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Related papers: Liquid-Argon Time Projection Chambers in the U.S

200 papers

LArIAT (Liquid Argon In A Testbeam) aims to characterize the response of a liquid argon time projection chamber (LArTPC) to the particles often seen as final-state products of ~1 GeV neutrino interactions in existing and planned detectors.…

Instrumentation and Detectors · Physics 2015-11-04 William Foreman

In this paper we present results from a test of a small Liquid Argon Large Electron Multiplier Time Projection Chamber (LAr LEM-TPC). This detector concept provides a 3D-tracking and calorimetric device capable of charge amplification,…

Instrumentation and Detectors · Physics 2011-07-28 A. Badertscher , A. Curioni , S. Horikawa , L. Knecht , D. Lussi , A. Marchionni , G. Natterer , F. Resnati , A. Rubbia , T. Viant

The Liquid Argon Time Projection Chamber (LArTPC) is a prime type of detector for future large-mass neutrino observatories and proton decay searches. In this paper we present the design and operation, as well as experimental results from…

Instrumentation and Detectors · Physics 2015-06-15 A. Ereditato , C. C. Hsu , S. Janos , I. Kreslo , M. Messina , C. Rudolf von Rohr , B. Rossi , T. Strauss , M. S. Weber , M. Zeller

The capabilities of liquid argon time projection chambers (LArTPCs) to reconstruct the spatial and calorimetric information of neutrino events have made them the detectors of choice in a number of experiments, specifically those looking to…

The dual phase Liquid Argon Time Projection Chamber (LAr TPC) is the state-of-art technology for neutrino detection thanks to its superb 3D tracking and calorimetry performance. Its main feature is the charge amplification in gas argon…

Instrumentation and Detectors · Physics 2019-08-14 Sebastien Murphy

The Liquid Argon Time Projection Chamber (LAr-TPC) detectors provide excellent imaging and particle identification ability for studying neutrinos. An efficient and automatic reconstruction procedures are required to exploit potential of…

Computer Vision and Pattern Recognition · Computer Science 2015-03-02 Piotr Płoński , Dorota Stefan , Robert Sulej , Krzysztof Zaremba

We present the results of the first exposure of a Liquid Argon TPC to a multi-GeV neutrino beam. The data have been collected with a 50 liters ICARUS-like chamber located between the CHORUS and NOMAD experiments at the CERN West Area…

Instrumentation and Detectors · Physics 2008-11-26 F. Arneodo et al.

Neutrinos are one of the least known elementary particles. The detection of neutrinos is an extremely difficult task since they are affected only by weak sub-atomic force or gravity. Therefore large detectors are constructed to reveal…

Computer Vision and Pattern Recognition · Computer Science 2015-05-05 Piotr Płoński , Dorota Stefan , Robert Sulej , Krzysztof Zaremba

A good understanding of the cross sections for neutrino interactions with nucleons and nuclei is crucial for neutrino oscillation studies, in addition to providing a tool for the exploration of nucleon and nuclear structures. The MicroBooNE…

High Energy Physics - Experiment · Physics 2018-10-15 Vassili Papavassiliou

We investigate the potential of Liquid Argon (LAr) neutrino detectors to search for millicharged particles, a well-motivated extension of the standard model. Detectors located downstream of an intense proton beam that is striking a target…

High Energy Physics - Phenomenology · Physics 2019-08-02 Roni Harnik , Zhen Liu , Ornella Palamara

A 10 kilo-tonne dual-phase liquid argon TPC is one of the detector options considered for the Deep Underground Neutrino Experiment (DUNE). The detector technology relies on amplification of the ionisation charge in ultra-pure argon vapour…

