English
Related papers

Related papers: Modeling impurity concentrations in liquid argon d…

200 papers

We report an ab-initio comparative study of the electric-field-gradient tensor (EFG) and structural relaxations introduced by acceptor (Cd) and donor (Ta) impurities when they replace cations in a series of binary oxides: TiO2, SnO2, and…

Materials Science · Physics 2008-04-24 L. A. Errico , G. Fabricius , M. Renteria

Precision measurements of solar neutrinos emitted by specific nuclear reaction chains in the Sun are of great interest for developing an improved understanding of star formation and evolution. Given the expected neutrino fluxes and known…

Ionization electron diffusion in Liquid Argon Time Projection Chambers (LArTPCs) has typically been considered at the detector design stage, but little attention has been given to its effects on calibration and particle identification. We…

Instrumentation and Detectors · Physics 2022-05-26 A. Lister , M. Stancari

The MicroBooNE liquid argon time projection chamber (LArTPC) maintains a high level of liquid argon purity through the use of a filtration system that removes electronegative contaminants in continuously-circulated liquid, recondensed boil…

Instrumentation and Detectors · Physics 2022-11-17 MicroBooNE collaboration , P. Abratenko , J. Anthony , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , C. Barnes , G. Barr , J. Barrow , V. Basque , L. Bathe-Peters , O. Benevides Rodrigues , S. Berkman , A. Bhanderi , A. Bhat , M. Bhattacharya , M. Bishai , A. Blake , T. Bolton , J. Y. Book , L. Camilleri , D. Caratelli , I. Caro Terrazas , F. Cavanna , G. Cerati , Y. Chen , D. Cianci , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , M. Del Tutto , S. R. Dennis , P. Detje , A. Devitt , R. Diurba , R. Dorrill , K. Duffy , S. Dytman , B. Eberly , A. Ereditato , J. J. Evans , R. Fine , G. A. Fiorentini Aguirre , R. S. Fitzpatrick , B. T. Fleming , N. Foppiani , D. Franco , A. P. Furmanski , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , O. Goodwin , E. Gramellini , P. Green , H. Greenlee , W. Gu , R. Guenette , P. Guzowski , L. Hagaman , O. Hen , C. Hilgenberg , G. A. Horton-Smith , A. Hourlier , R. Itay , C. James , X. Ji , L. Jiang , J. H. Jo , C. Joe , R. A. Johnson , Y. J. Jwa , D. Kalra , N. Kamp , N. Kaneshige , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , I. Kreslo , I. Lepetic , J. -Y. Li , K. Li , Y. Li , K. Lin , B. R. Littlejohn , W. C. Louis , X. Luo , K. Manivannan , C. Mariani , D. Marsden , J. Marshall , D. A. Martinez Caicedo , K. Mason , A. Mastbaum , N. McConkey , V. Meddage , T. Mettler , K. Miller , J. Mills , K. Mistry , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , J. Mousseau , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , R. K. Neely , D. A. Newmark , J. Nowak , M. Nunes , O. Palamara , V. Paolone , A. Papadopoulou , V. Papavassiliou , H. B. Parkinson , S. F. Pate , N. Patel , A. Paudel , Z. Pavlovic , E. Piasetzky , I. Ponce-Pinto , S. Prince , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , L. Ren , L. C. J. Rice , L. Rochester , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , C. Rudolph von Rohr , G. Scanavini , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , J. Sinclair , A. Smith , E. L. Snider , M. Soderberg , S. Soldner-Rembold , P. Spentzouris , J. Spitz , M. Stancari , J. St. John , T. Strauss , K. Sutton , S. Sword-Fehlberg , A. M. Szelc , W. Tang , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , Y. -T. Tsai , M. A. Uchida , T. Usher , B. Viren , M. Weber , H. Wei , A. J. White , Z. Williams , S. Wolbers , T. Wongjirad , M. Wospakrik , K. Wresilo , N. Wright , W. Wu , E. Yandel , T. Yang , G. Yarbrough , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang , M. Zuckerbrot

