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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

The use of xenon-doped liquid argon is a promising alternative for large pure liquid-argon TPCs. Not only xenon-doped liquid argon enhances the light production, mitigating the possible suppression due to impurities, but also it increases…

Instrumentation and Detectors · Physics 2022-12-21 J. Soto-Oton , for DUNE Collaboration

The near-field photoluminescence of a gated two-dimensional electron gas is measured. We use the negatively charged exciton, formed by binding of an electron to a photo-excited electron-hole pair, as an indicator for the local presence of…

Mesoscale and Nanoscale Physics · Physics 2009-10-31 G. Eytan , Y. Yayon , M. Rappaport , H. Shtrikman , I. Bar-Joseph

Medium-energy electron beam-dump experiments provide an intense sources of secondary muons. These particles can be used to search for muon-coupling light dark scalars that may explain the $(g-2)_\mu$ anomaly. We applied this idea to SLAC…

High Energy Physics - Experiment · Physics 2018-12-26 L. Marsicano , M. Battaglieri , A. Celentano , R. De Vita , Yi-Ming Zhong

Monte Carlo simulations have been performed in order to evaluate the efficiencies of several light ions identification techniques. The detection system was composed with layers of scintillating material to measure either the deposited…

Nuclear Experiment · Physics 2013-10-02 S. Salvador , M. Labalme , J. M. Fontbonne , J. Dudouet , J. Colin , D. Cussol

A comprehensive model for describing the characteristics of pulsed signals, generated by particle interactions in xenon detectors, is presented. An emphasis is laid on two-phase time projection chambers, but the models presented are also…

Instrumentation and Detectors · Physics 2015-06-17 Jeremy Mock , Nichole Barry , Kareem Kazkaz , Matthew Szydagis , Mani Tripathi , Sergey Uvarov , Michael Woods , Nicholas Walsh

Within the MNPBEM toolbox, we show how to simulate electron energy loss spectroscopy (EELS) of plasmonic nanoparticles using a boundary element method approach. The methodology underlying our approach closely follows the concepts developed…

Mesoscale and Nanoscale Physics · Physics 2015-06-18 Ulrich Hohenester

This article reviews the progress made over the last 20 years in the development and applications of liquid xenon detectors in particle physics, astrophysics and medical imaging experiments. We begin with a summary of the fundamental…

Instrumentation and Detectors · Physics 2010-12-01 E. Aprile , T. Doke

Dual-phase liquid-xenon time projection chambers (LXe TPCs) deploying a few tonnes of liquid are presently leading the search for WIMP dark matter. Scaling these detectors to 10-fold larger fiducial masses, while improving their sensitivity…

Instrumentation and Detectors · Physics 2024-09-17 G. Martínez-Lema , A. Roy , A. Breskin , L. Arazi

Electron emission from liquid into gaseous xenon is a cornerstone of dark matter search detectors such as ZEPLIN, XENON, LUX and LZ. The probability of emission is a function of the applied electric field E, and electrons which fail to pass…

Instrumentation and Detectors · Physics 2017-02-17 Peter Sorensen

The XENON experiment aims at the direct detection of dark matter in the form of WIMPs (Weakly Interacting Massive Particles) via their elastic scattering off Xe nuclei. A fiducial mass of 1000 kg, distributed in ten independent liquid xenon…

In the search for a monochromatic peak as the signature of neutrinoless double beta decay an excellent energy resolution and an ultra-low background around the $Q$-value of the decay are essential. The LEGEND-200 experiment performs such a…

Instrumentation and Detectors · Physics 2023-02-02 L. Baudis , G. Benato , E. M. Bond , P. -J. Chiu , S. R. Elliott , R. Massarczyk , S. Meijer , Y. Müller

Electron-neutrino charged-current interactions with xenon nuclei were modeled in the nEXO neutrinoless double-$\beta$ decay detector (~5 metric ton, 90% ${}^{136}$Xe, 10% ${}^{134}$Xe) to evaluate its sensitivity to supernova neutrinos.…