Instrumentation and Detectors · Physics 2018-11-14 B. Aimard , Ch. Alt , J. Asaadi , M. Auger , V. Aushev , D. Autiero , M. M. Badoi , A. Balaceanu , G. Balik , L. Balleyguier , E. Bechetoille , D. Belver , A. M. Blebea-Apostu , S. Bolognesi , S. Bordoni , N. Bourgeois , B. Bourguille , J. Bremer , G. Brown , G. Brunetti , L. Brunetti , D. Caiulo , M. Calin , E. Calvo , M. Campanelli , K. Cankocak , C. Cantini , B. Carlus , B. M. Cautisanu , M. Chalifour , A. Chappuis , N. Charitonidis , A. Chatterjee , A. Chiriacescu , P. Chiu , S. Conforti , P. Cotte , P. Crivelli , C. Cuesta , J. Dawson , I. De Bonis , C. De La Taille , A. Delbart , D. Desforge , S. Di Luise , B. S. Dimitru , F. Doizon , C. Drancourt , D. Duchesneau , F. Dulucq , J. Dumarchez , F. Duval , S. Emery , A. Ereditato , T. Esanu , A. Falcone , K. Fusshoeller , A. Gallego-Ros , V. Galymov , N. Geroy , A. Gendotti , M. Gherghel-Lascu , C. Giganti , I. Gil-Botella , C. Girerd , M. C. Gomoiu , P. Gorodetzky , E. Hamada , R. Hanni , T. Hasegawa , A. Holin , S. Horikawa , M. Ikeno , S. Jimenez , A. Jipa , M. Karolak , Y. Karyotakis , S. Kasai , K. Kasami , T. Kishishita , I. Kreslo , D. Kryn , C. Lastoria , I. Lazanu , G. Lehmann-Miotto , N. Lira , K. Loo , D. Lorca , P. Lutz , T. Lux , J. Maalampi , G. Maire , M. Maki , L. Manenti , R. M. Margineanu , J. Marteau , G. Martin-Chassard , H. Mathez , E. Mazzucato , G. Misitano , B. Mitrica , D. Mladenov , L. Molina Bueno , C. Moreno Martinez , J. P. Mols , T. S. Mosu , W. Mug , A. Munteanu , S. Murphy , K. Nakayoshi , S. Narita , D. Navas-Nicolas , K. Negishi , M. Nessi , M. Niculescu-Oglinzanu , L. Nita , F. Noto , A. Noury , Y. Onishchuk , C. Palomares , M. Parvu , T. Patzak , Y. Penichot , E. Pennacchio , L. Periale , H. Pessard , F. Pietropaolo , Y. Piret , B. Popov , D. Pugnere , B. Radics , D. Redondo , C. Regenfus , A. Remoto , F. Resnati , Y. A. Rigaut , C. Ristea , A. Rubbia , A. Saftoiu , K. Sakashita , F. Sanchez , C. Santos , A. Scarpelli , C. Schloesser , L. Scotto Lavina , K. Sendai , F. Sergiampietri , S. Shahsavarani , M. Shoji , J. Sinclair , J. Soto-Oton , D. L. Stanca , D. Stefan , P. Stroescu , R. Sulej , M. Tanaka , V. Toboaru , A. Tonazzo , W. Tromeur , W. H. Trzaska , T. Uchida , F. Vannucci , G. Vasseur , A. Verdugo , T. Viant , S. Vihonen , S. Vilalte , M. Weber , S. Wu , J. Yu , L. Zambelli , M. Zito

The MicroBooNE experiment is a 170 ton Liquid Argon Time Projection Chamber (LArTPC) that will begin running at Fermilab in 2013. Its primary physics goal is to explore the low energy excess of events seen by the MiniBooNE experiment and it…

Instrumentation and Detectors · Physics 2011-10-10 C. M. Ignarra

We present a real-time anomaly detection framework for liquid argon time projection chambers (LArTPCs), targeting applications in particle physics experiments such as the Short Baseline Near Detector or the future Deep Underground Neutrino…

High Energy Physics - Experiment · Physics 2026-05-28 Seokju Chung , Jack Cleeve , Akshay Malige , Georgia Karagiorgi , Lino Gerlach , Adrian A. Pol , Isobel Ojalvo

The Liquid Argon Time Projection Chamber offers an innovative technology for a new class of massive detectors for rare-event detection. It is a precise tracking device that allows three-dimensional spatial reconstruction with mm-scale…

Instrumentation and Detectors · Physics 2015-06-15 A. Rubbia

The MicroBooNE experiment is designed to observe interactions of neutrinos with a Liquid Argon Time Projection Chamber (LArTPC) detector from the on-axis Booster Neutrino Beam (BNB) and off-axis Neutrinos at the Main Injector (NuMI) beam at…

Instrumentation and Detectors · Physics 2015-11-03 Jyoti Joshi , Xin Qian

Modelling and reconstructing neutrino-nucleus scattering is difficult, but it is crucial to do it precisely to enable next-generation oscillation measurements. Liquid argon time projection chambers (LArTPCs), such as MicroBooNE, can be the…

High Energy Physics - Experiment · Physics 2025-06-05 Holly B. Parkinson , for the MicroBooNE Collaboration

The Argon Dark Matter (ArDM) experiment consists of a liquid argon (LAr) time projection chamber (TPC) sensitive to nuclear recoils resulting from scattering of hypothetical Weakly Interacting Massive Particles (WIMPs) on argon targets.…

Neutrinos are particles that interact rarely, so identifying them requires large detectors which produce lots of data. Processing this data with the computing power available is becoming more difficult as the detectors increase in size to…

Instrumentation and Detectors · Physics 2021-02-03 Sophie Berkman , Giuseppe Cerati , Brian Gravelle , Boyana Norris , Allison Reinsvold Hall , Michael Wang

In this paper, we consider the physics performance of a single far detector composed of a 100 kton next generation Liquid Argon Time Projection Chamber (LAr TPC) possibly located at shallow depth, coupled to the J-PARC neutrino beam…

High Energy Physics - Phenomenology · Physics 2008-04-15 A. Badertscher , T. Hasegawa , T. Kobayashi , A. Marchionni , A. Meregaglia , T. Maruyama , K. Nishikawa , A. Rubbia