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Plastic scintillator detectors have been extensively used in particle physics experiments for decades. A large-scale detector is typically arranged as an array of staggered long bars which provide a fast trigger signal and/or particle…

This paper summarizes the results from measurements aiming to characterize ultracold neutron detection with 6Li-doped glass scintillators. Single GS10 or GS20 scintillators, with a thickness of 100-200 micrometer, fulfill the ultracold…

The NeuLAND (New Large-Area Neutron Detector) plastic-scintillator-based time-of-flight detector for 0.1-1.6 GeV neutrons is currently under construction at the Facility for Antiproton and Ion Research (FAIR), Darmstadt, Germany. In its…

Instrumentation and Detectors · Physics 2023-01-11 Thomas Hensel , David Weinberger , Daniel Bemmerer , Konstanze Boretzky , Igor Gašparić , Daniel Stach , Andreas Wagner , Kai Zuber

The Universe is awash with tens-of-MeV neutrinos of all species coming from all past core-collapse supernovae. These have never been observed, but this state of affairs will change in the near future. In the less than ten years, the…

High Energy Physics - Phenomenology · Physics 2021-01-04 André de Gouvêa , Ivan Martinez-Soler , Yuber F. Perez-Gonzalez , Manibrata Sen

Neutrino oscillation experiments require a precise measurement of the neutrino energy. However, the kinematic detection of the final-state neutron in the neutrino interaction is missing in current neutrino oscillation experiments. The…

The K2K long-baseline neutrino oscillation experiment uses a Scintillating Fiber Detector (SciFi) to reconstruct charged particles produced in neutrino interactions in the near detector. We describe the track reconstruction algorithm and…

T2K is a long-baseline neutrino oscillation experiment, in which a muon-neutrino beam is directed over a 295 km baseline from the J-PARC facility to the Super-Kamiokande detector. This allows neutrino oscillation to be studied in two…

High Energy Physics - Experiment · Physics 2019-08-14 Kirsty Duffy

The nuGeN experiment searches for coherent elastic neutrino-nucleus scattering (CEvNS) at the Kalinin Nuclear Power Plant. A 1.41-kg high-purity low-threshold germanium detector surrounded by active and passive shielding is deployed at the…

The T2K (Tokai to Kamioka) experiment is a long-baseline accelerator neutrino oscillation experiment. Intense muon neutrino and antineutrino beams are produced at the J-PARC accelerator complex situated in Tokai. After 280 metres the beam…

High Energy Physics - Experiment · Physics 2018-05-11 Marcela Batkiewicz

A detector material or configuration that can provide an unambiguous indication of neutron capture can substantially reduce random coincidence backgrounds in antineutrino detection and capture-gated neutron spectrometry applications. Here…

Instrumentation and Detectors · Physics 2015-05-28 P. Nelson , N. S. Bowden

We report the first measurement of neutron capture multiplicity in neutrino-oxygen neutral-current quasi-elastic-like interactions at the gadolinium-loaded Super-Kamiokande detector using the T2K neutrino beam, which has a peak energy of…

