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The Enriched Xenon Observatory (EXO) will search for double beta decays of 136Xe. We report the results of a systematic study of trace concentrations of radioactive impurities in a wide range of raw materials and finished parts considered…

The neutralization of slow positive ions on solid surfaces can lead to the emission of secondary electrons in Auger-type processes. We discuss the possibility of harnessing such mechanisms to the detection of positive ions in gaseous TPCs.…

Instrumentation and Detectors · Physics 2018-07-04 Lior Arazi

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

The NEMO experiment is investigating the neutrinoless double beta decay. The NEMO-3 detector is taking data in the Frejus Underground Laboratory. The goal of the SuperNEMO detector is to reach a sensitivity on the order of 10^26 year on the…

High Energy Physics - Experiment · Physics 2008-10-06 Laurent Simard

The search for neutrinoless double-beta decay (0{\nu}{\beta}{\beta}) requires extremely low background and a good understanding of their sources and their influence on the rate in the region of parameter space relevant to the…

The liquid xenon (LXe) time projection chamber (TPC) technology is probing a wide range of dark matter masses from sub-GeV to a few TeV. To further improve its sensitivity to sub-GeV dark matter and its application in reactor neutrino…

Instrumentation and Detectors · Physics 2021-01-22 Yuehuan Wei , Jianyu Long , Francesco Lombardi , Zhiheng Jiang , Jingqiang Ye , Kaixuan Ni

The SuperNEMO project aims to search for neutrinoless double beta decay ($0\nu\beta\beta$) up to a sensitivity of 10$^{26}$ years for the $0\nu\beta\beta$ half-life (down to 50 meV in the effective Majorana neutrino mass), using $\sim$100…

Nuclear Experiment · Physics 2008-07-22 Yu. Shitov

Liquid xenon time projection chambers are promising detectors to search for neutrinoless double beta decay (0$\nu \beta \beta$), due to their response uniformity, monolithic sensitive volume, scalability to large target masses, and…

Instrumentation and Detectors · Physics 2022-12-28 G. Gallina , Y. Guan , F. Retiere , G. Cao , A. Bolotnikov , I. Kotov , S. Rescia , A. K. Soma , T. Tsang , L. Darroch , T. Brunner , J. Bolster , J. R. Cohen , T. Pinto Franco , W. C. Gillis , H. Peltz Smalley , S. Thibado , A. Pocar , A. Bhat , A. Jamil , D. C. Moore , G. Adhikari , S. Al Kharusi , E. Angelico , I. J. Arnquist , P. Arsenault , I. Badhrees , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , J. P. Brodsky , E. Brown , E. Caden , L. Cao , C. Chambers , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , B. Cleveland , R. Collister , M. Cvitan , J. Dalmasson , T. Daniels , K. Deslandes , R. DeVoe , M. L. di Vacri , Y. Ding , M. J. Dolinski , A. Dragone , J. Echevers , B. Eckert , M. Elbeltagi , L. Fabris , W. Fairbank , J. Farine , Y. S. Fu , D. Gallacher , P. Gautam , G. Giacomini , C. Gingras , D. Goeldi , R. Gornea , G. Gratta , C. A. Hardy , S. Hedges , M. Heffner , E. Hein , J. Holt , E. W. Hoppe , J. Hößl , A. House , W. Hunt , A. Iverson , X. S. Jiang , A. Karelin , L. J. Kaufman , R. Krücken , A. Kuchenkov , K. S. Kumar , A. Larson , K. G. Leach , B. G. Lenardo , D. S. Leonard , G. Lessard , G. Li , S. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , M. Mahtab , S. Majidi , C. Malbrunot , P. Margetak , P. Martel-Dion , L. Martin , J. Masbou , N. Massacret , K. McMichael , B. Mong , K. Murray , J. Nattress , C. R. Natzke , X. E. Ngwadla , J. C. Nzobadila Ondze , A. Odian , J. L. Orrell , G. S. Ortega , C. T. Overman , S. Parent , A. Perna , A. Piepke , N. Pletskova , J. F. Pratte , V. Radeka , E. Raguzin , G. J. Ramonnye , T. Rao , H. Rasiwala , K. Raymond , B. M. Rebeiro , G. Richardson , J. Ringuette , V. Riot , T. Rossignol , P. C. Rowson , L. Rudolph , R. Saldanha , S. Sangiorgio , X. Shang , F. Spadoni , V. Stekhanov , X. L. Sun , A. Tidball , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , F. Vachon , M. Vidal , S. Viel , G. Visser , M. Wagenpfeil , M. Walent , K. Wamba , Q. Wang , W. Wang , Y. Wang , M. Watts , W. Wei , L. J. Wen , U. Wichoski , S. Wilde , M. Worcester , W. H. Wu , X. Wu , L. Xie , W. Yan , H. Yang , L. Yang , O. Zeldovich , J. Zhao , T. Ziegler

The XENONnT experiment, located at the INFN Laboratori Nazionali del Gran Sasso, Italy, features a 5.9 tonne liquid xenon time projection chamber surrounded by an instrumented neutron veto, all of which is housed within a muon veto water…

