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Related papers: ArDM: a ton-scale LAr detector for direct Dark Mat…

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Neutrinos are one of the least known elementary particles. The detection of neutrinos is an extremely difficult task since they are affected only by weak sub-atomic force or gravity. Therefore large detectors are constructed to reveal…

Computer Vision and Pattern Recognition · Computer Science 2015-05-05 Piotr Płoński , Dorota Stefan , Robert Sulej , Krzysztof Zaremba

Future giant liquid argon (LAr) time projection chambers (TPCs) require a purity of better than 0.1 parts per billion (ppb) to allow the ionised electrons to drift without significant capture by any electronegative impurities. We present a…

Instrumentation and Detectors · Physics 2015-05-28 K. Mavrokoridis , R. G. Calland , J. Coleman , P. K. Lightfoot , N. McCauley , K. J. McCormick , C. Touramanis

The ARIADNE Experiment, utilising a 1-ton dual-phase Liquid Argon Time Projection Chamber (LArTPC), aims to develop and mature optical readout technology for large scale LAr detectors. This paper describes the characterisation, using cosmic…

Instrumentation and Detectors · Physics 2020-12-02 Adam Lowe , Krishanu Majumdar , Konstantinos Mavrokoridis , Barney Philippou , Adam Roberts , Christos Touramanis , Jared Vann

We study a three stage dark matter and neutrino observatory based on multi-ton two-phase liquid Xe and Ar detectors with sufficiently low backgrounds to be sensitive to WIMP dark matter interaction cross sections down to 10E-47 cm^2, and to…

Instrumentation and Methods for Astrophysics · Physics 2015-03-19 K. Arisaka , P. Beltrame , C. W. Lam , P. F. Smith , C. Ghag , D. B. Cline , K. Lung , Y. Meng , E. Pantic , P. R. Scovell , A. Teymourian , H. Wang

XENON is a project for direct dark matter search located in the INFN underground laboratory LNGS. The previous generation of XENON detector, XENON1T, achieved an exposure of 1 ton$\times$year, setting the most stringent limits on the…

High Energy Physics - Experiment · Physics 2023-10-18 S. E. M. Ahmed Maouloud

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

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…

Systematic uncertainties in accelerator oscillation neutrino experiments arise mostly from nuclear models describing neutrino-nucleus interactions. To mitigate these uncertainties, we can study neutrino-nuclei interactions with detectors…

Instrumentation and Detectors · Physics 2023-10-31 R. M Amarinei , F. Sánchez , E. Roe , S. Bordoni , L. Giannessi , T Lux , E. Radicioni

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

Dual phase time projection chamber using liquid xenon as target material is one of most successful detectors for dark matter direct search, and has improved the sensitivities of searching for weakly interacting massive particles by almost…

Instrumentation and Detectors · Physics 2021-09-01 Qing Lin

The Liquid Argon Time Projection Chambers (LArTPCs) are a choice for the next generation of large neutrino detectors due to their optimal performance in particle tracking and calorimetry. The detection of Argon scintillation light plays a…

Instrumentation and Detectors · Physics 2018-04-18 G. Cancelo , F. Cavanna , C. O. Escobar , E. Kemp , A. A. Machado , A. Para , E. Segreto , D. Totani , D. Warner

The Deep Underground Neutrino Experiment (DUNE) is a next generation long baseline (1300 km) neutrino oscillation experiment. The neutrino beam measurements will be performed by a near detector (ND) and far detector (FD). The far detector…

Instrumentation and Detectors · Physics 2023-03-01 H. V. Souza

Ultralight dark matter (ULDM), as a class of low mass (< 1 eV) dark matter (DM) candidates, is a compelling alternative to historically dominant models such as WIMPs and has recently gained significant attention in the scientific community.…

High Energy Physics - Phenomenology · Physics 2024-11-22 Jordan Gué

Dark Matter experiments are recently focusing their detection techniques in low-mass WIMPs, which requires the use of light elements and low energy threshold. In this context, we describe the TREX-DM experiment, a low background…

Instrumentation and Detectors · Physics 2015-09-08 F. J. Iguaz , J. G. Garza , F. Aznar , J. F. Castel , S. Cebrian , T. Dafni , J. A. Garcia , I. G. Irastorza , A. Lagraba , G. Luzon , A. Peiro

The Deep Underground Neutrino Experiment (DUNE) is a dual-site experiment for long baseline neutrino oscillation studies, and for neutrino astrophysics and nucleon decay searches. DUNE will comprise four 10 kton fiducial liquid argon…

Instrumentation and Detectors · Physics 2019-10-23 C. Cuesta

The DEAP-3600 experiment uses 3.6 tons of liquid argon for a sensitive dark matter search, with a sensitivity to the spin-independent WIMP-nucleon cross-section of $10^{-46}$ cm$^2$ at 100 GeV WIMP mass. This high sensitivity is achievable…

Instrumentation and Methods for Astrophysics · Physics 2019-08-14 Bei Cai

Boosted dark matter (BDM) is a well-motivated class of dark matter (DM) candidates in which a small component of DM is relativistic at the present time. We lay the foundation for BDM searches via hadronic interactions in large liquid-argon…

High Energy Physics - Phenomenology · Physics 2021-05-26 Joshua Berger , Yanou Cui , Mathew Graham , Lina Necib , Gianluca Petrillo , Dane Stocks , Yun-Tse Tsai , Yue Zhao

Very recently, the Xenon1T collaboration has reported an intriguing electron recoil excess, which may imply for light dark matter. In order to interpret this anomaly, we propose the atmospheric dark matter (ADM) from the inelastic collision…

High Energy Physics - Phenomenology · Physics 2021-01-04 Liangliang Su , Wenyu Wang , Lei Wu , Jin Min Yang , Bin Zhu

Dual-phase time projection chambers (TPCs) filled with the liquid noble gas xenon (LXe) are currently the most sensitive detectors searching for interactions of WIMP dark matter in a laboratory-based experiment. This is achieved by…

Instrumentation and Methods for Astrophysics · Physics 2014-08-08 Marc Schumann

The WIMP proposed here yields the observed abundance of dark matter, and is consistent with the current limits from direct detection, indirect detection, and collider experiments, if its mass is $\sim 72$ GeV/$c^2$. It is also consistent…

High Energy Physics - Phenomenology · Physics 2021-08-02 Reagan Thornberry , Maxwell Throm , Gabriel Frohaug , John Killough , Dylan Blend , Michael Erickson , Brian Sun , Brett Bays , Roland E. Allen
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