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Related papers: The NEXT experiment

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$^{134}$Xe is a candidate isotope for neutrinoless double beta decay~($0\nu\beta\beta$) search. In addition, the two-neutrino case ($2\nu\beta\beta$) allowed by the Standard Model of particle physics has not yet been observed. Utilizing the…

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…

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 measurement of the internal $^{222}$Rn activity in the NEXT-White detector during the so-called Run-II period with $^{136}$Xe-depleted xenon is discussed in detail, together with its implications for double beta decay searches in NEXT.…

The NEXT-White detector, a high-pressure gaseous xenon time projection chamber, demonstrated the excellence of this technology for future neutrinoless double beta decay searches using photomultiplier tubes (PMTs) to measure energy and…

High Energy Physics - Experiment · Physics 2024-08-19 T. Contreras , B. Palmeiro , H. Almazán , A. Para , G. Martínez-Lema , R. Guenette , C. Adams , V. Álvarez , B. Aparicio , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , C. D. R. Azevedo , K. Bailey , F. Ballester , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodolin , N. Byrnes , S. Cárcel , A. Castillo , S. Cebrián , E. Church , L. Cid , C. A. N. Conde , F. P. Cossío , E. Dey , G. Díaz , T. Dickel , C. Echevarria , M. Elorza , J. Escada , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , A. L. Ferreira , F. W. Foss , Z. Freixa , J. García-Barrena , J. J. Gómez-Cadenas , R. González , J. W. R. Grocott , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , B. J. P. Jones , F. Kellerer , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. P. Marques , J. Martín-Albo , M. Martínez-Vara , R. L. Miller , K. Mistry , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , P. Novella , A. Nuñez , D. R. Nygren , E. Oblak , J. Palacio , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Pérez Maneiro , M. Querol , A. B. Redwine , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , P. A. O. C. Silva , A. Simón , S. R. Soleti , M. Sorel , J. Soto-Oton , J. M. R. Teixeira , S. Teruel-Pardo , J. F. Toledo , C. Tonnelé , J. Torrent , A. Trettin , A. Usón , P. R. G. Valle , J. F. C. A. Veloso , J. Waiton , A. Yubero-Navarro

A technical description of NEXT-MM and its commissioning and first performance is reported. Having an active volume of ~35 cm drift $\times$ 28 cm diameter, it constitutes the largest Micromegas-read TPC operated in Xenon ever constructed,…

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…

We propose a novel charge sensing concept for high-pressure Time Projection Chamber (TPC) to search for Neutrinoless Double-Beta Decay (NLDBD) with ton-scale isotope mass and beyond. A meter-sized plane, tiled with an array of CMOS…

Instrumentation and Detectors · Physics 2020-10-20 Yuan Mei , Xiangming Sun , Nu Xu

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

The XENON100 dark matter experiment uses liquid xenon (LXe) in a time projection chamber (TPC) to search for Xe nuclear recoils resulting from the scattering of dark matter Weakly Interacting Massive Particles (WIMPs). In this paper we…

The feasibility of a European next-generation very massive neutrino observatory in seven potential candidate sites located at distances from CERN ranging from 130 km to 2300 km, is being considered within the LAGUNA design study. The study…

High Energy Physics - Phenomenology · Physics 2010-03-10 A. Rubbia

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

There are recent considerations to increase the photomultiplier density in the IceCube detector array beyond that of DeepCore, which will lead to a lower detection threshold and a huge fiducial mass for the neutrino detection. This…

High Energy Physics - Phenomenology · Physics 2015-05-30 Jian Tang , Walter Winter

Neutrinoless double beta decay (0nbb) is a direct probe of physics beyond the Standard Model. Its discovery would demonstrate that the lepton number is not a symmetry of nature and would provide us with unique information on the nature and…

High Energy Physics - Experiment · Physics 2019-01-09 Chiara Brofferio , Stefano Dell'Oro