The Liquid Argon Time Projection Chamber offers an innovative technology for a new class of massive detectors for rare-event detection. It is a precise tracking device that allows three-dimensional spatial reconstruction with mm-scale…

Instrumentation and Detectors · Physics 2015-06-15 A. Rubbia

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 proliferation of liquid argon time projection chamber detectors makes the characterization of the dielectric properties of liquid argon a critical task. To improve understanding of these properties, a systematic study of the breakdown…

Instrumentation and Detectors · Physics 2015-03-27 R. Acciarri , B. Carls , C. James , B. Johnson , H. Jostlein , S. Lockwitz , B. Lundberg , J. L. Raaf , R. Rameika , B. Rebel , G. P. Zeller , M. Zuckerbrot

The paper is considering an opportunity for the CERN/GranSasso (CNGS) neutrino complex, concurrent time-wise with T2K and NOvA, to search for theta_13 oscillations and CP violation. Compared with large water Cherenkov (T2K) and fine grained…

Gaseous Optical Time Projection Chambers (OTPCs) aimed at Neutrino Physics and Rare Event Searches will likely exceed the tonne scale during the next decade. This will make their performance sensitive to gas contamination levels as low as…

Instrumentation and Detectors · Physics 2025-04-01 D. J. Fernández-Posada , D. González-Díaz , J. Baldonedo , J. Collazo , E. Casarejos , P. Hamacher-Baumann , P. Amedo , J. Llerena

In this paper we describe the design, construction, and operation of a first large area double-phase liquid argon Large Electron Multiplier Time Projection Chamber (LAr LEM-TPC). The detector has a maximum drift length of 60 cm and the…

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…

The hydrodynamic state of an impurity immersed in a low density granular gas is analyzed. Explicit expressions for the temperature and density fields of the impurity in terms of the hydrodynamic fields of the gas are derived. It is shown…

Statistical Mechanics · Physics 2009-11-11 J. Javier Brey , M. J. Ruiz-Montero , F. Moreno

Thanks to the simplicity and robustness of its calculation methods, algorithmic (or Kolmogorov) complexity appears as a useful tool to reveal chaotic dynamics when experimental time series are too short and noisy to apply Takens'…

The appropriate generalization of the isotropic impurity Anderson model for valence fluctuations between two magnetic multiplets $l^n$ and $l^{n+1}$ is solved in the strong-coupling limit of Wilson's renormalization group for $l\leq$ 3.…

Condensed Matter · Physics 2007-05-23 A. A. Aligia , M. Balina

The transport of excess electrons in liquid argon driven out of equilibrium by an applied electric field is revisited using a multi-term solution of Boltzmann's equation together with ab initio liquid phase cross-sections calculated using…

Chemical Physics · Physics 2015-05-04 G. J. Boyle , R. P. McEachran , D. G. Cocks , R. D. White

We theoretically investigate the correlated decoherence dynamics of two mobile impurities trapped within a gas of ultracold fermionic atoms. We use a mean-field approximation to self-consistently describe the effect of impurity-gas…

Quantum Gases · Physics 2026-01-06 Sindre Brattegard , Thomás Fogarty , Thomas Busch , Mark T. Mitchison

This paper describes the cryogenic and purification systems of the ICARUS T600 detector in its present implementation at the Fermi National Laboratory, Illinois, USA. The ICARUS T600 detector is made of four large Time Projection Chambers,…

