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Related papers: Probing Nonstandard Neutrino Physics at T2KK

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The Kamioka-Korea two detector system is a powerful experimental setup for resolving neutrino parameter degeneracies and probing CP violation in neutrino oscillation. In this paper, we study sensitivities of this same setup to several…

High Energy Physics - Phenomenology · Physics 2008-11-26 Nei Cipriano Ribeiro , Takaaki Kajita , Pyungwon Ko , Hisakazu Minakata , Shoei Nakayama , Hiroshi Nunokawa

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

We discuss the possibility of constraining or discovering the non-standard neutrino physics beyond the standard model with future long baseline neutrino oscillation experiments. Among very many possible experimental set up we discuss…

High Energy Physics - Phenomenology · Physics 2010-04-21 Shoichi Uchinami

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

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

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

We study the matter effect caused by nonstandard neutrino interactions (NSI) in the next generation long-baseline neutrino experiments, DUNE, T2HK and T2HKK. If multiple NSI parameters are nonzero, the potential of these experiments to…

High Energy Physics - Phenomenology · Physics 2017-01-20 Jiajun Liao , Danny Marfatia , Kerry Whisnant

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

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

I try to give an overview of future prospects of the experimental exploration of the unknowns in the neutrino mass pattern and the lepton flavor mixing. Because of the nature of the lectures on which this manuscript is based, I give some…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hisakazu Minakata

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

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

I report some progress that occurred since NO-VE08 in the field of non-standard interactions (NSI) of neutrinos. After briefly reviewing theoretical developments, I give a summary of the two works in which I was involved. Firstly, we have…

High Energy Physics - Phenomenology · Physics 2009-05-12 Hisakazu Minakata

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

Neutrino oscillation in the matter could get affected by the sub-dominant, yet unknown, non-standard interactions. The upcoming long-baseline (LBL) neutrino experiments will be sensitive to these effects and can provide information on the…

High Energy Physics - Phenomenology · Physics 2023-02-21 Barnali Brahma , Anjan Giri

The future long baseline experiments such as DUNE and T2HKK have promising prospects to determine the neutrino mass hierarchy and measuring standard $CP$ phase $\delta$. However, presence of possible non-standard interactions of neutrinos…

High Energy Physics - Phenomenology · Physics 2020-10-15 Surender Verma , Shankita Bhardwaj

We discuss ways to explore non-standard interactions (NSI) which neutrinos may possess by expressing them as effective four Fermi operators with coefficient of the order of (M_{W} / M_{NP})^2 ~0.01 (0.0001) for energy scales of new physics…

High Energy Physics - Phenomenology · Physics 2008-05-19 Hisakazu Minakata

We discuss the possible implications of physics beyond the standard model in the neutrino sector applying non-standard interaction. Recently, the NOvA and T2K neutrino experiments have announced their measurements for the CP violating…

High Energy Physics - Phenomenology · Physics 2025-04-01 Anjan Giri

Neutrino-electron scatterings are purely leptonic processes with robust Standard Model (SM) predictions. Their measurements can therefore provide constraints to physics beyond SM. The $\nuebar$-e data taken at the Kuo-Sheng Reactor Neutrino…

High Energy Physics - Phenomenology · Physics 2014-11-21 M. Deniz er al. , TEXONO Collaboration

This paper investigates the capability of long-baseline experiments, which are making use of neutrinos that are coming from Japan Proton Accelerator Research Complex (J-PARC), in establishing the unitarity of active-neutrino mixing by…

High Energy Physics - Phenomenology · Physics 2022-01-26 C Soumya
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