English
Related papers

Related papers: A two-phase argon avalanche detector operated in a…

200 papers

Electron avalanching in liquid argon is being studied as a function of voltage, pressure, radiation intensity, and the concentrations of certain additives, especially xenon. The avalanches produced in an intense electric field at the tip of…

High Energy Physics - Experiment · Physics 2009-11-07 J. G. Kim , S. M. Dardin , K. H. Jackson , R. W. Kadel , J. A. Kadyk , V. Peskov , W. A. Wenzel

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

We present the results of our recent studies of a Thick Gaseous Electron Multiplier (THGEM)-based detector, operated in Ar, Xe and Ar:Xe (95:5) at various gas pressures. Avalanche-multiplication properties and energy resolution were…

Instrumentation and Detectors · Physics 2009-11-13 R. Alon , J. Miyamoto , M. Cortesi , A. Breskin , R. Chechik , I. Carne , J. M. Maia , J. M. F. dos Santos , M. Gai , D. McKinsey , V. Dangendorf

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

We constructed and operated a double phase (liquid-vapour) pure argon Large Electron Multiplier Time Projection Chamber (LAr LEM-TPC) with a sensitive area of 10x10 cm$^2$ and up to 30 cm of drift length. The LEM is a macroscopic hole…

Instrumentation and Detectors · Physics 2015-05-13 A. Badertscher , L. Knecht , M. Laffranchi , D. Lussi , A. Marchionni , G. Natterer , P. Otiougova , F. Resnati , A. Rubbia , T. Viant

The Picosecond Avalanche Detector is a multi-junction silicon pixel detector based on a $\mathrm{(NP)_{drift}(NP)_{gain}}$ structure, devised to enable charged-particle tracking with high spatial resolution and picosecond time-stamp…

We have developed a novel technique for the measurement of the avalanche fluctuation of gaseous detectors using a UV laser. The technique is simple and requires a short data-taking time of about ten minutes. Furthermore, it is applicable…

We demonstrate an integral gated mode single photon detector at telecom wavelengths. The charge number of an avalanche pulse rather than the peak current is monitored for single-photon detection. The transient spikes in conventional gated…

We describe a work of a multi-cathode counter of the developed design in a single electron counting mode with a cathode made of aluminum alloy. The results of the calibration of the counter are presented. The coefficient of gas…

Instrumentation and Detectors · Physics 2018-10-17 A. V. Kopylov , I. V. Orekhov , V. V. Petukhov

We describe a detector of alpha particles based on wire type counters (single-wire and multiwire) operating in ambient air at high gas gains (100-1000). The main advantages of these detectors are: low cost, robustness and ability to operate…

Instrumentation and Detectors · Physics 2010-06-08 G. Charpak , P. Benaben , P. Breuil , E. Nappi , P. Martinengo , V. Peskov

The operation of a Micropattern Gaseous Detector (MPGD) comprising a cascade of two non-standard Gas Electron Multipliers (GEM) made from a 100 micrometer kapton foil was evaluated in pure krypton and in krypton-CO2 mixtures. The final…

Instrumentation and Detectors · Physics 2018-01-12 R. C. Roque , H. Natal da Luz , L. F. N. D. Carramate , C. D. R. Azevedo , J. A. Mir , F. D. Amaro

Motivated by the need for fast timing detectors to withstand up to 2 MGy of ionizing dose at the High Luminosity Large Hadron Collider, prototype low gain avalanche detectors (LGADs) have been fabricated in single pad configuration, 2x2…

Instrumentation and Detectors · Physics 2021-12-20 Martin Hoeferkamp , Alissa Howard , Gregor Kramberger , Sally Seidel , Josef Sorenson , Adam Yanez

New Cryogenic Avalanche Detector (CRAD) with ultimate sensitivity, that will be able to detect one primary electron released in the cryogenic liquid, is under development in the Laboratory of Cosmology and Particle Physics of the…

Instrumentation and Detectors · Physics 2015-10-28 A. Bondar , A. Buzulutskov , A. Dolgov , V. Nosov , L. Shekhtman , A. Sokolov

Charge multiplication through avalanche processes is commonly employed in the detection of single photons or charged particles in high-energy physics and beyond. In this report, we provide a detailed discussion of the properties of…

Instrumentation and Detectors · Physics 2021-04-23 Philipp Windischhofer , Werner Riegler

We present the results of the operation of an array of avalanche photodiodes (APDs) for the readout of an electroluminescence detector. The detector contains 24 APDs with a pitch of 15 mm between them allowing energy and position…

Instrumentation and Detectors · Physics 2015-12-30 B. Bourguille , A. Garcia Soto , I. Gil-Botella , T. Lux , C. Palomares , F. Sanchez , R. Santorelli

We study the performance of single- and double- THick Gas Electron Multiplier (THGEM) detectors in pure Hydrogen and Deuterium at low pressures, in the range of 100-450 Torr. The effect of the pressure on the maximum achievable gain,…

Instrumentation and Detectors · Physics 2015-11-19 Marco Cortesi , John Yurkon , Wolfgang Mittig , Daniel Bazin , Saul Beceiro-Novo , Andreas Stolz

Cryogenic Avalanche Detectors (CRADs) are referred to as a new class of noble-gas detectors operated at cryogenic temperatures with electron avalanching performed directly in the detection medium, the latter being in gaseous, liquid or…

Instrumentation and Detectors · Physics 2015-03-31 A. Buzulutskov

Liquid argon is used as a target material in several current and planned experiments related to dark matter direct searching and neutrino detection. SiPM is becoming the standard for scintillator detectors because of its advantages over…

Instrumentation and Detectors · Physics 2023-01-03 L. Wang , Y. Lei , T. A. Wang , C. Guo , K. K. Zhao , X. H. Liang , S. B. Wang , Y. D. Chen

We describe a new micro-pattern gas detector structure comprising a multi-layer hole-type multiplier (M-THGEM) combined with two in-built electrode meshes: the Multi-Mesh THGEM-type multiplier (MM-THGEM). Suitable potential differences…

Instrumentation and Detectors · Physics 2018-08-01 Rui de Olivera , Marco Cortesi

A successful operation of a new optical readout system (THGEM + WLS + MGPDs (multichannel array of multipixel avalanche Geiger photodiodes) in a two-phase liquid xenon detector was demonstrated.