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A particle detection system that exploits the scintillation light produced by ionizing particles in liquid argon (LAr) has been assembled at CERN. The system is based on 10 large-area photomultiplier tubes (PMT) immersed in a 1500-liter…

Proportional electroluminescence (EL) in noble gases is used in two-phase detectors for dark matter searches to record (in the gas phase) the ionization signal induced by particle scattering in the liquid phase. The "standard" EL mechanism…

Instrumentation and Detectors · Physics 2021-03-01 The DarkSide collaboration , C. E. Aalseth , S. Abdelhakim , P. Agnes , R. Ajaj , I. F. M. Albuquerque , T. Alexander , A. Alici , A. K. Alton , P. Amaudruz , F. Ameli , J. Anstey , P. Antonioli , M. Arba , S. Arcelli , R. Ardito , I. J. Arnquist , P. Arpaia , D. M. Asner , A. Asunskis , M. Ave , H. O. Back , V. Barbaryan , A. Barrado Olmedo , G. Batignani , M. G. Bisogni , V. Bocci , A. Bondar , G. Bonfini , W. Bonivento , E. Borisova , B. Bottino , M. G. Boulay , R. Bunker , S. Bussino , A. Buzulutskov , M. Cadeddu , M. Cadoni , A. Caminata , N. Canci , A. Candela , C. Cantini , M. Caravati , M. Cariello , F. Carnesecchi , A. Castellani , P. Castello , P. Cavalcante , D. Cavazza , S. Cavuoti , S. Cebrian , J. M. Cela Ruiz , B. Celano , R. Cereseto , S. Chashin , W. Cheng , A. Chepurnov , C. Cicalò , L. Cifarelli , M. Citterio , F. Coccetti , V. Cocco , M. Colocci , E. Conde Vilda , L. Consiglio , F. Cossio , G. Covone , P. Crivelli , I. D'Antone , M. D'Incecco , M. D. Da Rocha Rolo , O. Dadoun , M. Daniel , S. Davini , S. De Cecco , M. De Deo , A. De Falco , D. De Gruttola , G. De Guido , G. De Rosa , G. Dellacasa , P. Demontis , S. De Pasquale , A. V. Derbin , A. Devoto , F. Di Eusanio , L. Di Noto , G. Di Pietro , P. Di Stefano , C. Dionisi , G. Dolganov , F. Dordei , M. Downing , F. Edalatfar , A. Empl , M. Fernandez Diaz , C. Filip , G. Fiorillo , K. Fomenko , A. Franceschi , D. Franco , E. Frolov , G. E. Froudakis , N. Funicello , F. Gabriele , A. Gabrieli , C. Galbiati , M. Garbini , P. Garcia Abia , D. Gascón Fora , A. Gendotti , C. Ghiano , A. Ghisi , P. Giampa , R. A. Giampaolo , C. Giganti , M. A. Giorgi , G. K. Giovanetti , M. L. Gligan , O. Gorchakov , M. Grab , R. Graciani Diaz , M. Grassi , J. W. Grate , A. Grobov , M. Gromov , M. Guan , M. B. B. Guerra , M. Guerzoni , M. Gulino , R. K. Haaland , B. R. Hackett , A. Hallin , M. Haranczyk , B. Harrop , E. W. Hoppe , S. Horikawa , B. Hosseini , F. Hubaut , P. Humble , E. V. Hungerford , An. Ianni , A. Ilyasov , V. Ippolito , C. Jillings , K. Keeter , C. L. Kendziora , I. Kochanek , K. Kondo , G. Kopp , D. Korablev , G. Korga , A. Kubankin , R. Kugathasan , M. Kuss , M. La Commara , L. La Delfa , M. Lai , M. Lebois , B. Lehnert , N. Levashko , X. Li , Q. Liqiang , M. Lissia , G. U. Lodi , G. Longo , R. Lussana , L. Luzzi , A. A. Machado , I. N. Machulin , A. Mandarano , S. Manecki , L. Mapelli , A. Margotti , S. M. Mari , M. Mariani , J. Maricic , M. Marinelli , D. Marras , M. Martínez , A. D. Martinez Rojas , M. Mascia , J. Mason , A. Masoni , A. B. McDonald , A. Messina , T. Miletic , R. Milincic , A. Moggi , S. Moioli , J. Monroe , M. Morrocchi , T. Mroz , W. Mu , V. N. Muratova , S. Murphy , C. Muscas , P. Musico , R. Nania , T. Napolitano , A. Navrer Agasson , M. Nessi , I. Nikulin , V. Nosov , J. A. Nowak , A. Oleinik , V. Oleynikov , M. Orsini , F. Ortica , L. Pagani , M. Pallavicini , S. Palmas , L. Pandola , E. Pantic , E. Paoloni , F. Pazzona , S. Peeters , P. A. Pegoraro , K. Pelczar , L. A. Pellegrini , C. Pellegrino , N. Pelliccia , F. Perotti , V. Pesudo , E. Picciau , F. Pietropaolo , A. Pocar , T. R. Pollmann , D. Portaluppi , S. S. Poudel , P. Pralavorio , D. Price , B. Radics , F. Raffaelli , F. Ragusa , M. Razeti , C. Regenfus , A. L. Renshaw , S. Rescia , M. Rescigno , F. Retiere , L. P. Rignanese , C. Ripoli , A. Rivetti , J. Rode , A. Romani , L. Romero , N. Rossi , A. Rubbia , P. Sala , P. Salatino , O. Samoylov , E. Sánchez García , E. Sandford , S. Sanfilippo , M. Sant , D. Santone , R. Santorelli , C. Savarese , E. Scapparone , B. Schlitzer , G. Scioli , E. Segreto , A. Seifert , D. A. Semenov , A. Shchagin , A. Sheshukov , S. Siddhanta , M. Simeone , P. N. Singh , P. Skensved , M. D. Skorokhvatov , O. Smirnov , G. Sobrero , A. Sokolov , A. Sotnikov , R. Stainforth , A. Steri , S. Stracka , V. Strickland , G. B. Suffritti , S. Sulis , Y. Suvorov , A. M. Szelc , R. Tartaglia , G. Testera , T. Thorpe , A. Tonazzo , A. Tosi , M. Tuveri , E. V. Unzhakov , G. Usai , A. Vacca , E. Vázquez-Jáuregui , T. Viant , S. Viel , F. Villa , A. Vishneva , R. B. Vogelaar , J. Wahl , J. J. Walding , H. Wang , Y. Wang , S. Westerdale , R. J. Wheadon , R. Williams , J. Wilson , Ma. M. Wojcik , Ma. Wojcik , S. Wu , X. Xiao , C. Yang , Z. Ye , M. Zuffa , G. Zuzel

