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The T2K experiment reports updated measurements of neutrino and antineutrino oscillations using both appearance and disappearance channels. This result comes from an exposure of $14.9~(16.4) \times 10^{20}$ protons on target in neutrino…

High Energy Physics - Experiment · Physics 2021-06-23 T2K Collaboration , K. Abe , N. Akhlaq , R. Akutsu , A. Ali , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , Y. Awataguchi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , A. Beloshapkin , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , B. Bourguille , S. B. Boyd , A. Bravar , D. Bravo Bergu , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , S. Cao , S. L. Cartwright , M. G. Catanesi , A. Cervera , D. Cherdack , G. Christodoulou , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , D. Coplowe , A. Cudd , G. De Rosa , T. Dealtry , C. C. Delogu , S. R. Dennis , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , J. Dumarchez , P. Dunne , A. Eguchi , L. Eklund , S. Emery-Schrenk , A. Ereditato , A. J. Finch , G. Fiorillo , C. Francois , M. Friend , Y. Fujii , R. Fukuda , Y. Fukuda , K. Fusshoeller , C. Giganti , M. Gonin , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jes , P. Jonsson , C. K. Jung , P. B. Jurj , M. Kabirnezhad , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , J. Kisiel , T. Kobata , T. Kobayashi , L. Koch , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , K. Kowalik , Y. Kudenko , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , M. Lamoureux , D. Last , M. Laveder , M. Lawe , R. P. Litchfield , S. L. Liu , A. Longhin , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , L. Marti-Magro , T. Maruyama , T. Matsubara , K. Matsushita , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , A. Mefodiev , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , Th. A. Mueller , L. Munteanu , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , Y. Nishimura , E. Noah , T. S. Nonnenmacher , F. Nova , J. Nowak , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , K. Okumura , T. Okusawa , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , W. C. Parker , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , A. Pritchard , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , C. Riccio , E. Rondio , S. Roth , A. Rubbia , A. C. Ruggeri , C. Ruggles , A. Rychter , K. Sakashita , F. S , G. Santucci , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , K. Skwarczynski , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , R. Spina , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , M. Tajima , A. Takeda , Y. Takeuchi , H. K. Tanaka , Y. Tanihara , M. Tani , N. Teshima , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , S. Valder , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , T. Wachala , J. Walker , J. G. Walsh , Y. Wang , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , M. Yokoyama , T. Yoshida , Y. Yoshimoto , M. Yu , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , M. Ziembicki , M. Zito , S. Zsoldos

CP phase determination for the near future long baseline experiments, T2HK and DUNE, will require precise measurements of the oscillation probabilities. However, the uncertainty in the Earth's density must be considered in determining these…

High Energy Physics - Phenomenology · Physics 2023-03-22 Monojit Ghosh , Osamu Yasuda

The main aim of the T2K experiment in Japan is to discover CP violation in the leptonic sector by measuring the Dirac phase $\delta_{CP}$. For that purpose T2K has already started collecting data in both neutrino and antineutrino mode. But…

High Energy Physics - Phenomenology · Physics 2016-11-02 Monojit Ghosh

The main goal of the T2K long-baseline neutrino experiment is the precise measurement of the parameters of neutrino oscillation and the search for CP-violation in the lepton sector. In 2017, the T2K collaboration launched the Near Detector…

Instrumentation and Detectors · Physics 2020-08-26 S. Fedotov

We examine the use of two superbeam neutrino oscillation experiments with baselines $\lsim 1000$ km to resolve parameter degeneracies inherent in the three-neutrino analysis of such experiments. We find that with appropriate choices of…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , D. Marfatia , K. Whisnant

We present the numu to nue appearance and the numu disappearance results, using a total of 1.43 x 10^{20} protons on target collected with the T2K experiment. T2K is long baseline neutrino experiment in Japan with detectors located at…

