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The first phase of the long-baseline neutrino experiment, LBNE10, will use a broadband, high-energy neutrino beam with a 10-kt liquid argon TPC at 1300 km to study neutrino oscillation. In this paper, we describe potential upgrades to…

High Energy Physics - Experiment · Physics 2013-07-04 M. Bishai , M. Diwan , S. Kettell , J. Stewart , R. Tschirhart , B. Viren , L. Whitehead , E. Worcester

The Deep Underground Neutrino Experiment (DUNE) is a next generation long baseline (1300 km) neutrino oscillation experiment. The neutrino beam measurements will be performed by a near detector (ND) and far detector (FD). The far detector…

Instrumentation and Detectors · Physics 2023-03-01 H. V. Souza

SNO+ is a large liquid scintillator-based experiment located 2km underground at SNOLAB, Sudbury, Canada. It reuses the Sudbury Neutrino Observatory detector, consisting of a 12m diameter acrylic vessel which will be filled with about 780…

Instrumentation and Detectors · Physics 2016-08-08 SNO+ Collaboration , : , S. Andringa , E. Arushanova , S. Asahi , M. Askins , D. J. Auty , A. R. Back , Z. Barnard , N. Barros , E. W. Beier , A. Bialek , S. D. Biller , E. Blucher , R. Bonventre , D. Braid , E. Caden , E. Callaghan , J. Caravaca , J. Carvalho , L. Cavalli , D. Chauhan , M. Chen , O. Chkvorets , K. Clark , B. Cleveland , I. T. Coulter , D. Cressy , X. Dai , C. Darrach , B. Davis-Purcell , R. Deen , M. M. Depatie , F. Descamps , F. Di Lodovico , N. Duhaime , F. Duncan , J. Dunger , E. Falk , N. Fatemighomi , R. Ford , P. Gorel , C. Grant , S. Grullon , E. Guillian , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , M. Hedayatipour , W. J. Heintzelman , R. L. Helmer , B. Hreljac , J. Hu , T. Iida , C. M. Jackson , N. A. Jelley , C. Jillings , C. Jones , P. G. Jones , K. Kamdin , T. Kaptanoglu , J. Kaspar , P. Keener , P. Khaghani , L. Kippenbrock , J. R. Klein , R. Knapik , J. N. Kofron , L. L. Kormos , S. Korte , C. Kraus , C. B. Krauss , K. Labe , I. Lam , C. Lan , B. J. Land , S. Langrock , A. LaTorre , I. Lawson , G. M. Lefeuvre , E. J. Leming , J. Lidgard , X. Liu , Y. Liu , V. Lozza , S. Maguire , A. Maio , K. Majumdar , S. Manecki , J. Maneira , E. Marzec , A. Mastbaum , N. McCauley , A. B. McDonald , J. E. McMillan , P. Mekarski , C. Miller , Y. Mohan , E. Mony , M. J. Mottram , V. Novikov , H. M. O'Keeffe , E. O'Sullivan , G. D. Orebi Gann , M. J. Parnell , S. J. M. Peeters , T. Pershing , Z. Petriw , G. Prior , J. C. Prouty , S. Quirk , A. Reichold , A. Robertson , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , M. A. Schumaker , M. H. Schwendener , D. Scislowski , J. Secrest , M. Seddighin , L. Segui , S. Seibert , T. Shantz , T. M. Shokair , L. Sibley , J. R. Sinclair , K. Singh , P. Skensved , A. Soerensen , T. Sonley , R. Stainforth , M. Strait , M. I. Stringer , R. Svoboda , J. Tatar , L. Tian , N. Tolich , J. Tseng , H. W. C. Tseung , R. Van Berg , E. Vázquez-Jáuregui , C. Virtue , B. von Krosigk , J. M. G. Walker , M. Walker , O. Wasalski , J. Waterfield , R. F. White , J. R. Wilson , T. J. Winchester , A. Wright , M. Yeh , T. Zhao , K. Zuber

An Optical Transition Radiation monitor has been developed for the proton beam-line of the T2K long base-line neutrino oscillation experiment. The monitor operates in the highly radioactive environment in proximity to the T2K target. It…

