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A particle detection system that exploits the scintillation light produced by ionizing particles in liquid argon (LAr) has been assembled at CERN. The system is based on 10 large-area photomultiplier tubes (PMT) immersed in a 1500-liter…

The Large Hadron Collider (LHC) at CERN is expected to be upgraded to the High-Luminosity LHC (HL-LHC) by 2029 and achieve instantaneous luminosity around 5 - 7.5 $\times$ 10$^{34}$cm$^{-2}$ s$^{-1}$. This represents a more than 3-4 fold…

This paper reports the first results of a direct dark matter search with the DEAP-3600 single-phase liquid argon (LAr) detector. The experiment was performed 2 km underground at SNOLAB (Sudbury, Canada) utilizing a large target mass, with…

A method for calibration of cryogenic liquid argon detector response to recoils with certain energy -8.2 keV - is proposed. The method utilizes a process of inelastic scattering of monoenergetic neutrons produced by fusion DD neutron…

Instrumentation and Detectors · Physics 2014-07-11 Sergey Polosatkin , Evgeny Grishnyaev , Alexander Dolgov

The prevalent use of large volume liquid argon detectors strongly motivates the development of novel readout and monitoring technology which functions at cryogenic temperatures. This paper presents the development of a cryogenic CMOS camera…

Instrumentation and Detectors · Physics 2017-04-05 Nicola McConkey , Neil Spooner , Matthew Thiesse , Michael Wallbank , Thomas Karl Warburton

We describe the design of a 20-liter test stand constructed to study fundamental properties of liquid argon (LAr). This system utilizes a simple, cost-effective gas argon (GAr) purification to achieve high purity, which is necessary to…

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.

Large liquid argon detectors offer one of the best avenues for the detection of galactic weakly interacting massive particles (WIMPs) via their scattering on atomic nuclei. The liquid argon target allows exquisite discrimination between…

