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The T2K near-detector, ND280, employs three large argon gas TPCs (Time Projection Chambers) for particle tracking and identification. The gas inside the TPCs can be used as an active target to study the neutrino interactions in great…

Instrumentation and Detectors · Physics 2017-10-11 Lukas Koch

Liquid argon is an excellent medium for detecting particles, given its yields and transport properties of light and charge. The technology of liquid argon time projection chambers has reached its full maturity after four decades of…

High Energy Physics - Experiment · Physics 2024-05-03 Ettore Segreto

We propose to study atmospheric neutrino interactions with a unique event topology to distinguish neutrinos and anti-neutrinos using a liquid argon time projection chamber in an experiment such as DUNE. The detection of CC1P and CC0P events…

High Energy Physics - Phenomenology · Physics 2024-04-05 Animesh Chatterjee , Albert De Roeck

MiniBooNE seeks to confirm or refute the LSND muon-antineutrino to electron-antineutrino oscillation signal with high statistical significance and different systematics. MiniBooNE has accumulated the world's largest GeV neutrino data set.…

High Energy Physics - Experiment · Physics 2008-11-26 M. O. Wascko

The ICARUS liquid argon time projection chamber (LArTPC) neutrino detector has been taking physics data since 2022 as part of the Short-Baseline Neutrino (SBN) Program. This paper details the equalization of the response to charge in the…

High Energy Physics - Experiment · Physics 2024-08-06 ICARUS collaboration , P. Abratenko , N. Abrego-Martinez , A. Aduszkiewic , F. Akbar , L. Aliaga Soplin , M. Artero Pons , J. Asaadi , W. F. Badgett , B. Baibussinov , B. Behera , V. Bellini , R. Benocci , J. Berger , S. Berkman , S. Bertolucci , M. Betancourt , M. Bonesini , T. Boone , B. Bottino , A. Braggiotti , D. Brailsford , S. J. Brice , V. Brio , C. Brizzolari , H. S. Budd , A. Campani , A. Campos , D. Carber , M. Carneiro , I. Caro Terrazas , H. Carranza , F. Castillo Fernandez , A. Castro , S. Centro , G. Cerati , A. Chatterjee , D. Cherdack , S. Cherubini , N. Chitirasreemadam , M. Cicerchia , T. E. Coan , A. Cocco , M. R. Convery , L. Cooper-Troendle , S. Copello , A. A. Dange , A. de Roeck , S. Di Domizio , L. Di Noto , C. Di Stefano , D. Di Ferdinando , M. Diwan , S. Dolan , L. Domine , S. Donati , F. Drielsma , J. Dyer , S. Dytman , A. Falcone , C. Farnese , A. Fava , A. Ferrari , N. Gallice , F. G. Garcia , C. Gatto , D. Gibin , A. Gioiosa , W. Gu , A. Guglielmi , G. Gurung , H. Hausner , A. Heggestuen , B. Howard , R. Howell , I. Ingratta , C. James , W. Jang , Y. -J. Jwa , L. Kashur , W. Ketchum , J. S. Kim , D. -H. Koh , J. Larkin , Y. Li , C. Mariani , C. M. Marshall , S. Martynenko , N. Mauri , K. S. McFarland , D. P. Méndez , A. Menegolli , G. Meng , O. G. Miranda , A. Mogan , N. Moggi , E. Montagna , C. Montanari , A. Montanari , M. Mooney , G. Moreno-Granados , J. Mueller , M. Murphy , D. Naples , V. C. L. Nguyen , S. Palestini , M. Pallavicini , V. Paolone , R. Papaleo , L. Pasqualini , L. Patrizii , L. Paudel , G. Petrillo , C. Petta , V. Pia , F. Pietropaolo , F. Poppi , M. Pozzato , G. Putnam , X. Qian , A. Rappoldi , G. L. Raselli , S. Repetto , F. Resnati , A. M. Ricci , G. Riccobene , E. Richards , M. Rosenberg , M. Rossella , P. Roy , C. Rubbia , M. Saad , S. Saha , P. Sala , S. Samanta , P. Sapienza , A. Scaramelli , A. Scarpelli , D. Schmitz , A. Schukraft , D. Senadheera , S-H. Seo , F. Sergiampietri , G. Sirri , J. S. Smedley , J. Smith , L. Stanco , J. Stewart , H. A. Tanaka , F. Tapia , M. Tenti , K. Terao , F. Terranova , V. Togo , D. Torretta , M. Torti , F. Tortorici , R. Triozzi , Y. -T. Tsai , S. Tufanli , T. Usher , F. Varanini , S. Ventura , M. Vicenzi , C. Vignoli , B. Viren , Z. Williams , R. J. Wilson , P. Wilson , J. Wolfs , T. Wongjirad , A. Wood , E. Worcester , M. Wospakrik , H. Yu , J. Yu , A. Zani , J. Zennamo , J. Zettlemoyer , C. Zhang , S. Zucchelli

