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A novel liquid argon (LAr) purity monitor was developed with a sensitivity to electronegative impurities of the order of ppb (O$_2$ equivalent). Such a high purity is e.g. needed in a LAr drift chamber. The principle is to measure the…

Instrumentation and Detectors · Physics 2007-05-23 A. Badertscher , M. Laffranchi , A. Rubbia

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 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 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

A search for pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark, is presented. This is the first leptoquark search using ATLAS data to investigate top-philic cross-generational couplings…

High Energy Physics - Experiment · Physics 2021-04-27 ATLAS Collaboration

The Deep Underground Neutrino Experiment (DUNE) is a project to design, construct and operate a next-generation long-baseline neutrino detector with a liquid argon (LAr) target capable also of searching for proton decay and supernova…

Instrumentation and Detectors · Physics 2016-06-22 Vitaly A. Kudryavtsev

We explore the potential offered by large-mass Liquid Argon detectors for determination of the sign of Delta m_{31}^2, or the neutrino mass hierarchy, through interactions of atmospheric neutrinos. We give results for a 100 kT sized…

High Energy Physics - Phenomenology · Physics 2008-11-26 Raj Gandhi , Pomita Ghoshal , Srubabati Goswami , S Uma Sankar

In recent years cooling technology for Liquid Xenon (LXe) detectors has advanced driven by the development of Dark Matter (DM) detectors with target mass in the 100 - 1,000 kg range. The next generation of DM detectors based on LXe will be…

Instrumentation and Detectors · Physics 2019-09-24 K. L. Giboni , P. Juyal , E. Aprile , Y. Zhang , J. Naganoma

We propose to implement a two-stage detection strategy for exotic long-lived particles that could be produced at the CERN LHC, become trapped in detector material, and decay later. The proposed strategy relies on an array of metal rods,…

High Energy Physics - Phenomenology · Physics 2022-03-18 Jan Kieseler , Juliette Alimena , Jasmine Simms , Thea Aarrestad , Maurizio Pierini , Alexander Kish

A small liquid argon Time Projection Chamber (LAr TPC) was operated for the first time in a magnetic field of 0.55 Tesla. The imaging properties of the detector were not affected by the magnetic field. In a test run with cosmic rays a…

Instrumentation and Detectors · Physics 2008-11-26 A. Badertscher , M. Laffranchi , A. Meregaglia , A. Mueller , A. Rubbia

The Daya Bay and RENO experiments have recently observed a non-zero $\theta_{13}$ at more than $5\sigma$ CL. This has important consequences for future neutrino oscillation experiments. We analyze these within the LAGUNA design study which…

High Energy Physics - Phenomenology · Physics 2012-06-19 Pilar Coloma , Tracey Li , Silvia Pascoli

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

The ATLAS detector at CERN will provide a high-resolution longitudinally-segmented calorimeter and precision tracking for the upcoming study of heavy ion collisions at the LHC (sqrt(s_NN)=5520 GeV). The calorimeter covers |eta|<5 with both…

Nuclear Experiment · Physics 2019-08-13 P. Steinberg

The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be…

High Energy Physics - Experiment · Physics 2007-05-23 Felicitas Pauss , Michael Dittmar

$^{83m}Kr$ and $^{22}Na$ have been used in calibrating a liquid argon (LAr) detector.$^{83m}Kr$ atoms are produced through the decay of $^{83}Rb$ and introduced into the LAr detector through the circulating purification system. The light…

Instrumentation and Detectors · Physics 2019-09-06 Weixing Xiong , Mengyun Guan , Changgen Yang , Peng Zhang , Jinchang Liu , Cong Guo , Yuting wei , Youyu Gan , Qin Zhao , Jiajun Li

The possible detection of massive quasi-stable exotic particles at the high luminosity hadronic colliders is discussed. In the coming ten years the LHC, now under preparation, has the best opportunity to observe them at the TeV scale. The…

High Energy Physics - Phenomenology · Physics 2009-10-30 Aleandro Nisati , Silvano Petrarca , Giorgio Salvini

Future liquid-argon DarkSide-20k and ARGO detectors, designed for direct dark matter search, will be sensitive also to core-collapse supernova neutrinos, via coherent elastic neutrino-nucleus scattering. This interaction channel is…

