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The gaseous Xenon(Xe) time projection chamber (TPC) is an attractive detector technique for neutrinoless double beta decay and WIMP dark matter searches. While it is less dense compared to Liquid Xe detectors, it has intrinsic advantages in…

Instrumentation and Detectors · Physics 2016-04-13 Y. Nakajima , A. Goldshmidt , H. S. Matis , T. Miller , D. R. Nygren , C. A. B. Oliveira , J. Renner

A high-flow radon removal system based on cryogenic distillation was developed and constructed to reduce radon-induced backgrounds in liquid xenon detectors for rare event searches such as XENONnT. A continuous purification of the XENONnT…

Instrumentation and Detectors · Physics 2022-12-28 M. Murra , D. Schulte , C. Huhmann , C. Weinheimer

The XENON experiment is looking for non-baryonic particle dark matter in the universe. The setup is a dual phase time projection chamber (TPC) filled with 3200 kg of ultra-pure liquid xenon. The setup is operated at the Laboratori Nazionali…

Distributed, Parallel, and Cluster Computing · Computer Science 2019-09-19 Daniel Ahlin , Boris Bauermeister , Jan Conrad , Robert Gardner , Luca Grandi , Benedikt Riedel , Evan Shockley , Judith Stephen , Ragnar Sundblad , Suchandra Thapa , Christopher Tunnell

Dual-phase xenon detectors are widely used in dark matter direct detection experiments, and have demonstrated the highest sensitivities to a variety of dark matter interactions. However, a key component of the dual-phase detector…

Instrumentation and Detectors · Physics 2019-06-05 Jingke Xu , Sergey Pereverzev , Brian Lenardo , James Kingston , Daniel Naim , Adam Bernstein , Kareem Kazkaz , Mani Tripathi

We report the first precision measurement of the superheat temperature required for bubble nucleation in liquid xenon of $\Delta T_{wall,ONB}$ = (16.9$\pm$0.5) K and $\Delta T_{wall,ONB}$ = (19.2$^{+0.4}_{-1.1}$) K at pressures of P =…

Instrumentation and Detectors · Physics 2021-03-24 P. A. Breur , G. S. Ortega , P. C. Rowson , R. Saldanha , B. Mong , M. Oriunno , C. Mo

PandaX is a large upgradable liquid-xenon detector system that can be used for both direct dark-matter detection and $^{136}$Xe double-beta decay search. It is located in the Jinping Deep-Underground Laboratory in Sichuan, China. The…

nEXO is a proposed tonne-scale neutrinoless double beta decay ($0\nu\beta\beta$) experiment using liquid ${}^{136}Xe$ (LXe) in a Time Projection Chamber (TPC) to read out ionization and scintillation signals. Between the field cage and the…

Instrumentation and Detectors · Physics 2021-04-07 T. Stiegler , S. Sangiorgio , J. P. Brodsky , M. Heffner , S. Al Kharusi , G. Anton , I. J. Arnquist , I. Badhrees , P. S. Barbeau , D. Beck , V. Belov , T. Bhatta , A. Bolotnikov , P. A. Breur , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Cao , C. Chambers , B. Chana , S. A. Charlebois , M. Chiu , B. Cleveland , M. Coon , A. Craycraft , J. Dalmasson , T. Daniels , L. Darroch , A. De St. Croix , A. Der Mesrobian-Kabakian , K. Deslandes , R. DeVoe , M. L. Di Vacri , J. Dilling , Y. Y. Ding , M. J. Dolinski , A. Dragone , J. Echevers , F. Edaltafar , M. Elbeltagi , L. Fabris , D. Fairbank , W. Fairbank , J. Farine , S. Ferrara , S. Feyzbakhsh , G. Gallina , P. Gautam , G. Giacomini , D. Goeldi , R. Gornea , G. Gratta , E. V. Hansen , E. W. Hoppe , J. Hößl , A. House , M. Hughes , A. Iverson , A. Jamil , M. J. Jewell , X. S. Jiang , A. Karelin , L. J. Kaufman , T. Koffas , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , A. Larson , K. G. Leach , B. G. Lenardo , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , P. Lv , R. MacLellan , N. Massacret , T. McElroy , M. Medina-Peregrina , T. Michel , B. Mong , D. C. Moore , K. Murray , P. Nakarmi , C. R. Natzke , R. J. Newby , K. Ni , Z. Ning , O. Njoya , F. Nolet , O. Nusair , K. Odgers , A. Odian , M. Oriunno , J. L. Orrell , G. S. Ortega , I. Ostrovskiy , C. T. Overman , S. Parent , A. Piepke , A. Pocar , J. -F. Pratte , V. Radeka , E. Raguzin , S. Rescia , F. Retière , M. Richman , A. Robinson , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , K. Skarpaas VIII , A. K. Soma , G. St-Hilaire , V. Stekhanov , X. L. Sun , M. Tarka , S. Thibado , A. Tidball , J. Todd , T. I. Totev , R. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , S. Viel , G. Visser , C. Vivo-Vilches , J. -L. Vuilleumier , M. Wagenpfeil , T. Wager , M. Walent , Q. Wang , W. Wei , L. J. Wen , U. Wichoski , M. Worcester , S. X. Wu , W. H. Wu , X. Wu , Q. Xia , H. Yang , L. Yang , O. Zeldovich , J. Zhao , Y. Zhou , T. Ziegler