Due to their simplicity and comparatively low cost Resistive Plate Chambers are gaseous detectors widely used in high-energy and cosmic rays physics when large detection areas are needed. However, the best gaseous mixtures are currently…

Instrumentation and Detectors · Physics 2022-09-07 Alessandro Ferretti

The Argon Dark Matter (ArDM-1t) experiment is a ton-scale liquid argon (LAr) double-phase time projection chamber designed for direct Dark Matter searches. Such a device allows to explore the low energy frontier in LAr with a charge imaging…

This paper reports on a measurement of electron-ion recombination in liquid argon in the ICARUS liquid argon time projection chamber (LArTPC). A clear dependence of recombination on the angle of the ionizing particle track relative to the…

Instrumentation and Detectors · Physics 2025-06-11 ICARUS collaboration , P. Abratenko , N. Abrego-Martinez , A. Aduszkiewic , F. Akbar , L. Aliaga Soplin , M. Artero Pons , J. Asaadi , W. F. Badgett , B. Baibussinov , B. Behera , V. Bellini , R. Benocci , J. Berger , S. Berkman , S. Bertolucci , M. Betancourt , M. Bonesini , T. Boone , B. Bottino , A. Braggiotti , D. Brailsford , S. J. Brice , V. Brio , C. Brizzolari , H. S. Budd , A. Campani , A. Campos , D. Carber , M. Carneiro , I. Caro Terrazas , H. Carranza , F. Castillo Fernandez , A. Castro , S. Centro , G. Cerati , A. Chatterjee , D. Cherdack , S. Cherubini , N. Chitirasreemadam , M. Cicerchia , T. E. Coan , A. Cocco , M. R. Convery , L. Cooper-Troendle , S. Copello , A. A. Dange , A. de Roeck , S. Di Domizio , L. Di Noto , C. Di Stefano , D. Di Ferdinando , M. Diwan , S. Dolan , L. Domine , S. Donati , F. Drielsma , J. Dyer , S. Dytman , A. Falcone , C. Farnese , A. Fava , A. Ferrari , N. Gallice , F. G. Garcia , C. Gatto , D. Gibin , A. Gioiosa , W. Gu , A. Guglielmi , G. Gurung , H. Hausner , A. Heggestuen , B. Howard , R. Howell , I. Ingratta , C. James , W. Jang , Y. -J. Jwa , L. Kashur , W. Ketchum , J. S. Kim , D. -H. Koh , J. Larkin , Y. Li , C. Mariani , C. M. Marshall , S. Martynenko , N. Mauri , K. S. McFarland , D. P. Méndez , A. Menegolli , G. Meng , O. G. Miranda , A. Mogan , N. Moggi , E. Montagna , C. Montanari , A. Montanari , M. Mooney , G. Moreno-Granados , J. Mueller , M. Murphy , D. Naples , V. C. L. Nguyen , S. Palestini , M. Pallavicini , V. Paolone , R. Papaleo , L. Pasqualini , L. Patrizii , L. Paudel , G. Petrillo , C. Petta , V. Pia , F. Pietropaolo , F. Poppi , M. Pozzato , G. Putnam , X. Qian , A. Rappoldi , G. L. Raselli , S. Repetto , F. Resnati , A. M. Ricci , G. Riccobene , E. Richards , M. Rosenberg , M. Rossella , P. Roy , C. Rubbia , M. Saad , S. Saha , P. Sala , S. Samanta , P. Sapienza , A. Scaramelli , A. Scarpelli , D. Schmitz , A. Schukraft , D. Senadheera , S-H. Seo , F. Sergiampietri , G. Sirri , J. S. Smedley , J. Smith , L. Stanco , J. Stewart , H. A. Tanaka , F. Tapia , M. Tenti , K. Terao , F. Terranova , V. Togo , D. Torretta , M. Torti , F. Tortorici , R. Triozzi , Y. -T. Tsai , S. Tufanli , T. Usher , F. Varanini , S. Ventura , M. Vicenzi , C. Vignoli , B. Viren , Z. Williams , R. J. Wilson , P. Wilson , J. Wolfs , T. Wongjirad , A. Wood , E. Worcester , M. Wospakrik , H. Yu , J. Yu , A. Zani , J. Zennamo , J. Zettlemoyer , C. Zhang , S. Zucchelli

