English
Related papers

Related papers: Backgrounds and pulse shape discrimination in the …

200 papers

The scintillation time response of liquid argon has a key role in the discrimination of electronic backgrounds in dark matter search experiments. However, its extraordinary rejection power can be affected by various detector effects such as…

The neutron capture is a process that concerns most of the nuclei used to build our detectors. This process produces protons, alpha particles, and gamma rays which generate background signals. Characterizing this background is important for…

Instrumentation and Detectors · Physics 2026-04-06 Ilias Ourahou , Daniel Santos , Olivier Guillaudin , Pierre Louis-Cistac , Fairouz Malek , Nadine Sauzet , Charling Tao

The effect of driving frequency in the range of 13.56 MHz to 73 MHz on electron energy distribution and electron heating modes in a 50 mTorr capacitively coupled argon plasma discharge is studied using 1D-3V particle-in-cell simulations.…

We have constructed a liquid Argon TPC detector with fiducial mass of 150 kg as a part of the R&D program of the next generation neutrino and nucleon decay detector. This paper describes a study of particle identification performance of the…

The success of the ambitious programs of both long- and short-baseline neutrino-oscillation experiments employing liquid-argon time-projection chambers will greatly rely on the precision with which the weak response of the argon nucleus can…

A large area (0.5~m $\times$ 0.5~m) thermal neutron detector was developed based on 0.32~mm-thick $^{6}$LiF:ZnS(Ag) scintillator sheets. The detector was constructed for measurements of seasonal variations in low intensity thermal neutron…

Instrumentation and Detectors · Physics 2018-07-24 Alexandre Kozlov , Dmitry Chernyak

We present a measurement of the combined $\nu_e$ + $\bar{\nu}_e$ flux-averaged charged-current inclusive cross section on argon using data from the MicroBooNE liquid argon time projection chamber (LArTPC) at Fermilab. Using the off-axis…

High Energy Physics - Experiment · Physics 2021-09-15 MicroBooNE collaboration , P. Abratenko , M. Alrashed , R. An , J. Anthony , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , C. Barnes , G. Barr , V. Basque , L. Bathe-Peters , O. Benevides Rodrigues , S. Berkman , A. Bhanderi , A. Bhat , M. Bishai , A. Blake , T. Bolton , L. Camilleri , D. Caratelli , I. Caro Terrazas , R. Castillo Fernandez , F. Cavanna , G. Cerati , Y. Chen , E. Church , D. Cianci , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , M. Del Tutto , S. R. Dennis , D. Devitt , R. Diurba , L. Domine , R. Dorrill , K. Duffy , S. Dytman , B. Eberly , A. Ereditato , L. Escudero Sanchez , J. J. Evans , 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 , E. Hall , P. Hamilton , O. Hen , C. Hill , G. A. Horton-Smith , A. Hourlier , R. Itay , C. James , J. Jan de Vries , X. Ji , L. Jiang , J. H. Jo , R. A. Johnson , Y. J. Jwa , N. Kamp , N. Kaneshige , G. Karagiorgi , W. Ketchum , B. Kirby , M. Kirby , T. Kobilarcik , I. Kreslo , R. LaZur , I. Lepetic , K. Li , Y. Li , B. R. Littlejohn , D. Lorca , W. C. Louis , X. Luo , A. Marchionni , C. Mariani , D. Marsden , 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 , A. F. Moor , C. D. Moore , L. Mora Lepin , J. Mousseau , M. Murphy , D. Naples , A. Navrer-Agasson , R. K. Neely , P. Nienaber , J. Nowak , O. Palamara , V. Paolone , A. Papadopoulou , V. Papavassiliou , S. F. Pate , A. Paudel , Z. Pavlovic , E. Piasetzky , I. Ponce-Pinto , D. Porzio , S. Prince , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , L. Ren , L. Rochester , J. Rodriguez Rondon , H. E. Rogers , M. Rosenberg , M. Ross-Lonergan , 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 , C. Thorpe , M. Toups , Y. -T. Tsai , M. A. Uchida , T. Usher , W. Van De Pontseele , B. Viren , M. Weber , H. Wei , Z. Williams , S. Wolbers , T. Wongjirad , M. Wospakrik , W. Wu , E. Yandel , T. Yang , G. Yarbrough , L. E. Yates , G. P. Zeller , J. Zennamo , C. Zhang

Building on the successful experience in operating the DarkSide-50 detector, the DarkSide Collaboration is going to construct DarkSide-20k, a direct WIMP search detector using a two-phase Liquid Argon Time Projection Chamber (LArTPC) with…