High Energy Astrophysical Phenomena · Physics 2024-07-18 P. Agnes , S. Albergo , I. F. M. Albuquerque , T. Alexander , A. Alici , A. K. Alton , P. Amaudruz , S. Arcelli , M. Ave , I. Ch. Avetissov , R. I. Avetisov , O. Azzolini , H. O. Back , Z. Balmforth , V. Barbarian , A. Barrado Olmedo , P. Barrillon , A. Basco , G. Batignani , A. Bondar , W. M. Bonivento , E. Borisova , B. Bottino , M. G. Boulay , G. Buccino , S. Bussino , J. Busto , A. Buzulutskov , M. Cadeddu , M. Cadoni , A. Caminata , N. Canci , G. Cappello , M. Caravati , M. Cárdenas-Montes , M. Carlini , F. Carnesecchi , P. Castello , S. Catalanotti , V. Cataudella , P. Cavalcante , S. Cavuoti , S. Cebrian , J. M. Cela Ruiz , B. Celano , S. Chashin , A. Chepurnov , E Chyhyrynets , C. Cicalò , L. Cifarelli , D. Cintas , F. Coccetti , V. Cocco , M. Colocci , E. Conde Vilda , L. Consiglio , S. Copello , J. Corning , G. Covone , P. Czudak , S. D'Auria , M. D. Da Rocha Rolo , O. Dadoun , M. Daniel , S. Davini , A. De Candia , S. De Cecco , A. De Falco , G. De Filippis , D. De Gruttola , G. De Guido , G. De Rosa , M. Della Valle , G. Dellacasa , S. De Pasquale , A. V. Derbin , A. Devoto , L. Di Noto , C. Dionisi , P. Di Stefano , G. Dolganov , F. Dordei , L. Doria , M. Downing , T. Erjavec , M. Fernandez Diaz , G. Fiorillo , A. Franceschi , D. Franco , E. Frolov , N. Funicello , F. Gabriele , C. Galbiati , M. Garbini , P. Garcia Abia , A. Gendotti , C. Ghiano , R. A. Giampaolo , C. Giganti , M. A. Giorgi , G. K. Giovanetti , V. Goicoechea Casanueva , A. Gola , R. Graciani Diaz , G. Y. Grigoriev , A. Grobov , M. Gromov , M. Guan , M. Guerzoni , M. Gulino , C. Guo , B. R. Hackett , A. Hallin , M. Haranczyk , S. Hill , S. Horikawa , F. Hubaut , T. Hugues , E. V. Hungerford , An. Ianni , V. Ippolito , C. C. James , C. Jillings , P. Kachru , A. A. Kemp , C. L. Kendziora , G. Keppel , A. V. Khomyakov , S. Kim , A. Kish , I. Kochanek , K. Kondo , G. Korga , A. Kubankin , R. Kugathasan , M. Kuss , M. Kuźniak , M. La Commara , M. Lai , S. Langrock , M. Leyton , X. Li , L. Lidey , M. Lissia , G. Longo , I. N. Machulin , L. Mapelli , A. Marasciulli , A. Margotti , S. M. Mari , J. Maricic , M. Martínez , A. D. Martinez Rojas , C. J. Martoff , A. Masoni , A. Mazzi , A. B. McDonald , J. Mclaughlin , A. Messina , P. D. Meyers , T. Miletic , R. Milincic , A. Moggi , A. Moharana , S. Moioli , J. Monroe , S. Morisi , M. Morrocchi , E. N. Mozhevitina , T. Mróz , V. N. Muratova , C. Muscas , L. Musenich , P. Musico , R. Nania , T. Napolitano , A. Navrer Agasson , M. Nessi , I. Nikulin , J. Nowak , A. Oleinik , V. Oleynikov , L. Pagani , M. Pallavicini , L. Pandola , E. Pantic , E. Paoloni , G. Paternoster , P. A. Pegoraro , K. Pelczar , L. A. Pellegrini , C. Pellegrino , F. Perotti , V. Pesudo , E. Picciau , F. Pietropaolo , C. Pira , A. Pocar , D. M. Poehlmann , S. Pordes , S. S. Poudel , P. Pralavorio , D. Price , F. Raffaelli , F. Ragusa , A. Ramirez , M. Razeti , A. Razeto , A. L. Renshaw , S. Rescia , M. Rescigno , F. Resnati , F. Retiere , L. P. Rignanese , C. Ripoli , A. Rivetti , J. Rode , L. Romero , M. Rossi , A. Rubbia , P. Salatino , O. Samoylov , E. Sánchez García , E. Sandford , S. Sanfilippo , D. Santone , R. Santorelli , C. Savarese , E. Scapparone , B. Schlitzer , G. Scioli , D. A. Semenov , B. Shaw , A. Shchagin , A. Sheshukov , M. Simeone , P. Skensved , M. D. Skorokhvatov , O. Smirnov , B. Smith , A. Sokolov , A. Steri , S. Stracka , V. Strickland , M. Stringer , S. Sulis , Y. Suvorov , A. M. Szelc , R. Tartaglia , G. Testera , T. N. Thorpe , A. Tonazzo , S. Torres-Lara , A. Tricomi , E. V. Unzhakov , G. Usai , T. Vallivilayil John , T. Viant , S. Viel , A. Vishneva , R. B. Vogelaar , M. Wada , H. Wang , Y. Wang , S. Westerdale , R. J. Wheadon , L. Williams , Ma. M. Wojcik , Ma. Wojcik , X. Xiao , C. Yang , Z. Ye , A. Zani , A. Zichichi , G. Zuzel , M. P. Zykova

The Cryogenic Apparatus for Precision Tests of Argon Interactions with Neutrino (CAP- TAIN) program is designed to make measurements of scientific importance to long-baseline neutrino physics and physics topics that will be explored by…

In view of the evaluation of the physics goals of a large Liquid Argon TPC, evolving from the ICARUS technology, we have studied the possibility of performing precision measurements on atmospheric neutrinos. For this purpose we have…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Battistoni , A. Ferrari , C. Rubbia , P. R. Sala , F. Vissani

Several experimental techniques are currently under development, to measure the expected tiny fluxes of highest energy neutrinos above 10**18 eV. Projects in different stages of realisation are discussed here, which are based on optical and…

Astrophysics · Physics 2009-11-10 Rolf Nahnhauer
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