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The subject of space charge in ionisation detectors is reviewed, with particular attention to the case of liquid argon time projection chambers. Analytical and numerical description of the effects on the reconstructed coordinates along the…

Instrumentation and Detectors · Physics 2021-02-12 Sandro Palestini , Filippo Resnati

Liquid argon detectors are ubiquitous in particle, astroparticle, and applied physics. They reached an unprecedented level of maturity thanks to more than 20 years of R&D and the operation of large-scale facilities at CERN, Fermilab, and…

Instrumentation and Detectors · Physics 2024-10-30 W. M. Bonivento , F. Terranova

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

This paper describes the design and construction of the MicroBooNE liquid argon time projection chamber and associated systems. MicroBooNE is the first phase of the Short Baseline Neutrino program, located at Fermilab, and will utilize the…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE Collaboration , R. Acciarri , C. Adams , R. An , A. Aparicio , S. Aponte , J. Asaadi , M. Auger , N. Ayoub , L. Bagby , B. Baller , R. Barger , G. Barr , M. Bass , F. Bay , K. Biery , M. Bishai , A. Blake , V. Bocean , D. Boehnlein , V. D. Bogert , T. Bolton , L. Bugel , C. Callahan , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , S. Chappa , H. Chen , K. Chen , C. Y. Chi , C. S. Chiu , E. Church , D. Cianci , G. H. Collin , J. M. Conrad , M. Convery , J. Cornele , P. Cowan , J. I. Crespo-Anadon , G. Crutcher , C. Darve , R. Davis , M. Del Tutto , D. Devitt , S. Duffin , S. Dytman , B. Eberly , A. Ereditato , D. Erickson , L. Escudero Sanchez , J. Esquivel , S. Farooq , J. Farrell , D. Featherston , B. T. Fleming , W. Foreman , A. P. Furmanski , V. Genty , M. Geynisman , D. Goeldi , B. Goff , S. Gollapinni , N. Graf , E. Gramellini , J. Green , A. Greene , H. Greenlee , T. Griffin , R. Grosso , R. Guenette , A. Hackenburg , R. Haenni , P. Hamilton , P. Healey , O. Hen , E. Henderson , V Hewes , C. Hill , K. Hill , L. Himes , J. Ho , G. Horton-Smith , D. Huffman , C. M. Ignarra , C. James , E. James , J. Jan de Vries , W. Jaskierny , C. M. Jen , L. Jiang , B. Johnson , M. Johnson , R. A. Johnson , B. J. P. Jones , J. Joshi , H. Jostlein , D. Kaleko , L. N. Kalousis , G. Karagiorgi , T. Katori , P. Kellogg , W. Ketchum , J. Kilmer , B. King , B. Kirby , M. Kirby , E. Klein , T. Kobilarcik , I. Kreslo , R. Krull , R. Kubinski , G. Lange , F. Lanni , A. Lathrop , A. Laube , W. M. Lee , Y. Li , D. Lissauer , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , G. Lukhanin , M. Luethi , B. Lundberg , X. Luo , G. Mahler , I. Majoros , D. Makowiecki , A. Marchionni , C. Mariani , D. Markley , J. Marshall , D. A. Martinez Caicedo , K. T. McDonald , D. McKee , A. McLean , J. Mead , V. Meddage , T. Miceli , G. B. Mills , W. Miner , J. Moon , M. Mooney , C. D. Moore , Z. Moss , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , B. Norris , N. Norton , J. Nowak , M. OBoyle , T. Olszanowski , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , R. Pelkey , M. Phipps , S. Pordes , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , R. A Rameika , B. Rebel , R. Rechenmacher , S. Rescia , L. Rochester , C. Rudolf von Rohr , A. Ruga , B. Russell , R. Sanders , W. R. Sands , M. Sarychev , D. W. Schmitz , A. Schukraft , R. Scott , W. Seligman , M. H. Shaevitz , M. Shoun , J. Sinclair , W. Sippach , T. Smidt , A. Smith , E. L. Snider , M. Soderberg , M. Solano-Gonzalez , S. Soldner-Rembold , S. R. Soleti , J. Sondericker , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , K. Sutton , A. M. Szelc , K. Taheri , N. Tagg , K. Tatum , J. Teng , K. Terao , M. Thomson , C. Thorn , J. Tillman , M. Toups , Y. T. Tsai , S. Tufanli , T. Usher , M. Utes , R. G. Van de Water , C. Vendetta , S. Vergani , E. Voirin , J. Voirin , B. Viren , P. Watkins , M. Weber , T. Wester , J. Weston , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , K. C. Wu , T. Yang , B. Yu , G. P. Zeller , J. Zennamo , C. Zhang , M. Zuckerbrot