High Energy Physics - Experiment · Physics 2026-04-13 F. Abd Alrahman , P. Abratenko , N. Abrego-Martinez , A. Aduszkiewicz , F. Akbar , L. Aliaga Soplin , M. Artero Pons , J. Asaadi , W. F. Badgett , B. Behera , V. Bellini , R. Benocci , J. Berger , S. Berkman , O. Beltramello , S. Bertolucci , M. Betancourt , A. Blanchet , F. Boffelli , M. Bonesini , T. Boone , B. Bottino , A. Braggiotti , J. Bremer , S. J. Brice , V. Brio , C. Brizzolari , H. S. Budd , A. Campani , A. Campos , D. Carber , M. Carneiro , I. Caro Terrazas , H. Carranza , F. Castillo Fernandez , A. Castro , S. Centro , G. Cerati , M. Chalifour , P. Chambouvet , A. Chatterjee , D. Cherdack , S. Cherubini , N. Chithirasreemadam , T. E. Coan , A. Cocco , M. R. Convery , L. Cooper-Troendle , S. Copello , H. Da Motta , M. Dallolio , A. A. Dange , A. de Roeck , S. Di Domizio , L. Di Noto , D. Di Ferdinando , M. Diwan , S. Dolan , L. Domine , S. Donati , R. Doubnik , F. Drielsma , J. Dyer , S. Dytman , C. Fabre , A. Falcone , C. Farnese , A. Fava , N. Gallice , F. G. Garcia , C. Gatto , M. Geynisman , D. Gibin , A. Gioiosa , W. Gu , A. Guglielmi , G. Gurung , K. Hassinin , H. Hausner , A. Heggestuen , B. Howard , R. Howell , Z. Hulcher , I. Ingratta , C. James , W. Jang , Y. -J. Jwa , L. Kashur , W. Ketchum , J. S. Kim , D. -H. Koh , J. Larkin , Y. Li , C. Mariani , C. M. Marshall , S. Martynenko , N. Mauri , K. S. McFarland , D. P. Méndez , A. Menegolli , G. Meng , O. G. Miranda , D. Mladenov , A. Mogan , N. Moggi , E. Montagna , C. Montanari , A. Montanari , M. Mooney , G. Moreno-Granados , J. Mueller , M. Murphy , D. Naples , M. Nessi , T. Nichols , S. Palestini , M. Pallavicini , V. Paolone , L. Pasqualini , L. Patrizii , L. Paudel , G. Petrillo , C. Petta , V. Pia , F. Pietropaolo , F. Poppi , M. Pozzato , M. L Pumo , G. Putnam , X. Qian , A. Rappoldi , G. L. Raselli , S. Repetto , F. Resnati , A. M. Ricci , E. Richards , M. Rosenberg , M. Rossella , N. Rowe , P. Roy , C. Rubbia , M. Saad , S. Saha , G. Salmoria , S. Samanta , M. Satgia , A. Scaramelli , D. Schmit , F. Schwartz , A. Schukraft , D. Senadheera , S-H. Seo , F. Sergiampietri , G. Sirri , J. S. Smedley , J. Smith , L. Stanco , J. Stewart , H. A. Tanaka , F. Tapia , M. Tenti , K. Terao , F. Terranova , V. Togo , D. Torretta , M. Torti , F. Tortorici , R. Triozzi , Y. -T. Tsai , K. V. Tsang , S. Tufanli , T. Usher , F. Varanini , N. Vardy , S. Ventura , M. Vicenzi , C. Vignoli , B. Viren , F. A. Wieler , Z. Williams , R. J. Wilson , P. Wilson , J. Wolfs , T. Wongjirad , A. Wood , E. Worcester , M. Worcester , M. Wospakrik , S. Yadav , H. Yu , J. Yu , A. Zani , J. Zennamo , J. Zettlemoyer , C. Zhang , S. Zucchelli , M. Zuckerbrot

Coherent scattering is a flavor-blind, high-rate, as yet undetected neutrino interaction predicted by the Standard Model. We propose to use a compact (kg-scale), two-phase (liquid-gas) argon ionization detector to measure coherent neutrino…

Nuclear Experiment · Physics 2009-11-10 Chris Hagmann , Adam Bernstein

New light particles may be produced in large numbers in the far-forward region at the LHC and then decay to dark matter, which can be detected through its scattering in far-forward experiments. We consider the example of invisibly-decaying…

High Energy Physics - Phenomenology · Physics 2021-04-28 Brian Batell , Jonathan L. Feng , Sebastian Trojanowski

The performance of a two-phase Ar avalanche detector in a single electron counting mode was studied, with regard to potential application in coherent neutrino-nucleus scattering and dark matter search experiments. The detector comprised of…

‹ Prev 1 4 5 6 7 8 10 Next ›