High Energy Physics - Experiment · Physics 2024-09-16 XENON Collaboration , E. Aprile , J. Aalbers , K. Abe , S. Ahmed Maouloud , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , D. Antón Martin , F. Arneodo , L. Baudis , M. Bazyk , L. Bellagamba , R. Biondi , A. Bismark , K. Boese , A. Brown , G. Bruno , R. Budnik , J. M. R. Cardoso , A. P. Cimental Chávez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , L. C. Daniel Garcia , M. P. Decowski , A. Deisting , C. Di Donato , P. Di Gangi , S. Diglio , K. Eitel , A. Elykov , A. D. Ferella , C. Ferrari , H. Fischer , T. Flehmke , M. Flierman , W. Fulgione , C. Fuselli , P. Gaemers , R. Gaior , M. Galloway , F. Gao , S. Ghosh , R. Giacomobono , R. Glade-Beucke , L. Grandi , J. Grigat , H. Guan , M. Guida , P. Gyoergy , R. Hammann , A. Higuera , C. Hils , L. Hoetzsch , N. F. Hood , M. Iacovacci , Y. Itow , J. Jakob , F. Joerg , Y. Kaminaga , M. Kara , P. Kavrigin , S. Kazama , M. Kobayashi , D. Koke , A. Kopec , F. Kuger , H. Landsman , R. F. Lang , L. Levinson , I. Li , S. Li , S. Liang , Y. -T. Lin , S. Lindemann , M. Lindner , K. Liu , J. Loizeau , F. Lombardi , J. Long , J. A. M. Lopes , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , L. Manenti , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , E. Masson , S. Mastroianni , A. Melchiorre , J. Merz , M. Messina , A. Michael , K. Miuchi , A. Molinario , S. Moriyama , K. Morå , Y. Mosbacher , M. Murra , J. Müller , K. Ni , U. Oberlack , B. Paetsch , Y. Pan , Q. Pellegrini , R. Peres , C. Peters , J. Pienaar , M. Pierre , G. Plante , T. R. Pollmann , L. Principe , J. Qi , J. Qin , D. Ramírez García , M. Rajado , 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 , J. Shi , M. Silva , H. Simgen , A. Takeda , P. -L. Tan , A. Terliuk , D. Thers , F. Toschi , G. Trinchero , C. D. Tunnell , F. Tönnies , K. Valerius , S. Vecchi , S. Vetter , F. I. Villazon Solar , G. Volta , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , V. H. S. Wu , Y. Xing , D. Xu , Z. Xu , M. Yamashita , L. Yang , J. Ye , L. Yuan , G. Zavattini , M. Zhong

The idea of a hermetic quartz chamber in a dual-phase xenon time projection chamber (TPC) has the potential to improve the detector sensitivity for direct dark matter searches in the future. A major challenge facing TPC detectors in future…

The NEXT-White (NEW) detector is currently the largest radio-pure high-pressure xenon gas time projection chamber with electroluminescent readout in the world. NEXT-White has been operating at Laboratorio Subterr\'aneo de Canfranc (LSC)…

Dual-phase time projection chambers (TPCs) filled with the liquid noble gas xenon (LXe) are currently the most sensitive detectors searching for interactions of WIMP dark matter in a laboratory-based experiment. This is achieved by…

Instrumentation and Methods for Astrophysics · Physics 2014-08-08 Marc Schumann

The experimental rate of neutrinoless double beta decay can be saturated by the exchange of virtual sterile neutrinos, that mix with the ordinary neutrinos and are heavier than 200 MeV. Interestingly, this hypothesis is subject only to…

High Energy Physics - Phenomenology · Physics 2015-05-30 Manimala Mitra , Goran Senjanovic , Francesco Vissani

Liquid xenon time projection chambers offer a homogeneous detection medium with excellent intrinsic energy resolution, fast scintillation, and true three-dimensional position sensitivity, making them an attractive alternative to…

Instrumentation and Detectors · Physics 2026-03-30 B. Li , Y. Ma , K. Ni

Various large-scale experiments for double beta decay or dark matter are based on xenon. Current experiments are on the tonne scale but there are also ideas to aim for even larger sizes in the future. Here we study the potential of the…

Nuclear Theory · Physics 2020-09-03 J. Kostensalo , J. Suhonen , K. Zuber

A search for neutrinoless double-beta decay ($0\nu\beta\beta$) in $^{136}$Xe is performed with the full EXO-200 dataset using a deep neural network to discriminate between $0\nu\beta\beta$ and background events. Relative to previous…

Compelling experimental evidences of neutrino oscillations and their implication that neutrinos are massive particles have given neutrinoless double beta decay a central role in astroparticle physics. In fact, the discovery of this elusive…

Instrumentation and Detectors · Physics 2015-06-22 Valter Bonvicini , Silvia Capelli , Oliviero Cremonesi , Giacomo Cucciati , Luca Gironi , Maura Pavan , Ezio Previtali , Monica Sisti

Double beta plus decay is a rare nuclear disintegration process. Difficulties in its measurement arise from suppressed decay probabilities, experimentally challenging decay signatures and low natural abundances of suitable candidate nuclei.…

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