High Energy Physics - Experiment · Physics 2019-08-14 Francesca Di Lodovico

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

Reactor antineutrino experiments have the ability to search for neutrino oscillations independent of reactor flux predictions using a relative measurement of the neutrino flux and spectrum across a range of baselines. The range of…

High Energy Physics - Experiment · Physics 2013-07-11 K. M. Heeger , B. R. Littlejohn , H. P. Mumm

After the KamLAND results, the remaining important targets in neutrino experiments are to measure still unknown 3 basic parameters; absolute neutrino mass scale, CP violation phase $\delta_{CP}$ and last mixing angle $\theta_{13}$. The…

High Energy Physics - Experiment · Physics 2017-08-23 F. Suekane , K. Inoue , T. Araki , K. Jongok

We present the first measurement of the muon neutrino spectrum at the T2K near detector, ND280, using the data collected at the JPARC acc\ elerator facility in Tokai, Japan. ND280 is located 280 meters downstream from the target and…

High Energy Physics - Experiment · Physics 2013-11-20 Melody Ravonel Salzgeber

This article extends the work of Bernabeu and Espinoza by examining the CP-violation reach of a $^{150}$Dy electron capture beam through the variation of the two Lorentz boosts, the number of useful electron capture decays, the relative run…

High Energy Physics - Phenomenology · Physics 2011-03-28 Christopher Orme

The current focus of the CERN program is the Large Hadron Collider (LHC), however, CERN is engaged in long baseline neutrino physics with the CNGS project and supports T2K as recognized CERN RE13, and for good reasons: a number of observed…

High Energy Physics - Phenomenology · Physics 2009-10-29 A. Rubbia

Time reversal (T) symmetry violations in neutrino oscillations imply the presence of an $L$-odd component in the transition probability at fixed neutrino energy, with $L$ denoting the distance between neutrino source and detector. Within…

High Energy Physics - Phenomenology · Physics 2025-12-11 Sabya Sachi Chatterjee , Sudhanwa Patra , Thomas Schwetz , Kiran Sharma

In this paper we study the synergy among the future accelerator (T2HK), future atmospheric (ICAL) and future reactor (JUNO) neutrino experiments to determine the neutrino mass ordering. T2HK can measure the mass ordering only for favorable…

High Energy Physics - Phenomenology · Physics 2023-02-07 Deepak Raikwal , Sandhya Choubey , Monojit Ghosh

One of the major open problems of neutrino physics is MO (mass ordering). We discuss the prospects of measuring MO with two under-construction experiments T2HK and JUNO. JUNO alone is expected to measure MO with greater than $3\sigma$…

High Energy Physics - Phenomenology · Physics 2022-12-28 Sandhya Choubey , Monojit Ghosh , Deepak Raikwal

Hyper-Kamiokande (Hyper-K) is a proposed next generation underground water Cherenkov (WCh) experiment. The far detector will measure the oscillated neutrino flux from the long-baseline neutrino experiment using 0.6 GeV neutrinos produced by…

Instrumentation and Detectors · Physics 2017-05-01 Greig Cowan , Evangelia Drakopoulou , Matthew Needham , Mahdi Taani

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

This paper presents studies of the performance of water-based liquid scintillator in both 1-kt and 50-kt detectors. Performance is evaluated in comparison to both pure water Cherenkov detectors and a nominal model for pure scintillator…

Instrumentation and Detectors · Physics 2021-03-16 B. J. Land , Z. Bagdasarian , J. Caravaca , M. Smiley , M. Yeh , G. D. Orebi Gann

The measurement of the neutrino mixing angle $\theta_{13}$ opens a gateway for the next generation experiments to measure the neutrino mass hierarchy and the leptonic CP-violating phase. Future reactor experiments will focus on mass…

Instrumentation and Detectors · Physics 2013-10-29 Miao He

Measuring the neutrino mixing parameter \ensuremath{\sin^2\theta_{13}} to the sub-percent precision level could be necessary in the next ten years for the precision unitary test of the PMNS matrix. In this work, we discuss the possibility…

High Energy Physics - Experiment · Physics 2023-03-17 Jinnan Zhang , Jun Cao
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