High Energy Physics - Phenomenology · Physics 2024-12-02 nEXO Collaboration , S. Hedges , S. Al Kharusi , E. Angelico , J. P. Brodsky , G. Richardson , S. Wilde , A. Amy , A. Anker , I. J. Arnquist , P. Arsenault , A. Atencio , I. Badhrees , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Q. Cao , D. Cesmecioglu , E. Chambers , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , R. Collister , M. Cvitan , J. Dalmasson , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , Y. Y. Ding , M. J. Dolinski , B. Eckert , M. Elbeltagi , R. Elmansali , L. Fabris , W. Fairbank , J. Farine , N. Fatemighomi , B. Foust , Y. S. Fu , D. Gallacher , N. Gallice , W. Gillis , D. Goeldi , A. Gorham , R. Gornea , G. Gratta , Y. D. Guan , C. A. Hardy , M. Heffner , E. Hein , J. D. Holt , E. W. Hoppe , A. House , W. Hunt , A. Iverson , P. Kachru , A. Karelin , D. Keblbeck , A. Kuchenkov , K. S. Kumar , A. Larson , M. B. Latif , K. G. Leach , B. G. Lenardo , D. S. Leonard , H. Lewis , G. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , P. Martel-Dion , J. Masbou , K. McMichael , M. Medina-Peregrina , B. Mong , D. C. Moore , J. Nattress , C. R. Natzke , X. E. Ngwadla , K. Ni , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , J. L. Orrell , G. S. Ortega , C. T. Overman , L. Pagani , H. Peltz Smalley , A. Peña-Perez , A. Perna , A. Piepke , T. Pinto Franco , A. Pocar , J. -F. Pratte , H. Rasiwala , D. Ray , K. Raymond , S. Rescia , V. Riot , R. Ross , R. Saldanha , S. Sangiorgio , S. Schwartz , S. Sekula , J. Soderstrom , A. K. Soma , F. Spadoni , X. L. Sun , S. Thibado , A. Tidball , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , E. van Bruggen , M. Vidal , S. Viel , M. Walent , Q. D. Wang , W. Wang , Y. G. Wang , M. Watts , M. Wehrfritz , W. Wei , L. J. Wen , U. Wichoski , X. M. Wu , H. Xu , H. B. Yang , L. Yang , M. Yu , M. Yvaine , O. Zeldovich , J. Zhao

We report the first measurements of the absolute ionization yield of nuclear recoils in liquid xenon, as a function of energy and electric-field. Independent experiments were carried out with two dual-phase time projection chamber…

Dark matter detectors that utilize liquid xenon have now achieved tonne-scale targets, giving them sensitivity to all flavours of supernova neutrinos via coherent elastic neutrino-nucleus scattering. Considering for the first time a…

High Energy Astrophysical Phenomena · Physics 2016-12-21 Rafael F. Lang , Christopher McCabe , Shayne Reichard , Marco Selvi , Irene Tamborra

This thesis explores experimental and theoretical approaches to dark matter detection, from gas-based detectors to quantum sensors, tackling the challenge of identifying dark matter, which makes up 27% of the Universe's energy. It reviews…

Instrumentation and Methods for Astrophysics · Physics 2025-12-05 David Díez-Ibáñez

Decays of the neutral and long-lived $\eta$ and $\eta'$ mesons provide a unique, flavor-conserving laboratory to test low-energy Quantum Chromodynamics and search for new physics beyond the Standard Model. They have drawn world-wide…

High Energy Physics - Phenomenology · Physics 2022-01-05 Liping Gan , Bastian Kubis , Emilie Passemar , Sean Tulin

An ultimate liquid xenon experiment would be limited in its dark matter science reach by irreducible neutrino backgrounds, which are an exciting signal in their own right. To achieve such sensitivity, other backgrounds that currently plague…

High Energy Physics - Experiment · Physics 2024-02-27 Abigail Kopec

Proportional electroluminescence (EL) in noble gases is used in two-phase detectors for dark matter search to record ionization signals in the gas phase induced by particle scattering in the liquid phase (S2 signals). In this work, the EL…

Instrumentation and Detectors · Physics 2020-07-06 A. Bondar , E. Borisova , A. Buzulutskov , E. Frolov , V. Oleynikov , A. Sokolov

If dark matter self-annihilates into neutrinos or a second component of ("boosted") dark matter that is nucleophilic, the annihilation products may be detected with high rates via coherent nuclear scattering. A future multi-ten-tonne liquid…

High Energy Physics - Phenomenology · Physics 2019-05-22 David McKeen , Nirmal Raj