LArGO (Liquid Argon Gamma-ray Observatory) consists of a new design for a $\gamma$-ray telescope, which exploits the idea of using a Liquid Argon Time Projection Chamber (LAr-TPC) as tracker-converter. Particle tracking in LAr-TPC can…

Instrumentation and Methods for Astrophysics · Physics 2013-12-17 Giuseppe Andrea Caliandro , Biagio Rossi , Francesco Longo , Giuliana Fiorillo , Claudio Labanti , Federico Sanchez , Thorsten Lux

Liquid Argon Time Projection Chamber detectors are ideally suited for studying neutrino interactions and probing the parameters that characterize neutrino oscillations. The ability to drift ionization particles over long distances in…

Instrumentation and Detectors · Physics 2009-10-20 M. Soderberg

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 $3 \times 1 \times 1$ m$^3$ demonstrator is a dual phase liquid argon time projection chamber that has recorded cosmic rays events in 2017 at CERN. The light signal in these detectors is crucial to provide precise timing capabilities.…

Instrumentation and Detectors · Physics 2021-03-24 B. Aimard , L. Aizawa , C. Alt , J. Asaadi , M. Auger , V. Aushev , D. Autiero , 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. Chiriacescuf , P. Chiu , S. Conforti , P. Cotte , P. Crivelli , C. Cuesta , J. Dawson , I. De Bonis , C. De La Taille , A. Delbart , S. Di Luise , F. Doizon , C. Drancourt , D. Duchesneau , F. Dulucq , F. Duval , S. Emery , A. Ereditato , A. Falcone , K. Fusshoeller , A. Gallego-Ros , V. Galymov , N. Geffroy , A. Gendotti , A. Gherghel-Lascu , I. Gil-Botella , C. Girerd , M. C. Gomoiu , P. Gorodetzky , E. Hamada , R. Hanni , T. Hasegawa , A. Holin , S. Horikawa , M. Ikeno , S. Jiménez , A. Jipa , M. Karolak , Y. Karyotakis , S. Kasai , K. Kasami , T. Kishishita , H. Konari , I. Kreslo , D. Kryn , P. Kunzé , M. Kurokawa , Y. Kuromori , C. Lastoria , I. Lazanu , G. Lehmann-Miotto , M. Leyton , 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 , D. Mladenov , L. Molina Bueno , T. S. Mosu , W. Mu , S. Murphy , K. Nakayoshi , S. Narita , D. Navas-Nicolás , K. Negishi , M. Nessi , M. Niculescu-Oglinzanu , F. Noto , A. Noury , Y. Onishchuk , C. Palomares , M. Parvu , T. Patzak , Y. Penichot , E. Pennacchio , L. Periale , H. Pessard , F. Pietropaolo , D. Pugnere , B. Radics , D. Redondo , C. Regenfus , A. Remoto , F. Resnati , O. Ristea , A. Rubbia , A. Saftoiu , K. Sakashita , F. Sanchez , C. Santos , A. Scarpelli , C. Schloesser , K. Sendai , F. Sergiampietri , S. Shahsavarani , M. Shoji , J. Sinclair , J. Soto-Oton , D. I. Stanca , D. Stefan , R. Sulej , M. Tanaka , V. Toboaru , A. Tonazzo , W. Tromeur , W. H. Trzaska , T. Uchida , L. Urda , F. Vannucci , G. Vasseur , A. Verdugo , T. Viant , S. Vihonen , S. Vilalte , M. Weber , S. Wu , J. Yu , L. Zambelli , M. Zito

