English
Related papers

Related papers: The Yale Lar TPC

200 papers

In this paper, we show that a hybrid approach to generative modeling via combining the decoder from an autoencoder together with an explicit generative model for the latent space is a promising method for producing images of particle…

High Energy Physics - Experiment · Physics 2022-04-07 Paul Lutkus , Taritree Wongjirad , Shuchin Aeron

For the International Large Detector concept at the planned International Linear Collider, the use of time projection chambers (TPC) with micro-pattern gas detector readout as the main tracking detector is investigated. In this paper,…

A time projection chamber (TPC) can be used to measure the polarization of gamma rays with excellent angular precision and sensitivity in the MeV-GeV energy range through the conversion of photons to e+e- pairs. The Hermetic ARgon…

Tests with cosmic ray muons of a small liquid argon time projection chamber (LAr TPC) in a magnetic field of 0.55 T are described. No effect of the magnetic field on the imaging properties were observed. In view of a future large,…

Instrumentation and Detectors · Physics 2011-07-28 A. Badertscher , L. Knecht , M. Laffranchi , G. Natterer , A. Rubbia , Th. Strauss

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

Mature technology of Liquid Argon Time Projection Chambers in conjunction with intense neutrino beams constructed at Fermilab offer a broad program of neutrino physics for the next decade.

High Energy Physics - Experiment · Physics 2009-09-29 L. Bartoszek

The 50 liter liquid Argon TPC is a detector built and successfully operated at CERN for R&D purposes within the ICARUS programme. In the year 1997 it has been exposed at the CERN neutrino beam for the entire SPS neutrino run period as…

High Energy Physics - Experiment · Physics 2012-08-27 The ICARUS Collaboration

The ICARUS T600, a liquid argon time projection chamber (LAr-TPC) detector mainly devoted to neutrino physics, underwent a major overhauling at CERN in 2016-2017, which included also a new design of the read-out electronics, in view of its…

Liquid argon time projection chambers (LArTPCs) are now a standard detector technology for making accelerator neutrino measurements, due to their high material density, precise tracking, and calorimetric capabilities. An electric field…

Instrumentation and Detectors · Physics 2020-08-26 MicroBooNE collaboration , C. Adams , M. Alrashed , R. An , J. Anthony , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , C. Barnes , G. Barr , V. Basque , M. Bass , F. Bay , S. Berkman , A. Bhanderi , A. Bhat , M. Bishai , A. Blake , T. Bolton , L. Camilleri , D. Caratelli , I. Caro Terrazas , R. Carr , R. Castillo Fernandez , F. Cavanna , G. Cerati , Y. Chen , E. Church , D. Cianci , E. O. Cohen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , M. Del Tutto , D. Devitt , A. Diaz , L. Domine , K. Duffy , S. Dytman , B. Eberly , A. Ereditato , L. Escudero Sanchez , J. J. Evans , R. S. Fitzpatrick , B. T. Fleming , N. Foppiani , D. Franco , A. P. Furmanski , D. Garcia-Gamez , S. Gardiner , V. Genty , D. Goeldi , S. Gollapinni , O. Goodwin , E. Gramellini , P. Green , H. Greenlee , R. Grosso , L. Gu , W. Gu , R. Guenette , P. Guzowski , P. Hamilton , O. Hen , C. Hill , G. A. Horton-Smith , A. Hourlier , E. C. Huang , R. Itay , C. James , J. Jan de Vries , X. Ji , L. Jiang , J. H. Jo , R. A. Johnson , J. Joshi , Y. J. Jwa , G. Karagiorgi , W. Ketchum , B. Kirby , M. Kirby , T. Kobilarcik , I. Kreslo , I. Lepetic , Y. Li , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , M. Luethi , B. Lundberg , X. Luo , A. Marchionni , S. Marcocci , C. Mariani , J. Marshall , J. Martin-Albo , D. A. Martinez Caicedo , K. Mason , A. Mastbaum , N. McConkey , V. Meddage , T. Mettler , K. Miller , J. Mills , K. Mistry , T. Mohayai , A. Mogan , J. Moon , M. Mooney , C. D. Moore , J. Mousseau , M. Murphy , R. Murrells , D. Naples , R. K. Neely , P. Nienaber , J. Nowak , O. Palamara , V. Pandey , V. Paolone , A. Papadopoulou , V. Papavassiliou , S. F. Pate , A. Paudel , Z. Pavlovic , E. Piasetzky , D. Porzio , S. Prince , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , L. Ren , L. Rochester , H. E. Rogers , M. Ross-Lonergan , C. Rudolf von Rohr , B. Russell , G. Scanavini , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Sinclair , A. Smith , E. L. Snider , M. Soderberg , S. Soldner-Rembold , S. R. Soleti , P. Spentzouris , J. Spitz , M. Stancari , J. St. John , T. Strauss , K. Sutton , S. Sword-Fehlberg , A. M. Szelc , N. Tagg , W. Tang , K. Terao , R. T. Thornton , M. Toups , Y. -T. Tsai , S. Tufanli , M. A. Uchida , T. Usher , W. Van De Pontseele , R. G. Van de Water , B. Viren , M. Weber , H. Wei , D. A. Wickremasinghe , Z. Williams , S. Wolbers , T. Wongjirad , K. Woodruff , M. Wospakrik , W. Wu , T. Yang , G. Yarbrough , L. E. Yates , G. P. Zeller , J. Zennamo , C. Zhang