Instrumentation and Methods for Astrophysics · Physics 2020-04-22 The DarkSide Collaboration , C. E. Aalseth , S. Abdelhakim , F. Acerbi , P. Agnes , R. Ajaj , I. F. M. Albuquerque , T. Alexander , A. Alici , A. K. Alton , P. Amaudruz , F. Ameli , J. Anstey , P. Antonioli , M. Arba , S. Arcelli , R. Ardito , I. J. Arnquist , P. Arpaia , D. M. Asner , A. Asunskis , M. Ave , H. O. Back , A. Barrado Olmedo , G. Batignani , M. G. Bisogni , V. Bocci , A. Bondar , G. Bonfini , W. Bonivento , E. Borisova , B. Bottino , M. G. Boulay , R. Bunker , S. Bussino , A. Buzulutskov , M. Cadeddu , M. Cadoni , A. Caminata , N. Canci , A. Candela , C. Cantini , M. Caravati , M. Cariello , F. Carnesecchi , M. Carpinelli , A. Castellani , P. Castello , S. Catalanotti , V. Cataudella , P. Cavalcante , D. Cavazza , S. Cavuoti , S. Cebrian , J. M. Cela Ruiz , B. Celano , R. Cereseto , W. Cheng , A. Chepurnov , C. Cicalò , L. Cifarelli , M. Citterio , A. G. Cocco , V. Cocco , M. Colocci , L. Consiglio , F. Cossio , G. Covone , P. Crivelli , I. D'Antone , M. D'Incecco , D. D'Urso , M. D. Da Rocha Rolo , O. Dadoun , M. Daniel , S. Davini , A. De Candia , S. De Cecco , M. De Deo , A. De Falco , G. De Filippis , D. De Gruttola , G. De Guido , G. De Rosa , G. Dellacasa , P. Demontis , S. DePaquale , A. V. Derbin , A. Devoto , F. Di Eusanio , L. Di Noto , G. Di Pietro , P. Di Stefano , C. Dionisi , G. Dolganov , F. Dordei , M. Downing , F. Edalatfar , A. Empl , M. Fernandez Diaz , A. Ferri , C. Filip , G. Fiorillo , K. Fomenko , A. Franceschi , D. Franco , G. E. Froudakis , F. Gabriele , A. Gabrieli , C. Galbiati , P. Garcia Abia , D. Gascón Fora , A. Gendotti , C. Ghiano , A. Ghisi , S. Giagu , P. Giampa , R. A. Giampaolo , C. Giganti , M. A. Giorgi , G. K. Giovanetti , M. L. Gligan , A. Gola , O. Gorchakov , M. Grab , R. Graciani Diaz , F. Granato , M. Grassi , J. W. Grate , G. Y. Grigoriev , A. Grobov , M. Gromov , M. Guan , M. B. B. Guerra , M. Guerzoni , M. Gulino , R. K. Haaland , B. R. Hackett , A. Hallin , B. Harrop , E. W. Hoppe , S. Horikawa , B. Hosseini , F. Hubaut , P. Humble , E. V. Hungerford , An. Ianni , A. Ilyasov , V. Ippolito , C. Jillings , K. Keeter , C. L. Kendziora , S. Kim , I. Kochanek , K. Kondo , G. Kopp , D. Korablev , G. Korga , A. Kubankin , R. Kugathasan , M. Kuss , M. Kuźniak , M. La Commara , L. La Delfa , M. Lai , S. Langrock , M. Lebois , B. Lehnert , N. Levashko , X. Li , Q. Liqiang , M. Lissia , G. U. Lodi , G. Longo , R. López Manzano , R. Lussana , L. Luzzi , A. A. Machado , I. N. Machulin , A. Mandarano , L. Mapelli , M. Marcante , A. Margotti , S. M. Mari , M. Mariani , J. Maricic , M. Marinelli , D. Marras , M. Martínez , J. J. Martínez Morales , A. D. Martinez Rojas , C. J. Martoff , M. Mascia , J. Mason , A. Masoni , A. Mazzi , A. B. McDonald , A. Messina , P. D. Meyers , T. Miletic , R. Milincic , A. Moggi , S. Moioli , J. Monroe , M. Morrocchi , T. Mroz , W. Mu , V. N. Muratova , S. Murphy , C. Muscas , P. Musico , R. Nania , T. Napolitano , A. Navrer Agasson , M. Nessi , I. Nikulin , A. Oleinik , V. Oleynikov , M. Orsini , F. Ortica , L. Pagani , M. Pallavicini , S. Palmas , L. Pandola , E. Pantic , E. Paoloni , G. Paternoster , V. Pavletcov , F. Pazzona , S. Peeters , P. A. Pegoraro , K. Pelczar , L. A. Pellegrini , C. Pellegrino , N. Pelliccia , F. Perotti , V. Pesudo , E. Picciau , C. Piemonte , F. Pietropaolo , A. Pocar , T. Pollman , D. Portaluppi , S. S. Poudel , P. Pralavorio , D. Price , B. Radics , F. Raffaelli , F. Ragusa , M. Razeti , A. Razeto , V. Regazzoni , C. Regenfus , A. L. Renshaw , S. Rescia , M. Rescigno , F. Retiere , L. P. Rignanese , A. Rivetti , A. Romani , L. Romero , N. Rossi , A. Rubbia , D. Sablone , P. Sala , P. Salatino , O. Samoylov , E. Sánchez García , S. Sanfilippo , M. Sant , D. Santone , R. Santorelli , C. Savarese , E. Scapparone , B. Schlitzer , G. Scioli , E. Segreto , A. Seifert , D. A. Semenov , A. Shchagin , A. Sheshukov , S. Siddhanta , M. Simeone , P. N. Singh , P. Skensved , M. D. Skorokhvatov , O. Smirnov , G. Sobrero , A. Sokolov , A. Sotnikov , R. Stainforth , A. Steri , S. Stracka , V. Strickland , G. B. Suffritti , S. Sulis , Y. Suvorov , A. M. Szelc , R. Tartaglia , G. Testera , T. Thorpe , A. Tonazzo , A. Tosi , M. Tuveri , E. V. Unzhakov , G. Usai , A. Vacca , E. Vázquez-Jáuregui , M. Verducci , T. Viant , S. Viel , F. Villa , A. Vishneva , R. B. Vogelaar , M. Wada , J. Wahl , J. J. Walding , H. Wang , Y. Wang , S. Westerdale , R. J. Wheadon , R. Williams , J. Wilson , Marcin Wojcik , Mariusz Wojcik , S. Wu , X. Xiao , C. Yang , Z. Ye , M. Zuffa , G. Zuzel

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

In June 2012, an Expression of Interest for a long-baseline experiment (LBNO) has been submitted to the CERN SPSC. LBNO considers three types of neutrino detector technologies: a double-phase liquid argon (LAr) TPC and a magnetised iron…