Instrumentation and Detectors · Physics 2018-08-09 C. E. Aalseth , F. Acerbi , P. Agnes , I. F. M. Albuquerque , T. Alexander , A. Alici , A. K. Alton , P. Antonioli , S. Arcelli , R. Ardito , I. J. Arnquist , D. M. Asner , M. Ave , H. O. Back , A. I. Barrado Olmedo , G. Batignani , E. Bertoldo , S. Bettarini , M. G. Bisogni , V. Bocci , A. Bondar , G. Bonfini , W. Bonivento , M. Bossa , B. Bottino , M. Boulay , R. Bunker , S. Bussino , A. Buzulutskov , M. Cadeddu , M. Cadoni , A. Caminata , N. Canci , A. Candela , C. Cantini , M. Caravati , M. Cariello , M. Carlini , M. Carpinelli , A. Castellani , S. Catalanotti , V. Cataudella , P. Cavalcante , S. Cavuoti , R. Cereseto , A. Chepurnov , C. Cicalò , L. Cifarelli , M. Citterio , A. G. Cocco , M. Colocci , S. Corgiolu , G. Covone , P. Crivelli , I. D'Antone , M. D'Incecco , D. D'Urso , M. D. Da Rocha Rolo , M. Daniel , S. Davini , A. de Candia , S. De Cecco , M. De Deo , G. De Filippis , G. De Guido , G. De Rosa , G. Dellacasa , M. Della Valle , P. Demontis , A. Derbin , A. Devoto , F. Di Eusanio , G. Di Pietro , C. Dionisi , A. Dolgov , I. Dormia , S. Dussoni , A. Empl , M. Fernandez Diaz , A. Ferri , C. Filip , G. Fiorillo , K. Fomenko , D. Franco , G. E. Froudakis , F. Gabriele , A. Gabrieli , C. Galbiati , P. Garcia Abia , A. Gendotti , A. Ghisi , S. Giagu , P. Giampa , G. Gibertoni , C. Giganti , M. A. Giorgi , G. K. Giovanetti , M. L. Gligan , A. Gola , O. Gorchakov , A. M. Goretti , F. Granato , M. Grassi , J. W. Grate , G. Y. Grigoriev , M. Gromov , M. Guan , M. B. B. Guerra , M. Guerzoni , M. Gulino , R. K. Haaland , A. Hallin , B. Harrop , E. W. Hoppe , S. Horikawa , B. Hosseini , D. Hughes , P. Humble , E. V. Hungerford , An. Ianni , C. Jillings , T. N. Johnson , K. Keeter , C. L. Kendziora , S. Kim , G. Koh , D. Korablev , G. Korga , A. Kubankin , M. Kuss , M. Kuźniak , B. Lehnert , X. Li , M. Lissia , G. U. Lodi , B. Loer , G. Longo , P. Loverre , R. Lussana , L. Luzzi , Y. Ma , A. A. Machado , I. N. Machulin , A. Mandarano , L. Mapelli , M. Marcante , A. Margotti , S. M. Mari , M. Mariani , J. Maricic , C. J. Martoff , M. Mascia , M. Mayer , A. B. McDonald , A. Messina , P. D. Meyers , R. Milincic , A. Moggi , S. Moioli , J. Monroe , A. Monte , M. Morrocchi , B. J. Mount , W. Mu , V. N. Muratova , S. Murphy , P. Musico , R. Nania , A. Navrer Agasson , I. Nikulin , V. Nosov , A. O. Nozdrina , N. N. Nurakhov , 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 , K. Pelczar , L. A. Pellegrini , N. Pelliccia , F. Perotti , R. Perruzza , V. Pesudo Fortes , C. Piemonte , F. Pilo , A. Pocar , T. Pollmann , D. Portaluppi , D. A. Pugachev , H. Qian , B. Radics , F. Raffaelli , F. Ragusa , M. Razeti , A. Razeto , V. Regazzoni , C. Regenfus , B. Reinhold , A. L. Renshaw , M. Rescigno , F. Retière , Q. Riffard , A. Rivetti , S. Rizzardini , A. Romani , L. Romero , B. Rossi , N. Rossi , A. Rubbia , D. Sablone , P. Salatino , O. Samoylov , E. Sánchez García , W. Sands , M. Sant , R. Santorelli , C. Savarese , E. Scapparone , B. Schlitzer , G. Scioli , E. Segreto , A. Seifert , D. A. Semenov , A. Shchagin , L. Shekhtman , E. Shemyakina , A. Sheshukov , M. Simeone , P. N. Singh , P. Skensved , M. D. Skorokhvatov , O. Smirnov , G. Sobrero , A. Sokolov , A. Sotnikov , F. Speziale , R. Stainforth , C. Stanford , G. B. Suffritti , Y. Suvorov , R. Tartaglia , G. Testera , A. Tonazzo , A. Tosi , P. Trinchese , E. V. Unzhakov , A. Vacca , E. Vázquez-Jáuregui , M. Verducci , T. Viant , F. Villa , A. Vishneva , B. Vogelaar , M. Wada , J. Wahl , J. Walding , S. Walker , H. Wang , Y. Wang , A. W. Watson , S. Westerdale , R. Williams , M. M. Wojcik , S. Wu , X. Xiang , X. Xiao , C. Yang , Z. Ye , A. Yllera de Llano , F. Zappa , G. Zappalà , C. Zhu , A. Zichichi , M. Zullo , A. Zullo