We analyse the performance of a gas time projection chamber (TPC) as a high-performance gamma-ray telescope and polarimeter in the e$^+$e$^-$ pair creation regime. We use data collected at a gamma-ray beam of known polarisation. The TPC…

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 LArIAT liquid argon time projection chamber, placed in a tertiary beam of charged particles at the Fermilab Test Beam Facility, has collected large samples of pions, muons, electrons, protons, and kaons in the momentum range 300-1400…

Instrumentation and Detectors · Physics 2020-06-17 LArIAT Collaboration , R. Acciarri , C. J. Adams , J. Asaadi , M. Backfish , W. Badgett , B. Baller , O. Benevides Rodrigues , F. d. M. Blaszczyk , R. Bouabid , C. Bromberg , R. Carey , R. Castillo Fernandez , F. Cavanna , J. I. Cevallos Aleman , A. Chatterjee , P. Dedin Neto , M. V. Dos Santos , S. Dytman , D. Edmunds , M. Elkins , C. O. Escobar , J. Esquivel , J. Evans , A. Falcone , A. Farbin , W. Flanagan , B. Fleming , W. Foreman , D. Garcia-Gamez , D. Gastler , T. Ghosh , R. A. Gomes , E. Gramellini , R. Gran , P. Guzowski , A. Habig , A. Hahn , P. Hamilton , C. Hill , J. Ho , A. Holin , J. Hugon , E. Iwai , D. Jensen , R. A. Johnson , H. Jostlein , H. Kawai , E. Kearns , E. Kemp , M. Kirby , T. Kobilarcik , M. Kordosky , P. Kryczynski , K. Lang , R. Linehan , S. Lockwitz , X. Luo , A. A. B. Machado , A. Marchionni , T. Maruyama , L. Mendes Santos , W. Metcalf , C. A. Moura , R. Nichol , I. Nutini , A. Olivier , O. Palamara , J. Paley , I. Parmaksiz , B. Passarelli Gelli , L. Paulucci , D. Phan , G. Pulliam , J. L. Raaf , B. Rebel , M. Reggiani Guzzo , M. Ross-Lonergan , D. Schmitz , D. Sessumes , S. Shahsavarani , D. Shooltz , E. Segreto , D. Smith , M. Soares Nunes , M. Soderberg , B. Soubasis , F. Spagliardi , J. M. St. John , M. Stancari , D. Stefan , M. Stephens , R. Sulej , A. Szelc , M. Tabata , D. Totani , M. Tzanov , G. Valdiviesso , D. Walker , H. Wenzel , Z. Williams , T. Yang , J. Yu , G. Zeller , S. Zhang , J. Zhu

We have operated a liquid-argon large-electron-multiplier time-projection chamber (LAr LEM-TPC) with a large active area of 76 $\times$ 40 cm$^2$ and a drift length of 60 cm. This setup represents the largest chamber ever achieved with this…

We have exposed a dual-phase Liquid Argon Time Projection Chamber (LAr-TPC) to a low energy pulsed narrowband neutron beam, produced at the Notre Dame Institute for Structure and Nuclear Astrophysics to study the scintillation light yield…

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…

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

Liquid Argon Time Projection Chambers (LArTPCs) have been selected for the future long-baseline Deep Underground Neutrino Experiment (DUNE). To allow LArTPCs to operate in the high-multiplicity near detector environment of DUNE, a new…

Instrumentation and Detectors · Physics 2018-01-30 J. Asaadi , M. Auger , A. Ereditato , D. Goeldi , R. Haenni , U. Kose , I Kreslo , D. Lorca , M. Luethi , C. Rudolf Von Rohr , J. R. Sinclair , F. Stocker , C. Tognina , M. Weber

A number of liquid argon time projection chambers (LAr TPC's) are being build or are proposed for neutrino experiments on long- and short baseline beams. For these detectors a distortion in the drift field due to geometrical or physics…

Instrumentation and Detectors · Physics 2015-01-13 A. Ereditato , I. Kreslo , M. Lüthi , C. Rudolf von Rohr , M. Schenk , T. Strauss , M. Weber , M. Zeller

We propose a relatively simple method to measure the event time in liquid Argon (LAr) TPC-based neutrino detectors that takes advantage of the topological reconstruction of each event from the TPC data prior to performing a one-parameter…

Instrumentation and Detectors · Physics 2020-04-02 Evan Angelico , Andrey Elagin , Henry J. Frisch , Matthew Wetstein