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The NEXT-DEMO++ detector, a high-pressure xenon gas time projection chamber serving as a prototype for the NEXT-100 experiment, was used to measure the electroluminescence (EL) yield as a function of reduced electric field ($E/p$) across…

Instrumentation and Detectors · Physics 2026-04-20 NEXT Collaboration , J. Renner , J. D. Villamil , N. López-March , K. Mistry , P. Novella , A. Simón , V. Álvarez , J. M. Benlloch-Rodríguez , M. Cid , C. Cortes-Parra , R. Esteve , F. Kellerer , J. Martín-Albo , A. Martínez , G. Martínez-Lema , M. Martínez-Vara , M. Querol , P. Saharia , M. Sorel , S. Teruel-Pardo , H. Almazán , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , Y. Ayyad , C. D. R. Azevedo , F. Ballester , J. E. Barcelon , M. del Barrio-Torregrosa , F. I. G. M. Borges , A. Brodoline , N. Byrnes , A. Castillo , E. Church , X. Cid , C. A. N. Conde , F. P. Cossío , R. Coupe , E. Dey , P. Dietz , C. Echeverria , M. Elorza , R. Felkai , L. M. P. Fernandes , P. Ferrario , P. Ferrero Mancheño , F. W. Foss , Z. Freixa , J. García-Barrena , J. J. Gómez-Cadenas , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , A. F. B. Isabel , B. J. P. Jones , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , R. Madigan , R. D. P. Mano , A. Marauri , A. P. Marques , R. L. Miller , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , D. R. Nygren , E. Oblak , I. Osborne , J. Palacio , B. Palmeiro , A. Para , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Pérez Maneiro , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , E. Ruiz-Chóliz , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , A. L. M. Silva , P. A. O. C. Silva , S. R. Soleti , J. Soto-Oton , J. M. R. Teixeira , J. F. Toledo , C. Tonnelé , S. Torelli , J. Torrent , A. Trettin , P. R. G. Valle , M. Vanga , P. Vázquez Cabaleiro , J. F. C. A. Veloso , L. M. Villar Padruno , J. Waiton , A. Yubero-Navarro

The PANCAKE facility is the world's largest liquid xenon test platform. Inside its cryostat with an internal diameter of 2.75 m, components for the next generation of liquid xenon experiments, such as DARWIN or XLZD, will be tested at their…

We have built and operated a crystalline/vapor xenon TPC, with the goal of improving searches for dark matter. The motivation for this instrument is the fact that beta decays from the radon decay chain to the ground state presently limit…

Instrumentation and Detectors · Physics 2022-05-04 S. Kravitz , H. Chen , R. Gibbons , S. J. Haselschwardt , Q. Xia , P. Sorensen

The technique to realize 3D position sensitivity in a two-phase xenon time projection chamber (XeTPC) for dark matter search is described. Results from a prototype detector (XENON3) are presented.

The Large Underground Xenon (LUX) collaboration has designed and constructed a dual-phase xenon detector, in order to conduct a search for Weakly Interacting Massive Particles(WIMPs), a leading dark matter candidate. The goal of the LUX…

Two cryogenic bath-type heat exchangers for ultra-pure noble gas applications were developed with particular emphasis on noble gas liquefaction in cryogenic distillation systems. The main objective was to construct heat exchangers for xenon…

Instrumentation and Detectors · Physics 2022-06-08 M. Murra , D. Schulte , I. Cristescu , J. -M. Disdier , C. Huhmann , D. Tatananni , C. Weinheimer

The next-generation of $0\nu\beta\beta$ searches are targeting half-life sensitivities towards 10$^{27}$--10$^{28}$ years. Gaseous xenon time projection chamber (GXeTPC) detectors may be able to meet this challenge due to their excellent…

Instrumentation and Detectors · Physics 2026-03-19 K. Mistry , Y. Mei , D. R. Nygren

The performance of a detector using liquid xenon (LXe) as a scintillator is strongly dependent on the collection efficiency for xenon scintillation light, which in turn is critically dependent on the reflectance of the surfaces that…

Instrumentation and Detectors · Physics 2017-03-08 F. Neves , A. Lindote , A. Morozov , V. Solovov , C. Silva , P. Bras , J. P. Rodrigues , M. I. Lopes

XENON10 is the first two-phase xenon time projection chamber (TPC) developed within the XENON dark matter search program. The TPC, with an active liquid xenon (LXe) mass of about 14 kg, was installed at the Gran Sasso underground laboratory…

The XMASS detector is a large single phase liquid Xenon scintillator.After its feasibility had been studied using a 100 kg size prototype detector, an 800 kg size detector is being built for dark matter search with the sensitivity of…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 Hiroyuki Sekiya

We briefly discuss the expected level of supersymmetric dark matter cross-sections as a reference for dark matter detectors. We then discuss the current ZEPLIN II program as a prototype of large liquid Xenon detectors. Cryoarray is a…

Astrophysics · Physics 2007-05-23 David B. Cline

LXeGRIT is the first prototype of a novel concept of Compton telescope, based on the complete 3-dimensional reconstruction of the sequence of interactions of individual gamma rays in one position sensitive detector. This balloon-borne…