We report on the design and construction of a LED-based fiber calibration system for large liquid argon time projection detectors. This system was developed to calibrate the optical systems of the MicroBooNE experiment. As well as detailing…

Instrumentation and Detectors · Physics 2015-06-04 J. Conrad , B. J. P. Jones , Z. Moss , T. Strauss , M. Toups

One of the most convincing explanations of the LSND and MiniBooNE anomalies relies on a heavy, mostly sterile neutrino with a small muon neutrino component, which decays to an electron neutrino and an invisible light scalar field. We…

High Energy Physics - Phenomenology · Physics 2025-12-11 Sabya Sachi Chatterjee , Stéphane Lavignac , O. G. Miranda

We report the design, construction, and initial commissioning results of a large high pressure gaseous Time Projection Chamber (TPC) with Micromegas modules for charge readout. The detector vessel has an inner volume of about 600 L and an…

The net contribution of the strange quark spins to the proton spin, $\Delta s$, can be determined from neutral current elastic neutrino-proton interactions at low momentum transfer combined with data from electron-proton scattering. The…

High Energy Physics - Experiment · Physics 2019-08-13 Katherine Woodruff

We report measurements of annual and diurnal modulations of the cosmic-ray muon rate in the Yangyang underground laboratory (Y2L) using 952 days of COSINE-100 data acquired between September 2016 and July 2019. A correlation of the muon…

The measurement of the flux of muons produced in cosmic ray air showers is essential for the study of primary cosmic rays. Such measurements are important in extensive air shower detectors to assess the energy spectrum and the chemical…

High Energy Astrophysical Phenomena · Physics 2024-09-16 KM3NeT Collaboration

Cosmic-rays with energies up to $3\times10^{20}$ eV have been observed. The nuclear composition of these cosmic rays is unknown but if the incident nuclei are protons then the corresponding center of mass energy is $\sqrt{s_{nn}} = 700$…

Nuclear Experiment · Physics 2009-11-18 Spencer R. Klein

The 50~kton Iron Calorimeter (ICAL) detector at the underground India based Neutrino Observatory (INO) will make measurements on atmospheric neutrinos. Muons produced in charged current (CC) interactions of muon neutrinos with the iron are…

Instrumentation and Detectors · Physics 2014-10-22 N. Dash , V. M. Datar , G. Majumder

A search for millicharged particles, a simple extension of the standard model, has been performed with the ArgoNeuT detector exposed to the Neutrinos at the Main Injector beam at Fermilab. The ArgoNeuT Liquid Argon Time Projection Chamber…

A key feature for the success of the liquid Argon imaging TPC (LAr-TPC) technology is the industrial purification against electro-negative impurities, especially Oxygen and Nitrogen remnants, which have to be continuously kept at an…

Production of high-energy muons in cosmic-ray air showers, relevant for underground detectors, depends on the properties of the primary cosmic ray as well as the atmospheric temperature through the competition between decay and…

High Energy Astrophysical Phenomena · Physics 2021-07-26 Stef Verpoest , Thomas K. Gaisser

The Cryogenic Apparatus for Precision Tests of Argon Interactions with Neutrinos (CAPTAIN) is being built at Los Alamos National Laboratory. A hexagonal time projection chamber (TPC) with a 1 m drift length will be constructed inside a…

Instrumentation and Detectors · Physics 2013-09-11 Keith Rielage