A new detector is being developed at the National Superconducting Cyclotron Laboratory (NSCL) to measure low energy charged-particles from beta-delayed particle emission. These low energy particles are very important for nuclear…

Instrumentation and Detectors · Physics 2016-06-27 D. Perez-Loureiro , C. Wrede

The PandaX project consists of a series of xenon-based experiments that are used to search for dark matter (DM) particles and to study the fundamental properties of neutrinos. The next DM experiment PandaX-4T will be using 4 ton liquid…

Instrumentation and Detectors · Physics 2020-12-15 Qibin Zheng , Yanlin Huang , Di Huang , Jianglai Liu , Xiangxiang Ren , Anqing Wang , Meng Wang , Jijun Yang , Binbin Yan , Yong Yang

Motivated by the possibility of guiding daughter ions from double beta decay events to single-ion sensors for barium tagging, the NEXT collaboration is developing a program of R&D to test radio frequency (RF) carpets for ion transport in…

Noble liquid time projection chambers (TPCs) are a leading technology in the detection of ionizing radiation, particularly in applications such as accelerator neutrino physics, dark matter detection, and neutrinoless double beta decay. This…

Instrumentation and Detectors · Physics 2026-03-02 R. Saldanha , L. Pagani , E. Angelico , E. P. Bernard , B. Chana , S. Delaquis , R. DeVoe , M. Elbeltagi , S. Ferrara , D. Goeldi , R. Gornea , A. Odian , G. S. Ortega , C. T. Overman , L. Placzek , P. C. Rowson , K. Skarpaas , F. Spadoni , P. Acharya , A. Amy , A. Anker , I. J. Arnquist , A. Atencio , J. Bane , V. Belov , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , E. Brown , T. Brunner , B. Burnell , E. Caden G. F. Cao , L. Q. Cao , D. Cesmecioglu , D. Chernyak , M. Chiu , R. Collister , M. Marquis , T. Daniels , L. Darroch , M. L. di Vacri , Y. Y. Ding , M. J. Dolinski , B. Eckert , A. Emara , N. Fatemighomi , W. Fairbank , B. Foust , D. Gallacher , N. Gallice , A. Gaur , W. Gillis , F. Girard , G. Gratta , C. A. Hardy , S. Hedges , E. Hein , J. D. Holt , A. Iverson , X. S. Jiang , A. Karelin , D. Keblbeck , A. Kuchenkov , K. S. Kumar , A. Larson , M. B. Latif , S. Lavoie , K. G. Leach , B. G. Lenardo , K. K. H. Leung , H. Lewis , G. Li , X. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , J. Masbou , M. Medina-Peregrina , S. Mngonyama , B. Mong , D. C. Moore , K. Ni , I. Nitu , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , J. L. Orrell , A. Pena-Perez , H. Peltz Smalley , A. Piepke , A. Pocar , E. Raguzin , R. Rai , H. Rasiwala , D. Ray , S. Rescia , F. Retiere , G. Richardson , V. Riot , N. Rocco , R. Ross , S. Sangiorgio , S. Sekula , T. Shetty , L. Si , V. Stekhanov , X. L. Sun , S. Thibado , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , E. van Bruggen , M. Vidal , S. Viel , Q. D. Wang , M. Watts , W. Wei , M. Wehrfritz , L. J. Wen , S. Wilde , M. Worcester , X. M. Wu , H. Xu , H. B. Yang , L. Yang , M. Yu , O. Zeldovich , J. Zhao

An experimental setup is being developed to extract Ba ions from a high-pressure Xe gas environment. It aims to transport Ba ions from 10 bar Xe to vacuum conditions. The setup utilizes a converging-diverging nozzle in combination with a…

Instrumentation and Detectors · Physics 2019-08-13 T. Brunner , D. Fudenberg , A. Sabourov , V. L. Varentsov , G. Gratta , D. Sinclair

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