This manuscript details the proof-of-concept of a small-scale cryogenic heat pump demonstrator, a technology designed to enable high-flow xenon distillation systems for the removal of $^{222}$Rn in future liquid xenon observatories such as…

Instrumentation and Detectors · Physics 2026-04-23 P. Schulte , D. Wenz , L. Althueser , R. Braun , V. Hannen , C. Huhmann , D. Koke , Y. -T. Lin , P. Unkhoff , C. Weinheimer

Detectors based on liquid or gas xenon have been used and are in use for a number of applications, in particular for the detection of gamma rays. Xenon is a well-suited medium for gamma spectroscopy thanks to its high atomic number and,…

Instrumentation and Detectors · Physics 2013-09-10 F. Resnati

We present a detector apparatus, DireXeno (DIRectinal Xenon), designed to measure the spatial and temporal properties of scintillation in liquid xenon to very high accuracy. The properties of scintillation are of primary importance for dark…

Instrumentation and Detectors · Physics 2020-06-17 R. Itay , P. Z. Szabo , G. Koltman , M. M. Devi , M. Shutman , H. Landsman , R. Budnik

Micromegas is a type of micro-pattern gaseous detector currently under R&D for applications in rare event search experiments. Here we report the performance of a Micromegas structure constructed with a micromesh thermo-bonded to a readout…

Instrumentation and Detectors · Physics 2014-05-13 Yuehuan Wei , Liang Guan , Zhiyong Zhang , Qing Lin , Xiaolian Wang , Kaixuan Ni , Tianchi Zhao

We characterize single- and few-electron backgrounds that are observed in dual-phase liquid xenon time projection chambers at timescales greatly exceeding a maximum drift time after an interaction. These instrumental backgrounds limit a…

Instrumentation and Detectors · Physics 2021-07-13 Abigail Kopec , Amanda L. Baxter , Michael Clark , Rafael F. Lang , Shengchao Li , Juehang Qin , Riya Singh

The Cornell Electron-positron Storage Ring (CESR) has been converted from a High Energy Physics electron-positron collider to operate as a dedicated synchrotron light source for the Cornell High Energy Synchrotron Source (CHESS) and to…

A new design for the anode of a time projection chamber, consisting of a charge-detecting "tile", is investigated for use in large scale liquid xenon detectors. The tile is produced by depositing 60 orthogonal metal charge-collecting…

Instrumentation and Detectors · Physics 2018-01-23 nEXO Collaboration , M. Jewell , A. Schubert , W. R. Cen , J. Dalmasson , R. DeVoe , L. Fabris , G. Gratta , A. Jamil , G. Li , A. Odian , M. Patel , A. Pocar , D. Qiu , Q. Wang , L. J. Wen , J. B. Albert , G. Anton , I. J. Arnquist , I. Badhrees , P. Barbeau , D. Beck , V. Belov , F. Bourque , J. P. Brodsky , E. Brown , T. Brunner , A. Burenkov , G. F. Cao , L. Cao , C. Chambers , S. A. Charlebois , M. Chiu , B. Cleveland , M. Coon , A. Craycraft , W. Cree , M. Côté , T. Daniels , S. J. Daugherty , J. Daughhetee , S. Delaquis , A. Der Mesrobian-Kabakian , T. Didberidze , J. Dilling , Y. Y. Ding , M. J. Dolinski , A. Dragone , W. Fairbank , J. Farine , S. Feyzbakhsh , R. Fontaine , D. Fudenberg , G. Giacomini , R. Gornea , E. V. Hansen , D. Harris , M. Hasan , M. Heffner , E. W. Hoppe , A. House , P. Hufschmidt , M. Hughes , J. Hößl , Y. Ito , A. Iverson , X. S. Jiang , S. Johnston , A. Karelin , L. J. Kaufman , T. Koffas , S. Kravitz , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , D. S. Leonard , S. Li , Z. Li , C. Licciardi , Y. H. Lin , R. MacLellan , T. Michel , B. Mong , D. Moore , K. Murray , R. J. Newby , Z. Ning , O. Njoya , F. Nolet , K. Odgers , M. Oriunno , J. L. Orrell , I. Ostrovskiy , C. T. Overman , G. S. Ortega , S. Parent , A. Piepke , J. -F. Pratte , V. Radeka , E. Raguzin , T. Rao , S. Rescia , F. Retiere , A. Robinson , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , S. Sangiorgio , S. Schmidt , J. Schneider , D. Sinclair , K. Skarpaas , A. K. Soma , G. St-Hilaire , V. Stekhanov , T. Stiegler , X. L. Sun , M. Tarka , J. Todd , T. Tolba , R. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , G. Visser , J. -L. Vuilleumier , M. Wagenpfeil , M. Weber , W. Wei , U. Wichoski , G. Wrede , S. X. Wu , W. H. Wu , Z. Xuan , L. Yang , D. Yayun , Y. -R. Yen , O. Zeldovich , X. Zhang , J. Zhao , N. Zhe , Y. Zhou , T. Ziegler
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