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The T2K experiment is a long-baseline neutrino oscillation experiment with the ability to measure precisely $\nu_{\mu}\rightarrow\nu_e$ and $\nu_{\mu}\rightarrow\nu_{\mu}$ oscillations. Control of systematic uncertainties-dominated by flux…

High Energy Physics - Experiment · Physics 2019-08-14 A. Kaboth

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 discovery of neutrino oscillations and the large mixing parameters in the Pontecorvo Maki Nakagawa Sakata matrix has opened a window to search for CP-violation in neutrinos. Two long-baseline neutrino experiments, DUNE and…

High Energy Physics - Experiment · Physics 2022-07-18 Blair Jamieson

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

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

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

We study the possibility of measuring T (time reversal) violation in a future long baseline neutrino oscillation experiment. By assuming a neutrino factory as a staging scenario of a muon collider at the J-PARC site, we find that the $\nu_e…

High Energy Physics - Phenomenology · Physics 2024-12-10 Ryuichiro Kitano , Joe Sato , Sho Sugama

Neutrino experiments at J-PARC are reviewed. After an introduction to neutrino physics, with emphasis on neutrino oscillation, the T2K experiment at the Main Ring neutrino beam line and its peripheral experiments are introduced. Also future…

High Energy Physics - Experiment · Physics 2021-04-14 Masahiro Kuze

The T2K experiment is a long-baseline accelerator neutrino experiment using a near detector complex ND280 and a far detector, Super-Kamiokande. Neutrino interactions are detected by Cherenkov light in Super-Kamiokande in order to measure…

High Energy Physics - Experiment · Physics 2019-08-14 L. Haegel

The measurements of the parameters of the neutrino mixing matrix in the present and future neutrino oscillation experiments at accelerators are presented. The perspectives for high intensity new neutrino facilities as SuperBeams, BetaBeams…

High Energy Physics - Phenomenology · Physics 2016-09-06 A. Guglielmi , M. Mezzetto , P. Migliozzi , F. Terranova

Neutrino oscillations are clear evidence for physics beyond the standard model. The goal of next-generation neutrino oscillation experiments is to find a non-zero $\theta_{13}$, the last mixing matrix element for which we only know an upper…

High Energy Physics - Experiment · Physics 2008-05-19 Teppei Katori

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 letter, we analyze for the first time the physics reach in terms of sensitivity to leptonic CP violation of the proposed MuOn-decay MEdium baseline NeuTrino beam (MOMENT) experiment, a novel neutrino oscillation facility that would…

High Energy Physics - Phenomenology · Physics 2016-05-04 Mattias Blennow , Pilar Coloma , Enrique Fernandez-Martinez

On 2010 MINOS experiment was showing an hint of possible different mass splitting and mixing angles for neutrinos and anti-neutrinos, suggesting a charge-parity-time (CPT) violation in the lepton sector; last year 2012 a second result from…

High Energy Physics - Phenomenology · Physics 2013-03-13 D. Fargion , D. D Armiento

Neutrino oscillation physics has entered the precision era and the potential forthcoming experiments Hyper-Kamiokande and Deep Under-ground Neutrino Experiment (DUNE) are expected to lead this endeavor. In this paper we perform a…

High Energy Physics - Phenomenology · Physics 2017-12-01 Kaustav Chakraborty , K. N. Deepthi , Srubabati Goswami

Hyper-Kamiokande consists of two identical water-Cherenkov detectors of total 520~kt with the first one in Japan at 295~km from the J-PARC neutrino beam with 2.5$^{\textrm{o}}$ Off-Axis Angles (OAAs), and the second one possibly in Korea in…

High Energy Physics - Experiment · Physics 2019-12-06 Hyper-Kamiokande proto-collaboration , : , K. Abe , Ke. Abe , S. H. Ahn , 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-Bergu no , F. d. M. Blaszczyk , A. Blondel , S. Bolognesi , S. B. Boyd , A. Bravar , C. Bronner , M. Buizza Avanzini , F. S. Cafagna , B. G. Cheon , M. K. Cheoun , K. Cho , K. Y. Choi , E. J. Chun , 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 , G. A. Fiorentini , G. Fiorillo , M. Fitton , K. Frankiewicz , M. Friend , Y. Fujii , Y. Fukuda , D. Fukuda , K. Ganezer , M. Ghosh , 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 , K. S. Jeong , M. Jiang , P. Jonsson , K. K. Joo , A. Kaboth , C. Kachulis , T. Kajita , S. K. Kang , J. Kameda , Y. Kataoka , T. Katori , K. Kayrapetyan , E. Kearns , M. Khabibullin , A. Khotjantsev , C. S. Kim , H. B. Kim , H. J. Kim , J. H. Kim , J. -S. Kim , J. Y. Kim , S. B. Kim , S. C. Kim , S. -W. Kim , S. Y. Kim , S. King , T. J. Kim , W. Kim , Y. Kishimoto , P. Ko , 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 , K. Kwak , E. H. Kwon , L. Labarga , J. Lagoda , P. J. J. Lasorak , M. Laveder , M. Lawe , J. G. Learned , C. H. Lee , S. J. Lee , W. J. Lee , 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 , C. S. Moon , 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 , Y. D. Oh , Y. Oh , 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 , H. S. Park , J. C. Park , M. G. Park , S. C. Park , 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 , M. Quinto , 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 , D. Ryu , R. Sacco , M. Sakuda , M. C. Sanchez , E. Scantamburlo , M. Scott , S. Molina Sedgwick , Y. Seiya , T. Sekiguchi , H. Sekiya , H. Seo , 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 , D. C. Son , 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 , E. Won , T. Xin , K. Yamamoto , C. Yanagisawa , T. Yano , O. Yasuda , S. Yen , N. Yershov , D. N. Yeum , M. Yokoyama , H. D. Yoo , J. Yoo , S. C. Yoon , T. S. Yoon , T. Yoshida , I. Yu , M. Yu , J. Zalipska , K. Zaremba , M. Ziembicki , M. Zito , S. Zsoldos

We consider the nu_mu to nu_e oscillation measurements that would be possible at upgraded 1 GeV and multi-GeV conventional neutrino sources driven by future megawatt-scale proton drivers. If these neutrino superbeams are used together with…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Barger

Effects of the Leptonic CP violating phase,\delta, on 3 generation neutrino oscillation rates and asymmetries are discussed. A figure of merit argument is used to show that our ability to measure the phase \delta is rather insensitive to…

High Energy Physics - Phenomenology · Physics 2007-05-23 William Marciano , Zohreh Parsa

New low-cost, high-power proton cyclotrons open the opportunity for a novel precision search for CP violation in the neutrino sector. The accelerators can produce decay-at-rest neutrino beams located at multiple distances from a Gd-doped…

High Energy Physics - Experiment · Physics 2010-04-14 J. M. Conrad , M. H. Shaevitz

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