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

Panda-X is a liquid xenon dual-phase detector for the Dark Matter Search. The first modestly-sized module will soon be installed in the China JinPing Deep Underground Laboratory in Sichuan province, P.R. China. The cryogenics system is…

Instrumentation and Methods for Astrophysics · Physics 2015-06-05 Zhao Li , Karl Ludwig Giboni , Haowei Gong , Xiangdong Ji , Andy Tan

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 Xenon nuclei. With a fiducial mass of 1000 kg of liquid xenon, a sufficiently low…

Astrophysics · Physics 2007-05-23 XENON Collaboration , Elena Aprile

Scintillation light produced in liquid xenon (LXe) by alpha particles, electrons and gamma-rays was detected with a large area avalanche photodiode (LAAPD) immersed in the liquid. The alpha scintillation yield was measured as a function of…

Instrumentation and Detectors · Physics 2009-11-11 K. Ni , E. Aprile , D. Day , K. L. Giboni , J. A. M. Lopes , P. Majewski , M. Yamashita

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

The nEXO neutrinoless double beta decay experiment is designed to use a time projection chamber and 5000 kg of isotopically enriched liquid xenon to search for the decay in $^{136}$Xe. Progress in the detector design, paired with higher…

Nuclear Experiment · Physics 2022-02-24 nEXO Collaboration , G. Adhikari , S. Al Kharusi , E. Angelico , G. Anton , I. J. Arnquist , I. Badhrees , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , A. Bolotnikov , P. A. Breur , J. P. Brodsky , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Cao , C. Chambers , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , B. Cleveland , R. Collister , S. A. Czyz , J. Dalmasson , T. Daniels , L. Darroch , R. DeVoe , M. L. Di Vacri , J. Dilling , Y. Y. Ding , A. Dolgolenko , M. J. Dolinski , A. Dragone , J. Echevers , M. Elbeltagi , L. Fabris , D. Fairbank , W. Fairbank , J. Farine , S. Ferrara , S. Feyzbakhsh , Y. S. Fu , G. Gallina , P. Gautam , G. Giacomini , W. Gillis C. Gingras , D. Goeldi , R. Gornea , G. Gratta , C. A. Hardy , K. Harouaka , M. Heffner , E. W. Hoppe , A. House , A. Iverson , A. Jamil , M. Jewell , X. S. Jiang , A. Karelin , L. J. Kaufman , I. Kotov , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , A. Larson , K. G. Leach , B. G. Lenardo , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , M. Mahtab , P. Martel-Dion , J. Masbou , N. Massacret , T. McElroy , K. McMichael , M. Medina Peregrina , T. Michel , B. Mong , D. C. Moore , K. Murray , J. Nattress , C. R. Natzke , R. J. Newby , K. Ni , F. Nolet , O. Nusair , J. C. Nzobadila Ondze , K. Odgers , A. Odian , J. L. Orrell , G. S. Ortega , C. T. Overman , S. Parent , A. Perna , A. Piepke , A. Pocar , J-F. Pratte , N. Priel , V. Radeka , E. Raguzin , G. J. Ramonnye , T. Rao , H. Rasiwala , S. Rescia , F. Retière , J. Ringuette , V. Riot , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , S. Sangiorgio , X. Shang , A. K. Soma , F. Spadoni , V. Stekhanov , X. L. Sun , M. Tarka , S. Thibado , A. Tidball , J. Todd , T. Totev , S. Triambak , R. H. M. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , S. Viel , C. Vivo-Vilches , P. Vogel , J-L. Vuilleumier , M. Wagenpfeil , T. Wager , M. Walent , K. Wamba , Q. Wang , W. Wei , L. J. Wen , U. Wichoski , S. Wilde , M. Worcester , S. X. Wu , W. H. Wu , X. Wu , Q. Xia , W. Yan , H. Yang , L. Yang , O. Zeldovich , J. Zhao , T. Ziegler