High Energy Physics - Experiment · Physics 2025-06-02 T2K Collaboration , K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , M. Antonova , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , Y. Asada , Y. Ashida , N. Babu , G. Barr , D. Barrow , P. Bates , M. Batkiewicz-Kwasniak , V. Berardi , L. Berns , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , N. F. Calabria , S. Cao , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , P. S. Chong , A. Chvirova , G. Collazuol , F. Cormier , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , A. De Roeck , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , G. Fiorillo , M. D. Fitton , J. M. Franco Patiño , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , L. Giannessi , C. Giganti , V. Glagolev , M. Gonin , J. González Rosa , K. Gorshanov , M. Guigue , D. R. Hadley , J. T. Haigh , S. Han , D. A. Harris , T. Hasegawa , S. Hassani , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , M. Hogan , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , A. Izmaylov , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , P. Jonsson , S. Joshi , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , T. Koto , K. Kowalik , Y. Kudo , R. Kurjata , V. Kurochka , M. Kuze , M. La Commara , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , J. -F. Laporte , L. Lavitola , M. Lawe , Y. Lee , D. Leon Silverio , S. Levorato , S. V. Lewis , C. Lin , S. L. Liu , W. Li , A. Longhin , K. R. Long , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. Magaletti , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , A. D. Marino , D. G. R. Martin , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , J. McKean , A. Mefodiev , P. Mehta , L. Mellet , S. Miki , E. W. Miller , A. Minamino , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , Y. Oyama , V. Paolone , J. Pasternak , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez , P. N. Ratoff , M. Reh , C. Riccio , E. Rondio , S. Roth , N. Roy , L. Russo , A. Rychter , W. Saenz , K. Sakashita , E. M. Sandford , Y. Sato , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , K. Takifuji , H. K. Tanaka , H. Tanigawa , A. Teklu , V. V. Tereshchenko , N. Thamm , N. Tran , T. Tsukamoto , Y. Uchida , M. Vagins , M. Varghese , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , D. Wakabayashi , H. T. Wallace , J. G. Walsh , L. Wan , D. Wark , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , T. Yamamoto , T. Yamamoto , C. Yanagisawa , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

We propose modifying large water \v{C}erenkov detectors by the addition of 0.2% gadolinium trichloride, which is highly soluble, newly inexpensive, and transparent in solution. Since Gd has an enormous cross section for radiative neutron…

High Energy Physics - Phenomenology · Physics 2009-11-10 John F. Beacom , Mark R. Vagins

We propose the Hyper-Kamiokande (Hyper-K) detector as a next generation un- derground water Cherenkov detector. It will serve as a far detector of a long base- line neutrino oscillation experiment envisioned for the upgraded J-PARC beam,…

High Energy Physics - Experiment · Physics 2013-09-03 Kamiokande Working Group

The methodology and preliminary results for the search of single photons initiated by Neutral Current neutrino interactions with the ND280 detector at the T2K experiment are presented. This measurement aims to set the first limit on…

High Energy Physics - Experiment · Physics 2019-08-21 Pierre Lasorak

The SoLid experiment is a very-short-baseline experiment aimed at searching for nuclear reactor-produced active to sterile antineutrino oscillations. The detection principle is based on the pairing of two types of solid scintillators:…

Instrumentation and Detectors · Physics 2025-10-23 The SoLid collaboration

The nuGeN experiment is aimed to investigate neutrino properties using antineutrinos from the reactor of the Kalinin Nuclear Power Plant. The experimental setup is located at about 11 meters from the center of the 3.1 GWth reactor core.…

Since the Super-Kamiokande (SK) neutrino experiment in Japan added gadolinium sulphate octahydrate (Gd) to the pure water in its detector, it has entered a new era in supernova neutrino detection. The addition of Gd makes it possible to tag…

High Energy Astrophysical Phenomena · Physics 2024-04-02 L. Kneale

We discuss prospects for probing Z-prime and non-standard neutrino interactions using neutrino-nucleus coherent scattering with ultra-low energy (~ 10 eV) threshold Si and Ge detectors. The analysis is performed in the context of a specific…

High Energy Physics - Phenomenology · Physics 2016-03-04 Bhaskar Dutta , Rupak Mahapatra , Louis E. Strigari , Joel W. Walker

We propose a 3500 ton (3000 ton fiducial volume) SiO_2 neutrino detector with sampling calorimetry, charged particle tracking, and muon spectrometers to run in a Tevatron Fixed Target Program. Improvements to the Fermilab accelerator…

Riptide is a detector concept aiming to track fast neutrons. It is based on neutron--proton elastic collisions inside a plastic scintillator, where the neutron momentum can be measured by imaging the scintillation light. More specifically,…

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