A Nd:YAG laser was used to simulate charged particle tracks at known positions in the CERES Time Projection Chamber at the CERN SPS. The system was primarily developed to study the response of the readout electronics and to calibrate the…

Nuclear Experiment · Physics 2008-11-26 Dariusz Miskowiec , Peter Braun-Munzinger

The ICARUS detector is a liquid argon time projection chamber. It provides three dimensional imaging and calorimetry of ionizing particles over a large volume, with high granularity. Its Physics program includes the study of atmospheric,…

High Energy Physics - Experiment · Physics 2019-08-14 Javier Rico

We have previously reported on the construction and successful operation of the novel double phase Liquid Argon Large Electron Multiplier Time Projection Chamber (LAr LEM-TPC). This detector concept provides a 3D-tracking and calorimetric…

Instrumentation and Detectors · Physics 2015-03-17 A. Badertscher , A. Curioni , L. Knecht , D. Lussi , A. Marchionni , G. Natterer , F. Resnati , A. Rubbia , T. Viant

After a short review of previous attempts to observe and measure the near-infrared scintillation in liquid argon, we present new results obtained with NIR, a dedicated cryostat at the Fermilab Proton Assembly Building (PAB). The new results…

Instrumentation and Detectors · Physics 2018-03-22 C. O. Escobar , P. Rubinov , E. Tilly

The liquid argon time projection chamber (LArTPC) detector technology provides an opportunity for precision neutrino oscillation measurements, neutrino cross section measurements, and searches for rare processes, such as SuperNova neutrino…

Instrumentation and Detectors · Physics 2013-04-09 Georgia Karagiorgi

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. After successful…

Results are presented from a small-scale experiment to investigate the use of room temperature organic liquid scintillators as the active medium for a time projection chamber (TPC). The optical properties of liquid scintillators have long…

Instrumentation and Detectors · Physics 2015-06-05 N. McConkey , Y. A. Ramachers

We successfully operated a novel kind of LAr Time Projection Chamber based on a Large Electron Multiplier (LEM) readout system. The prototype, of about 3 liters active volume, is operated in liquid-vapour (double) phase pure Ar. The…

Instrumentation and Detectors · Physics 2008-11-21 A. Badertscher , L. Knecht , M. Laffranchi , A. Marchionni , G. Natterer , P. Otiougova , F. Resnati , A. Rubbia

Large volume Liquid Argon Time Projection Chambers (LAr-TPC) are used and proposed for neutrino physics and rare event search. Most of these detectors make use of the scintillation light of liquid argon for trigger purposes. Two different…

Instrumentation and Detectors · Physics 2020-04-13 O. Barnabà , A. Menegolli , R. Nardò , M. Pirola , M. C. Prata , G. L. Raselli , E. Romano , M. Rossella

Beam dump experiments proposed at the SPS are perfectly suited to explore the parameter space of models with long-lived particles, thanks to the combination of a large intensity with a high proton beam energy. In this paper, we study how…

High Energy Physics - Phenomenology · Physics 2024-03-08 Martina Ferrillo , Maksym Ovchynnikov , Filippo Resnati , Albert De Roeck

We describe in these GLA2011 proceedings the software package LArSoft, a toolkit to perform simulation, analysis and reconstruction with the Liquid Argon (LAr) Time Projection Chambers (TPCs) within the US program of proposed detectors. We…

Instrumentation and Detectors · Physics 2014-01-09 Eric D. Church

Liquid Argon time projection chamber (LArTPC) is a promising detector technology for future neutrino experiments. MicroBooNE is an upcoming LArTPC neutrino experiment which will be located on-axis of Booster Neutrino Beam (BNB) at Fermilab,…

High Energy Physics - Experiment · Physics 2015-05-28 Teppei Katori