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Liquid-xenon based particle detectors have been dramatically growing in size during the last years, and are now exceeding the one-ton scale. The required high xenon purity is usually achieved by continuous recirculation of xenon gas through…

Instrumentation and Detectors · Physics 2011-03-08 K. L. Giboni , E. Aprile , B. Choi , T. Haruyama , R. F. Lang , K. E. Lim , A. J. Melgarejo , G. Plante

We have developed an efficient cryogenic system with heat exchange and associated gas purification system, as a prototype for the XENON1T experiment. The XENON1T detector will use about 3 ton of liquid xenon (LXe) at a temperature of 175K…

Instrumentation and Detectors · Physics 2015-06-11 Elena Aprile , Ran Budnik , Bin Choi , Hugo Contreras , Karl Giboni , Luke Goetzke , Rafael Lang , Kyungeun Lim , Antonio melgarejo , Petr Shagin

The experiment for the 2$\beta$-decay of $^{136}$Xe search with two high-pressure copper proportional counters has been held in Baksan neutrino observatory. The search for the process is based on comparison of spectra measured with natural…

Nuclear Experiment · Physics 2008-11-26 Ju. M. Gavriljuk , A. M. Gangapshev , V. V. Kuzminov , S. I. Panasenko , S. S. Ratkevich

Scintillator detectors can be used in experiments searching for neutrinoless double beta decay. A wide variety of double beta decay candidate isotopes can be made into scintillators or can be loaded into scintillators. Experimental programs…

Instrumentation and Detectors · Physics 2008-12-18 Mark C. Chen

The multi-staged XENON program at INFN Laboratori Nazionali del Gran Sasso aims to detect dark matter with two-phase liquid xenon time projection chambers of increasing size and sensitivity. The XENONnT experiment is the latest detector in…

Instrumentation and Detectors · Physics 2025-08-14 XENON Collaboration , E. Aprile , J. Aalbers , K. Abe , S. Ahmed Maouloud , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , V. C. Antochi , D. Antón Martin , F. Arneodo , M. Balata , L. Baudis , A. L. Baxter , M. Bazyk , L. Bellagamba , R. Biondi , A. Bismark , E. J. Brookes , A. Brown , S. Bruenner , G. Bruno , R. Budnik , T. K. Bui , C. Cai , J. M. R. Cardoso , F. Cassese , A. Chiarini , D. Cichon , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , R. Corrieri , J. J. Cuenca-García , J. P. Cussonneau , O. Dadoun , V. D'Andrea , M. P. Decowski , B. De Fazio , P. Di Gangi , S. Diglio , J. M. Disdier , D. Douillet , K. Eitel , A. Elykov , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , S. Form , D. Front , W. Fulgione , C. Fuselli , P. Gaemers , R. Gaior , A. Gallo Rosso , M. Galloway , F. Gao , R. Gardner , N. Garroum , R. Glade-Beucke , L. Grandi , J. Grigat , H. Guan , M. Guerzoni , M. Guida , R. Hammann , A. Higuera , C. Hils , L. Hoetzsch , N. F. Hood , J. Howlett , C. Huhmann , M. Iacovacci , G. Iaquaniello , L. Iven , Y. Itow , J. Jakob , F. Joerg , A. Joy , M. Kara , P. Kavrigin , S. Kazama , M. Kobayashi , G. Koltman , A. Kopec , F. Kuger , H. Landsman , R. F. Lang , L. Levinson , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , K. Liu , J. Loizeau , F. Lombardi , J. Long , J. A. M. Lopes , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , L. Manenti , F. Marignetti , T. Marrodán Undagoitia , P. Martella , K. Martens , J. Masbou , D. Masson , E. Masson , S. Mastroianni , E. Mele , M. Messina , R. Michinelli , K. Miuchi , A. Molinario , S. Moriyama , K. Morå , Y. Mosbacher , M. Murra , J. Müller , K. Ni , S. Nisi , U. Oberlack , D. Orlandi , R. Othegraven , B. Paetsch , J. Palacio , S. Parlati , P. Paschos , Q. Pellegrini , R. Peres , C. Peters , J. Pienaar , M. Pierre , G. Plante , T. R. Pollmann , J. Qi , J. Qin , D. Ramírez García , M. Rynge , J. Shi , R. Singh , L. Sanchez , J. M. F. dos Santos , I. Sarnoff , G. Sartorelli , J. Schreiner , D. Schulte , P. Schulte , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Shi , E. Shockley , M. Silva , H. Simgen , J. Stephen , M. Stern , B. K. Stillwell , A. Takeda , P. -L. Tan , D. Tatananni , A. Terliuk , D. Thers , F. Toschi , G. Trinchero , C. Tunnell , F. Tönnies , K. Valerius , G. Volta , C. Weinheimer , M. Weiss , D. Wenz , J. Westermann , C. Wittweg , T. Wolf , V. H. S. Wu , Y. Xing , D. Xu , Z. Xu , M. Yamashita , L. Yang , J. Ye , L. Yuan , G. Zavattini , M. Zhong , T. Zhu

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

This article reviews the application of high pressure gas xenon (HPXe) time projection chambers to neutrinoless double beta decay experiments. First, the fundamentals of the technology and the historical development of the field are…

Instrumentation and Detectors · Physics 2019-03-07 J. J. Gomez-Cadenas , F. Monrabal , P. Ferrario