In our effort to develop a new kind of detector for low-energy, low-rate energy deposition events we have investigated the cathodo- and radioluminescence of Ho:YAG and Ho:YLF single crystals in an extended wavelength range from $200\,$nm to…

Atomic Physics · Physics 2018-08-01 F. Chiossi , A. F. Borghesani , G. Carugno

A large number of particle detectors employ liquid argon as their target material owing to its high scintillation yield and its ability to drift ionization charge over large distances. Scintillation light from argon is peaked at 128 nm and…

We examine the near-infrared (NIR) emission from low-luminosity AGNs (LLAGNs). Our galaxy sample includes 15 objects with detected 2-10 keV X-ray emission, dynamical black hole mass estimates from the literature, and available Gemini/NIFS…

Astrophysics of Galaxies · Physics 2020-01-15 Antoine Dumont , Anil Seth , Jay Strader , Jenny E. Greene , Leonard Burtscher , Nadine Neumayer

Liquid xenon is an important detection medium in direct dark matter experiments, which search for low-energy nuclear recoils produced by the elastic scattering of WIMPs with quarks. The two existing measurements of the relative…

A new experimental equipment allowing to study the sputtering induced by ion beam irradiation is presented. The sputtered particles are collected on a catcher which is analyzed in situ by Auger electron spectroscopy without breaking the…

Instrumentation and Detectors · Physics 2013-06-06 P. Salou , H. Lebius , A. Benyagoub , T. Langlinay , D. Lelièvre , B. Ban-d'Etat

The yields of identified particles have been measured at RHIC for Au+Au collisions at sqrt{s_NN} = 200 GeV using the PHOBOS spectrometer. The ratios of antiparticle to particle yields near mid-rapidity are presented. The first measurements…

Nuclear Experiment · Physics 2008-11-26 Barbara Wosiek

We have exposed a dual-phase Liquid Argon Time Projection Chamber (LAr-TPC) to a low energy pulsed narrowband neutron beam, produced at the Notre Dame Institute for Structure and Nuclear Astrophysics to study the scintillation light yield…

We have measured the properties of scintillation light in liquid argon doped with xenon concentrations from 165 ppm to 10,010 ppm using a $^{22}$Na source. The energy transfer processes in the xenon-doped liquid argon are discussed in…

Instrumentation and Detectors · Physics 2021-02-03 Y. Y. Gan , M. Y. Guan , Y. P. Zhang , P. Zhang , C. G. Yang , Q. Zhao , Y. T. Wei , W. X. Xiong

In order to detect ultrahigh-energy cosmic rays (UHECR), atmospheric fluorescence light from the trajectory of the extensive air shower may be measured by mirror-photosensor systems. In this type of experiment the photon yield from…

Astrophysics · Physics 2009-11-07 M. Nagano , K. Kobayakawa , N. Sakaki , K. Ando

Xenon scintillation has been widely used in rare event detection experiments such as neutrinoless double beta decay, double electron captures and dark matter searches. Nonetheless, experimental values for primary scintillation yield in…

Instrumentation and Methods for Astrophysics · Physics 2023-10-05 C. A. O. Henriques , J. M. R. Teixeira , P. A. O. C. Silva , R. D. P. Mano , J. M. F. dos Santos , C. M. B. Monteiro

Measurements are reported of the yield and spectrum of fluorescence, excited by a 28.5 GeV electron beam, in air at a range of pressures of interest to ultra-high energy cosmic ray detectors. The wavelength range was 300 - 420 nm. System…

In this paper we examine properties of the variable source Sgr A* in the near-infrared (NIR) using a very extensive Ks-band data set from NACO/VLT observations taken 2004 to 2009. We investigate the variability of Sgr A* with two different…

Knowledge of the neutron light-yield response is crucial to the understanding of scintillator-based neutron detectors. In this work, neutrons from 2--6 MeV have been used to study the scintillation light-yield response of the liquid…

Scintillation light generated as charged particles traverse large liquid argon detectors adds valuable information to studies of weakly-interacting particles. This paper uses both laboratory measurements and cosmic ray data from the Blanche…

Instrumentation and Detectors · Physics 2018-07-05 B. Howard , S. Mufson , D. Whittington , B. Adams , B. Baugh , J. R. Jordan , J. Karty , C. T. Macias , A. Pla-Dalmau

The air fluorescence technique is used to detect ultra-high energy cosmic rays (UHECR), and to estimate their energy. Of fundamental importance is the photon yield due to excitation by electrons, in air of various densities and…

Astrophysics · Physics 2009-11-10 M. Nagano , K. Kobayakawa , N. Sakaki , K. Ando

Ionization of atoms and molecules in strong laser fields is a fundamental process in many fields of research, especially in the emerging field of attosecond science. So far, demonstrably accurate data have only been acquired for atomic…

Detailed understanding of the ionization process in noble liquid detectors is important for their use in applications such as the search for dark matter and coherent elastic neutrino-nucleus scattering. The response of noble liquid…

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