We have studied the feasibility of a silicon photomultiplier (SiPM) to detect liquid xenon (LXe) scintillation light. The SiPM was operated inside a small volume of pure LXe, at -95 degree Celsius, irradiated with an internal Am-241 alpha…

Instrumentation and Detectors · Physics 2009-11-11 E. Aprile , P. Cushman , K. Ni , P. Shagin

Dual phase Xenon Time Projection Chambers (XeTPCs) are being used by several experiments as a promising technique for direct detection of dark matter. We report on the design and performance of a small 3-D sensitive dual phase XeTPC. The…

Instrumentation and Detectors · Physics 2015-06-17 Qing Lin , Yuehuan Wei , Jie Bao , Jie Hu , Xinran Li , Wolfgang Lorenzon , Kaixuan Ni , Michael Schubnell , Mengjiao Xiao , Xiang Xiao

Bubble formation in liquid xenon underneath a Thick Gaseous Electron Multiplier (THGEM) electrode immersed in liquid xenon was observed with a CCD camera. With voltage across the THGEM, the appearance of bubbles was correlated with that of…

Instrumentation and Detectors · Physics 2015-09-09 E. Erdal , L. Arazi , V. Chepel , M. L. Rappaport , D. Vartsky , A. Breskin

The next-generation Enriched Xenon Observatory (nEXO) is a proposed experiment to search for neutrinoless double beta ($0\nu\beta\beta$) decay in $^{136}$Xe with a target half-life sensitivity of approximately $10^{28}$ years using…

Nuclear Experiment · Physics 2018-10-23 nEXO Collaboration , J. B. Albert , G. Anton , I. J. Arnquist , I. Badhrees , P. S. Barbeau , D. Beck , V. Belov , F. Bourque , J. P. Brodsky , E. Brown , T. Brunner , A. Burenkov , G. F. Cao , L. Cao , W. R. Cen , C. Chambers , S. A. Charlebois , M. Chiu , B. Cleveland , M. Coon , M. Côté , A. Craycraft , W. Cree , J. Dalmasson , T. Daniels , S. J. Daugherty , J. Daughhetee , R. DeVoe , S. Delaquis , A. Der Mesrobian-Kabakian , T. Didberidze , J. Dilling , Y. Y. Ding , M. J. Dolinski , A. Dragone , L. Fabris , W. Fairbank , J. Farine , S. Feyzbakhsh , R. Fontaine , D. Fudenberg , G. Giacomini , R. Gornea , K. Graham , G. Gratta , E. V. Hansen , D. Harris , M. Hasan , M. Heffner , E. W. Hoppe , J. Hößl , A. House , P. Hufschmidt , M. Hughes , Y. Ito , A. Iverson , A. Jamil , M. J. Jewell , X. S. Jiang , T. N. Johnson , S. Johnston , A. Karelin , L. J. Kaufman , R. Killick , T. Koffas , S. Kravitz , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , Y. H. Lin , R. MacLellan , T. Michel , B. Mong , D. C. Moore , K. Murray , R. J. Newby , Z. Ning , O. Njoya , F. Nolet , K. Odgers , A. Odian , M. Oriunno , J. L. Orrell , G. S. Ortega , I. Ostrovskiy , C. T. Overman , S. Parent , A. Piepke , A. Pocar , J. -F. Pratte , D. Qiu , V. Radeka , E. Raguzin , T. Rao , S. Rescia , F. Retière , A. Robinson , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , S. Sangiorgio , S. Schmidt , J. Schneider , A. Schubert , D. Sinclair , K. Skarpaas VIII , 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 , P. Vogel , J. -L. Vuilleumier , M. Wagenpfeil , Q. Wang , M. Weber , W. Wei , L. J. Wen , U. Wichoski , G. Wrede , S. X. Wu , W. H. Wu , L. Yang , Y. -R. Yen , O. Zeldovich , J. Zettlemoyer , X. Zhang , J. Zhao , Y. Zhou , T. Ziegler