently of $\theta_{12}$. It has the form…

High Energy Physics - Phenomenology · Physics 2017-07-06 Paul H. Frampton

We revisit correlations of neutrino oscillation parameters in reactor and long-baseline neutrino oscillation experiments. A framework based on an effective value of $\theta_{13}$ is presented, which can easily reproduce experimental…

High Energy Physics - Phenomenology · Physics 2018-04-25 Manfred Lindner , Werner Rodejohann , Xun-Jie Xu

A review of accelerator long-baseline neutrino oscillation experiments is provided, including all experiments performed to date and the projected sensitivity of those currently in progress. Accelerator experiments have played a crucial role…

High Energy Physics - Experiment · Physics 2013-05-09 G. J. Feldman , J. Hartnell , T. Kobayashi

A brief overview of the development of neutrino detectors for long-baseline oscillation experiments at accelerators and reactors is presented. Basic principles and main features of detectors of running accelerator experiments T2K and NOvA…

Instrumentation and Detectors · Physics 2017-06-28 Yury Kudenko

As discussed elsewhere, the measurement of a non-zero value for $\theta_{13}$ would open up a wide range of possibilities to explore CP-violation and the mass hierarchy. Experimental methods to measure currently the unknown mixing angle…

High Energy Physics - Experiment · Physics 2015-06-03 Zelimir Djurcic

In a recent work by 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 discuss how…

High Energy Physics - Phenomenology · Physics 2016-10-04 Kalpana Bora , Gayatri Ghosh , Debajyoti Dutta

Solar and atmospheric neutrino data require physics beyond the Standard Model of particle physics. The simplest, most generic, but not yet unique, interpretation of the data is in terms of neutrino oscillations. I summarize the results of…

Astrophysics · Physics 2007-05-23 J. W. F. Valle

We analyze the physics potential of long baseline neutrino oscillation experiments planned for the coming ten years, where the main focus is the sensitivity limit to the small mixing angle $\theta_{13}$. The discussed experiments include…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Huber , M. Lindner , M. Rolinec , T. Schwetz , W. Winter

In this addendum to arXiv:1103.0734 we consider the recent results from long-baseline $\nu_\mu\to\nu_e$ searches at the T2K and MINOS experiments and investigate their implications for the mixing angle $\theta_{13}$ and the leptonic Dirac…

High Energy Physics - Phenomenology · Physics 2015-05-30 Thomas Schwetz , Mariam Tortola , J. W. F. Valle

It is now widely accepted that a new middle baseline disappearance reactor neutrino experiment with multiple detectors could provide a clean measurement of the $\theta_{13}$ mixing angle, free from any parameter degeneracies and…

High Energy Physics - Experiment · Physics 2009-11-10 Th. Lasserre

Precisely measuring $\theta_{13}$ is one of the highest priority in neutrino oscillation study. Reactor experiments can cleanly determine $\theta_{13}$. Past reactor neutrino experiments are reviewed and status of next precision…

High Energy Physics - Experiment · Physics 2007-12-07 Jun Cao

The three-flavor neutrino oscillation paradigm is well established in particle physics thanks to the crucial contribution of accelerator neutrino beam experiments. In this paper we review the most important contributions of these…

High Energy Physics - Experiment · Physics 2020-02-13 M. Mezzetto , F. Terranova

We present an up-to-date global analysis of solar, atmospheric, reactor, and accelerator neutrino data in the framework of three-neutrino oscillations. We provide results on the determination of theta_13 from global data and discuss the…

High Energy Physics - Phenomenology · Physics 2013-01-04 M. C. Gonzalez-Garcia , Michele Maltoni , Jordi Salvado , Thomas Schwetz

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

We discuss the physics potential of intermediate $L \sim 20 \div 30$ km baseline experiments at reactor facilities, assuming that the solar neutrino oscillation parameters $\Delta m^2_{\odot}$ and $\theta_{\odot}$ lie in the high-LMA…

High Energy Physics - Phenomenology · Physics 2011-02-11 Sandhya Choubey , S. T. Petcov , M. Piai