Double electron capture by proton-rich nuclei is a second-order nuclear process analogous to double beta decay. Despite their similarities, the decay signature is quite different, potentially providing a new channel to measure the…

We introduce high-resolution solid-state imaging detectors for the search of neutrinoless double $\beta$ decay. Based on the present literature, imaging devices from amorphous $^{82}$Se evaporated on a complementary…

Instrumentation and Detectors · Physics 2017-03-22 A. E. Chavarria , C. Galbiati , X. Li , J. A. Rowlands

The PandaX-xT is a next-generation experiment with broad scientific goals, including the search for dark matter, Neutrinoless Double Beta Decay, and astrophysical neutrinos, using a dual-phase time projection chamber with about 43 tons of…

Instrumentation and Detectors · Physics 2026-04-09 Xu Wang , Li Zhao , Xiang Xiao , Xiangyi Cui , Shuaijie Li , Jianglai Liu

This proceedings contribution reports the first experimental search for Lorentz- and CPT-violating signals specifically studying the effect of the Standard-Model Extension (SME) oscillation-free momentum-independent neutrino coupling…

High Energy Physics - Phenomenology · Physics 2019-08-14 L. J. Kaufman

A difficult task with many particle detectors focusing on interactions below ~100 keV is to perform a calibration in the appropriate energy range that adequately probes all regions of the detector. Because detector response can vary greatly…

Instrumentation and Methods for Astrophysics · Physics 2010-07-23 A. Manalaysay , T. Marrodan Undagoitia , A. Askin , L. Baudis , A. Behrens , A. D. Ferella , A. Kish , O. Lebeda , R. Santorelli , D. Venos , A. Vollhardt

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…

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

The sensitivity for double beta decay studies of Xe-134 and Xe-124 is investigated assuming a potential large scale Xe experiment developed for dark matter searches depleted in Xe-136. The opportunity for an observation of the 2nu double…

Nuclear Experiment · Physics 2015-06-23 N. Barros , J. Thurn , K. Zuber

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

Precise measurement of two-neutrino double beta decay (DBD) half-life is an important step for the searches of Majorana neutrinos with neutrinoless double beta decay. We report the measurement of DBD half-life of $^{136}$Xe using the…

The XENON1T experiment aims for the direct detection of dark matter in a cryostat filled with 3.3 tons of liquid xenon. In order to achieve the desired sensitivity, the background induced by radioactive decays inside the detector has to be…

Instrumentation and Detectors · Physics 2017-05-09 XENON Collaboration , E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , F. D. Amaro , M. Anthony , F. Arneodo , P. Barrow , L. Baudis , B. Bauermeister , M. L. Benabderrahmane , T. Berger , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , L. Bütikofer , J. Calvén , J. M. R. Cardoso , M. Cervantes , D. Cichon , D. Coderre , A. P. Colijn , J. Conrad , J. P. Cussonneau , M. P. Decowski , P. de Perio , P. Di Gangi , A. Di Giovanni , S. Diglio , E. Duchovni , G. Eurin , J. Fei , A. D. Ferella , A. Fieguth , D. Franco , W. Fulgione , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , C. Geis , L. W. Goetzke , L. Grandi , Z. Greene , C. Grignon , C. Hasterok , E. Hogenbirk , R. Itay , B. Kaminsky , G. Kessler , A. Kish , H. Landsman , R. F. Lang , D. Lellouch , L. Levinson , M. Le Calloch , Q. Lin , S. Lindemann , M. Lindner , J. A. M. Lopes A. Manfredini , I. Maris , T. Marrodán Undagoitia , J. Masbou , F. V. Massoli , D. Masson , D. Mayani , Y. Meng , M. Messina , K. Micheneau , B. Miguez , A. Molinario , M. Murra , J. Naganoma , K. Ni , U. Oberlack , S. E. A. Orrigo , P. Pakarha , B. Pelssers , R. Persiani , F. Piastra , J. Pienaar , M. -C. Piro , V. Pizzella , G. Plante , N. Priel , L. Rauch , S. Reichard , C. Reuter , A. Rizzo , S. Rosendahl , N. Rupp , R. Saldanha , J. M. F. dos Santos , G. Sartorelli , M. Scheibelhut , S. Schindler , J. Schreiner , M. Schumann , L. Scotto Lavina , M. Selvi , P. Shagin , E. Shockley , M. Silva , H. Simgen , M. v. Sivers , A. Stein , D. Thers , A. Tiseni , G. Trinchero , C. Tunnell , N. Upole , H. Wang , Y. Wei , C. Weinheimer , J. Wulf , J. Ye , Y. Zhang , I. Cristescu

The XMASS project is designed for multiple physics goals using highly-purified liquid xenon scintillator in an ultra-low radioactivity environment. As the first stage of the project, the detector with 835 kg of liquid xenon was constructed…

Instrumentation and Detectors · Physics 2019-08-13 Katsuki Hiraide

Low-background liquid xenon detectors are utilized in the investigation of rare events, including dark matter and neutrinoless double beta decay. For their calibration, gaseous $^{220}$Rn can be used. After being introduced into the xenon,…

Instrumentation and Detectors · Physics 2023-11-15 Florian Jörg , Shengchao Li , Jochen Schreiner , Hardy Simgen , Rafael F. Lang