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

The determination of the missing $U_{e3}$ element (magnitude and phase) of the PMNS neutrino mixing matrix is possible via the detection of $\numu\to\nue$ oscillations at a baseline $L$ and energy $E$ given by the atmospheric observations,…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Meregaglia , A. Rubbia

Neutrino Factory is a facility for future precision studies of neutrino oscillations. A so called near detector is essential for reaching the aimed precision of neutrino oscillation analysis. Main task of the near detector is to measure the…

High Energy Physics - Experiment · Physics 2011-10-11 Rosen Matev , Roumen Tsenov

One of the most promising approaches for the next generation of neutrino experiments is the realization of large hybrid Cherenkov/scintillation detectors made possible by recent innovations in photodetection technology and liquid…

We report on the 3-year INFN ATLAS-CMS joint research activity in collaboration with FBK, started in 2014, and aimed at the development of new thin pixel detectors for the High Luminosity LHC Phase-2 upgrades. The program is concerned with…

Radiation detectors with noble gasses as the active medium are becoming increasingly common in experimental programs searching for physics beyond the standard model. Nearly all of these experiments rely to some degree on collecting…

Instrumentation and Detectors · Physics 2015-06-16 V. M. Gehman

A long-baseline neutrino-oscillation experiment using a well-defined neutrino beam is in preparation at KEK. Neutrinos generated at KEK will be detected by the Super-kamiokande detector 250 km away. The design of the neutrino beam line,…

High Energy Physics - Experiment · Physics 2009-09-25 Yuichi Oyama

The SciBath-768 detector is a prototype neutral particle detector offering high-precision reconstruction of neutrino and neutron events. It consists of a three dimensional grid of 768 wavelength-shifting fibers immersed in 82 liters of…

High Energy Physics - Experiment · Physics 2011-10-21 R. Cooper , L. Garrison , H. -O. Meyer , T. Mikev , L. Rebenitsch , R. Tayloe

The K2K (KEK to Kamioka) long-baseline neutrino-oscillation experiment was successfully started in early 1999. A total intensity of 7.20 x 10^18 protons on target, which is about 7% of the goal of the experiment, was accumulated in 39.4…

High Energy Physics - Experiment · Physics 2007-05-23 Yuichi Oyama

This paper presents a comprehensive optimisation study to maximise the light collection efficiency of scintillating cube elements used in the SoLid detector. Very short baseline reactor experiments, like SoLid, look for active to sterile…

The main irreducible background in the T2K $\nu_e$ appearance analysis is the $\nu_e$ contamination in the $\nu_\mu$ beam. In order to quantify this background, a selection for charged-current $\nu_e$ interactions in the near detector…

High Energy Physics - Experiment · Physics 2015-04-28 Luke Southwell

A novel low-energy ($\sim$few keV) neutrino-oscillation experiment NOSTOS, combining a strong tritium source and a high pressure spherical Time Projection Chamber (TPC) detector 10 m in radius has been recently proposed. The oscillation of…

Neutrino oscillations were discovered by atmospheric and solar neutrino experiments, and have been confirmed by experiments using neutrinos from accelerators and nuclear reactors. It has been found that there are large mixing angles in the…

High Energy Physics - Experiment · Physics 2009-10-23 Trung Le

The design and characteristics of the new very small angle neutron scattering spectrometer under construction at the Laboratoire Leon Brillouin is described. Its goal is to extend the range of scattering vectors magnitudes towards 2x10{-4}…

Soft Condensed Matter · Physics 2007-06-13 Sylvain Desert , Vincent Thevenot , Julian Oberdisse , Annie Brulet

Large-scale particle physics detectors often contain millions of repeated components, making precise and efficient quality control essential. We have developed a semiautomatic system for dimensional screening of 1 cm$^3$ plastic…

Instrumentation and Detectors · Physics 2026-03-31 Tatsuya Kikawa , Mao Tani , Atsuko K. Ichikawa , Tsunayuki Matsubara , Tsuyoshi Nakaya , Tomohisa Ogawa