Instrumentation and Detectors · Physics 2014-09-17 L. Agostino , B. Andrieu , R. Asfandiyarov , D. Autiero , O. Bésida , F. Bay , R. Bayes , A. M. Blebea-Apostu , A. Blondel , M. Bogomilov , S. Bolognesi , S. Bordoni , A. Bravar , M. Buizza-Avanzini , F. Cadoux , D. Caiulo , M. Calin , M. Campanelli , C. Cantini , L. Chaussard , D. Chesneanu , N. Colino , P. Crivelli , I. De Bonis , Y. Déclais , J. Dawson , C. De La Taille , P. Del Amo Sanchez , A. Delbart , S. Di Luise , D. Duchesneau , F. Dulucq , J. Dumarchez , I. Efthymiopoulos , S. Emery , T. Enqvist , L. Epprecht , T. Esanu , D. Franco , D. Franco , M. Friend , V. Galymov , A. Gendotti , C. Giganti , I. Gil-Botella , M. C Gomoiu , P. Gorodetzky , A. Haesler , T. Hasegawa , S. Horikawa , M. Ieva , A. Jipa , Y. Karadzhov , I. Karpikov , A. Khotjantsev , A. Korzenev , D. Kryn , Y. Kudenko , P. Kuusiniemi , I. Lazanu , J. -M. Levy , K. Loo , T. Lux , J. Maalampi , R. M. Margineanu , J. Marteau , C. Martin , G. Martin-Chassard , E. Mazzucato , A. Mefodiev , O. Mineev , B. Mitrica , S. Murphy , T. Nakadaira , M. Nessi , K. Nikolics , L. Nita , E. Noah , P. Novella , G. A. Nuijten , T. Ovsiannikova , C. Palomares , T. Patzak , E. Pennacchio , L. Periale , H. Pessard , B. Popov , M. Ravonel , M. Rayner , C. Regenfus , C. Ristea , O. Ristea , A. Robert , A. Rubbia , K. Sakashita , F. Sanchez , R. Santorelli , E. Scantamburlo , F. Sergiampietri , D. Sgalaberna , M. Slupecki , F. J. P. Soler , D. L. Stanca , A. Tonazzo , W. H. Trzaska , R. Tsenov , G. Vankova-Kirilova , F. Vannucci , G. Vasseur , A. Verdugo , T. Viant , S. Wu , N. Yershov , L. Zambelli , M. Zito

Detectors based on liquid argon (LAr) often require surfaces that can shift vacuum ultraviolet (VUV) light and reflect the visible shifted light. For the LAr instrumentation of the LEGEND-200 neutrinoless double beta decay experiment,…

Instrumentation and Detectors · Physics 2022-05-17 G. R. Araujo , L. Baudis , N. McFadden , P. Krause , S. Schönert , V. H. S. Wu

The neutron time-of-flight (n_TOF) facility at the European Laboratory for Particle Physics (CERN) is a pulsed white-spectrum neutron spallation source producing neutrons for two experimental areas: the Experimental Area 1 (EAR1), located…

Capacitive devices are customarily used as probes to measure the level of noble liquids in detectors operated for neutrino studies and dark matter searches. In this work we describe the use of a high-temperature superconducting material as…

Instrumentation and Detectors · Physics 2009-02-20 A. Bueno , A. J. Melgarejo , J. L. Navarro , S. Navas , A. G. Ruiz

Liquid argon time projection chambers (LArTPCs) are widely used in particle detection for their tracking and calorimetric capabilities. The particle physics community actively builds and improves high-quality simulators for such detectors…

Instrumentation and Detectors · Physics 2023-09-12 Sean Gasiorowski , Yifan Chen , Youssef Nashed , Pierre Granger , Camelia Mironov , Daniel Ratner , Kazuhiro Terao , Ka Vang Tsang

This paper presents a preliminary study into the use of CCDs to image secondary scintillation light generated by THick Gas Electron Multipliers (THGEMs) in a two phase LAr TPC. A Sony ICX285AL CCD chip was mounted above a double THGEM in…

Instrumentation and Detectors · Physics 2015-06-18 K. Mavrokoridis , F. Ball , J. Carroll , M. Lazos , K. J. McCormick , N. A. Smith , C. Touramanis , J. Walker

We report a robust method of stabilizing a laser to the frequency of an atomic transition using a hollow cathode lamp. In contrast to the standard dichroic atomic vapor laser lock (DAVLL) method, which uses dichroism induced by a…

We have explored a concept for an advanced Normal-Conducting Radio-Frequency (NCRF) C-band linear accelerator (linac) structure to achieve a high gradient, high power e$^+$e$^-$ linear collider in the TeV class. This design study represents…

At the beginning of 2010, we presented at the J-PARC PAC an R$&$D program towards large (100 kton scale) liquid argon TPCs, suitable to investigate, in conjunction with the J-PARC neutrino beam, the possibility of CP violation in the…

This paper reports on laser-induced multiphoton ionization at 266 nm of liquid argon in a time projection chamber (LAr TPC) detector. The electron signal produced by the laser beam is a formidable tool for the calibration and monitoring of…

Instrumentation and Detectors · Physics 2010-12-21 I. Badhrees , A. Ereditato , I. Kreslo , M. Messina , U. Moser , B. Rossi , M. S. Weber , M. Zeller , C. Altucci , S. Amoruso , R. Bruzzese , R. Velotta

A device has been built and tested, in which a ceramic superconducting cathode and a copper anode cause electrical discharges in low pressure gases, at temperatures between 50 and 70 K. The electrodes are connected to a capacitors array…

General Physics · Physics 2007-05-23 Evgeny Podkletnov , Giovanni Modanese
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