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Related papers: Status and Prospects of the PandaX-III Experiment

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The PandaX-III experiment uses a high pressure xenon gas TPC to search for the NLDBD of $^{136}$Xe. The Microbulk Micromegas will be used for charge amplification and readout in order to record both the energy and track of an event with…

Instrumentation and Detectors · Physics 2020-06-17 Shaobo Wang

The search for the neutrinoless double beta decay (0$\nu\beta\beta$) is one of the most important quests nowadays in neutrino physics. Among the different techniques used, high pressure xenon (HPXe) gas time projection chambers (TPC) stand…

Instrumentation and Detectors · Physics 2016-05-25 J. Galan

In the search for the neutrinoless double beta decay of $^{136}$Xe, a high pressure xenon time projection chamber (HPXe-TPC) has two advantages over liquid xenon TPCs: a better energy resolution and the access to topological features, which…

Instrumentation and Detectors · Physics 2017-10-11 F. J. Iguaz , F. Aznar , J. F. Castel , S. Cebrian , T. Dafni , J. Galan , J. G. Garza , I. G. Irastorza , G. Luzon , H. Mirallas , E. Ruiz-Choliz

The PandaX-III (Particle And Astrophysical Xenon Experiment III) experiment will search for Neutrinoless Double Beta Decay (NLDBD) of 136Xe at the China Jin-Ping underground Laboratory II (CJPL-II). In the first phase of the experiment, a…

Instrumentation and Detectors · Physics 2019-08-14 Ke Han

The Particle And Astrophysical Xenon Experiment III (PandaX-III) is an experiment to search for the Neutrinoless Double Beta Decay (NLDBD) using 200 kg radio-pure high-pressure gaseous xenon TPC with Micromegas detectors at both ends and…

Instrumentation and Detectors · Physics 2019-09-04 Danyang Zhu , Shubin Liu , Changqing Feng , Cheng Li , Haolei Chen

The PandaX-III experiment plans to search for neutrinoless double beta decay (0$\nu\beta\beta$) of $^{136}$Xe in the China JinPing underground Laboratory (CJPL). The experiment will use a high pressure gaseous Time Projection Chamber (TPC)…

A high-pressure xenon gas time projection chamber, with a unique cellular readout structure based on electroluminescence, has been developed for a large-scale neutrinoless double-beta decay search. In order to evaluate the detector…

The PandaX-III experiment will search for neutrinoless double beta decay of $^{136}$Xe with high pressure gaseous time projection chambers at the China Jin-Ping underground Laboratory. The tracking feature of gaseous detectors helps…

Instrumentation and Detectors · Physics 2018-08-14 Hao Qiao , Chunyu Lu , Xun Chen , Ke Han , Xiangdong Ji , Siguang Wang

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

High pressure gas detectors offer advantages for the detection of rare events, where background reduction is crucial. For the neutrinoless double beta decay of 136Xe a high pressure xenon gas Time Projection Chamber (TPC) combines a good…

Instrumentation and Detectors · Physics 2015-06-16 S Cebrian , T Dafni , H Gomez , D C Herrera , F J Iguaz , I G Irastorza , G Luzon , L Segui , A Tomas

As part of the T-REX project, a number of R&D and prototyping activities have been carried out during the last years to explore the applicability of gaseous Micromegas-read TPCs in rare event searches like double beta decay (DBD), axion…

The use of Time Projection Chambers (TPCs) in particle physics experiments has been growing since their invention, reaching sizes equivalent to buildings (ALICE or ATLAS at CERN). However, their application in another class of experiments,…

Instrumentation and Detectors · Physics 2024-12-24 Hector Mirallas

nEXO is a proposed experiment to search for the neutrino-less double beta decay ($0\nu\beta\beta$) of $^{136}$Xe in a tonne-scale liquid xenon time projection chamber (TPC). The nEXO TPC will be equipped with charge collection tiles to form…

Instrumentation and Detectors · Physics 2019-10-21 Z. Li , W. R. Cen , A. Robinson , D. C. Moore , L. J. Wen , A. Odian , S. Al Kharusi , G. Anton , I. J. Arnquist , I. Badhrees , P. S. Barbeau , D. Beck , V. Belov , T. Bhatta , J. P. Brodsky , 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 , S. J. Daugherty , A. De St. Croix , A. Der Mesrobian-Kabakian , R. DeVoe , M. L. Di Vacri , J. Dilling , Y. Y. Ding , M. J. Dolinski , A. Dragone , J. Echevers , M. Elbeltagi , L. Fabris , D. Fairbank , W. Fairbank , J. Farine , S. Ferrara , S. Feyzbakhsh , R. Fontaine , A. Fucarino , G. Gallina , P. Gautam , G. Giacomini , D. Goeldi , R. Gornea , G. Gratta , E. V. Hansen , M. Heffner , E. W. Hoppe , J. Hößl , A. House , M. Hughes , A. Iverson , A. Jamil , M. J. Jewell , X. S. Jiang , A. Karelin , L. J. Kaufman , D. Kodroff , 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 , C. Licciardi , Y. H. Lin , P. Lv , R. MacLellan , T. McElroy , M. Medina-Peregrina , T. Michel , B. Mong , K. Murray , P. Nakarmi , C. R. Natzke , R. J. Newby , Z. Ning , O. Njoya , F. Nolet , O. Nusair , K. Odgers , 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 , T. Rossignol , P. C. Rowson , N. Roy , J. Runge , R. Saldanha , S. Sangiorgio , K. Skarpaas VIII , A. K. Soma , G. St-Hilaire , V. Stekhanov , T. Stiegler , X. L. Sun , M. Tarka , J. Todd , T. Tolba , T. I. Totev , R. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , S. Viel , G. Visser , C. Vivo-Vilches , J. -L. Vuilleumier , M. Wagenpfeil , M. Walent , Q. Wang , M. Ward , J. Watkins , M. Weber , W. Wei , U. Wichoski , S. X. Wu , W. H. Wu , X. Wu , Q. Xia , H. Yang , L. Yang , Y. -R. Yen , O. Zeldovich , J. Zhao , Y. Zhou , T. Ziegler

We have been developing a high-pressure xenon gas time projection chamber (TPC) to search for neutrinoless double beta ($0\nu\beta\beta$) decay of $^{136}$Xe. The unique feature of this TPC is in the detection part of ionization electrons,…

NEXT (Neutrino Experiment with a Xenon TPC) aims to observe the neutrinoless double beta decay of \ensuremath{{}^{136}\rm Xe} in a high-pressure gas xenon Time Projection Chamber using electroluminescence to amplify the signal from…

Instrumentation and Detectors · Physics 2019-08-14 Paola Ferrario

NEXT (Neutrino Experiment with a Xenon TPC) is an experimental program whose goals are to discover neutrinoless double beta decay using $^{136}$Xe in high pressure xenon TPCs with electroluminescent readout. In this paper, results from the…

High Energy Physics - Experiment · Physics 2019-06-06 J. J. Gomez-Cadenas

Neutrinoless double beta decay is a hypothetical, very slow nuclear transition in which two neutrons undergo beta decay simultaneously and without the emission of neutrinos. The importance of this process goes beyond its intrinsic interest:…

Instrumentation and Detectors · Physics 2019-08-13 D. Lorca , J. Martín-Albo , F. Monrabal

In this paper we describe an innovative type of Time Projection Chamber (TPC), which uses high-pressure xenon gas (HPXe) and electroluminescence amplification of the ionization charge as the basis of an apparatus capable of fully…

Instrumentation and Detectors · Physics 2019-08-13 J. J. Gómez-Cadenas , J. Martín-Albo , F. Monrabal
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