The DEAP-1 \SI{7}{kg} single phase liquid argon scintillation detector was operated underground at SNOLAB in order to test the techniques and measure the backgrounds inherent to single phase detection, in support of the \mbox{DEAP-3600}…

A new method of searching for dark matter in the form of weakly interacting massive particles (WIMP) has been developed with the direct detection of the low energy nuclear recoils observed in a massive target (ultimately many tons) of ultra…

DarkSide-50 achieved leading WIMP limits down to 1.2 GeV/c2 with an ionization-only analysis, despite its small active mass of 46 kg compared to multi-ton noble-liquid detectors. Accurate modelling of the nuclear-recoil ionization yield…

High Energy Physics - Experiment · Physics 2026-01-28 Davide Franco

We present a study on the dependence of electric breakdown discharge properties on electrode geometry and the breakdown field in liquid argon near its boiling point. The measurements were performed with a spherical cathode and a planar…

Instrumentation and Detectors · Physics 2016-03-17 M. Auger , A. Blatter , A. Ereditato , D. Goeldi , S. Janos , I. Kreslo , M. Luethi , C. Rudolf von Rohr , T. Strauss , M. S. Weber

We present a real-time anomaly detection framework for liquid argon time projection chambers (LArTPCs), targeting applications in particle physics experiments such as the Short Baseline Near Detector or the future Deep Underground Neutrino…

High Energy Physics - Experiment · Physics 2026-05-28 Seokju Chung , Jack Cleeve , Akshay Malige , Georgia Karagiorgi , Lino Gerlach , Adrian A. Pol , Isobel Ojalvo

The Alpha Magnetic Spectrometer (AMS) is a high-precision particle detector onboard the International Space Station containing six different subdetectors. The Transition Radiation Detector and Electromagnetic Calorimeter (ECAL) are used to…

High Energy Physics - Experiment · Physics 2025-02-07 Raheem Karim Hashmani , Emre Akbaş , Melahat Bilge Demirköz

Liquid argon is an excellent medium for detecting particles, given its yields and transport properties of light and charge. The technology of liquid argon time projection chambers has reached its full maturity after four decades of…

High Energy Physics - Experiment · Physics 2024-05-03 Ettore Segreto

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

The possibility of nuclear reactions within a low voltage DC deuterium discharge with palladium electrodes is addressed. The solid-state nuclear track detector known as CR-39 was chosen to investigate the emission of energetic charged…

Nuclear Experiment · Physics 2024-02-09 Erik P. Ziehm , George H. Miley

The Lennard-Jones (LJ) potential is a cornerstone of Molecular Dynamics (MD) simulations and among the most widely used computational kernels in science. The potential models atomistic attraction and repulsion with century old prescribed…

Emerging studies are geared toward exploring new methods of nuclear rocket propulsion to provide more efficient space transit beyond Earth's orbit. One method is to employ a Fission Fragment Rocket Engine utilizing fissionable layers…

Instrumentation and Detectors · Physics 2024-05-29 Sandeep Puri , Andrew Gillespie , Ian Jones , Cuikun Lin , Ryan Weed , Robert V. Duncan

The AMANDE facility at IRSN-Cadarache produces mono-energetic neutron fields from 2 keV to 20 MeV with metrological quality. To be considered as a standard facility, characteristics of neutron field i.e fluence distribution must be well…

Instrumentation and Detectors · Physics 2009-12-08 A. Allaoua , O. Guillaudin , S. Higueret , D. Husson , L. Lebreton , F. Mayet , M. Nourreddine , D. Santos , A. Trichet