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NEXT-100 is an electroluminescent high pressure Time Projection Chamber currently under construction. It will search for the neutrino-less double beta decay in 136Xe at the Canfranc Underground Laboratory. NEXT-100 aims to achieve nearly…

Instrumentation and Detectors · Physics 2019-08-16 C. A. B. Oliveira

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

Xenon dual-phase time projection chambers designed to search for Weakly Interacting Massive Particles have so far shown a relative energy resolution which degrades with energy above $\sim$200 keV due to the saturation effects. This has…

Instrumentation and Detectors · Physics 2020-09-10 E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , L. Althueser , F. D. Amaro , V. C. Antochi , E. Angelino , J. Angevaare , F. Arneodo , D. Barge , L. Baudis , B. Bauermeister , L. Bellagamba , M. L. Benabderrahmane , T. Berger , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , D. Cichon , B. Cimmino , M. Clark , D. Coderre , A. P. Colijn , J. Conrad , J. P. Cussonneau , M. P. Decowski , A. Depoian P. Di Gangi A. Di Giovanni R. Di Stefano , S. Diglio , A. Elykov , G. Eurin , A. D. Ferella , W. Fulgione , P. Gaemers , R. Gaior , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , L. Grandi , C. Hasterok , C. Hils , K. Hiraide , L. Hoetzsch , E. Hogenbirk , J. Howlett , M. Iacovacci , Y. Itow , F. Joerg , N. Kato , S. Kazama , M. Kobayashi , G. Koltman , A. Kopec , H. Landsman , R. F. Lang , L. Levinson , Q. Lin , S. Lindemann , M. Lindner , F. Lombardi , J. A. M. Lopes , E. López Fune , C. Macolino , J. Mahlstedt , L. Manenti , A. Manfredini , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , D. Masson , S. Mastroianni , M. Messina , K. Miuchi , A. Molinario , K. Morå , S. Moriyama , Y. Mosbacher , M. Murra , J. Naganoma , K. Ni , U. Oberlack , K. Odgers , J. Palacio , B. Pelssers , R. Peres , J. Pienaar , V. Pizzella , G. Plante J. Qin , H. Qiu , D. Ramírez García , S. Reichard , A. Rocchetti , N. Rupp , J. M. F. dos Santos , G. Sartorelli , N. Šarčević , M. Scheibelhut , S. Schindler , J. Schreiner , D. Schulte , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , E. Shockley , M. Silva , H. Simgen , A. Takeda , C. Therreau , D. Thers , F. Toschi , G. Trinchero , C. Tunnell , M. Vargas , G. Volta , O. Wack , H. Wang , Y. Wei , C. Weinheimer , M. Weiss Xu , D. Wenz , C. Wittweg , J. Wulf , Z. Xu , M. Yamashita , J. Ye , G. Zavattini , Y. Zhang , T. Zhu , J. P. Zopounidis

Possibility to use ultra pure liquid Xenon as a low energy solar neutrino detector by means of $\nu$+e scatterings is evaluated. A possible detector with 10 tons of fiducial volume will give $\sim$14 events for pp-neutrinos and $\sim$6…

High Energy Physics - Phenomenology · Physics 2017-08-23 Y. Suzuki

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

nEXO is a proposed next-generation experiment searching for the neutrinoless double beta decay of $^{136}$Xe using a tonne-scale liquid xenon (LXe) time projection chamber (TPC). To image the ionization signals from events in the liquid…

Instrumentation and Detectors · Physics 2025-12-15 Z. Li , M. Yu , E. Angelico , A. Atencio , A. Gupta , P. Knauss , A. Pena-Perez , B. G. Lenardo , P. Acharya , A. Amy , A. Anker , I. J. Arnquist , J. Bane , V. Belov , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , J. P. Brodsky , 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 , R. DeVoe , M. L. di Vacri , X. Defay , Y. Y. Ding , D. Doering , M. J. Dolinski , A. Dragone , B. Eckert , A. Emara , N. Fatemighomi , W. Fairbank , B. T. Foust , D. Gallacher , N. Gallice , A. Gaur , W. Gillis , F. Girard , A. Gorham , K. Gracequist , G. Gratta , C. A. Hardy , J. Hasi , S. Hedges , M. Heffner , E. Hein , H. Hernandez Herrera , J. D. Holt , A. Iverson , X. S. Jiang , A. Karelin , D. Keblbeck , C. Kenney , I. Kotov , A. Kuchenkov , K. S. Kumar , S. Lavoie , A. Larson , M. B. Latif , K. G. Leach , D. S. Leonard , G. Lessard , K. K. H. Leung , G. Li , X. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , B. Markovic , 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 , A. Odian , J. L. Orrell , G. S. Ortega , L. Pagani , H. Peltz Smalley , A. Piepke , A. Pocar , S. Prentice , V. Radeka , E. Raguzin , R. Rai , H. Rasiwala , D. Ray , B. Reese , S. Rescia , F. Retiere , G. Richardson , V. Riot , R. Ross , L. Rota , P. C. Rowson , R. Saldanha , S. Sangiorgio , S. Sekula , T. Shetty , L. Si , F. Spadoni , V. Stekhanov , X. L. Sun , S. Thibado , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , T. Vallivilayil John , E. van Bruggen , M. Vidal , S. Viel , M. Walent , H. Wang , Q. D. Wang , M. Watts , W. Wei , M. Wehrfritz , L. J. Wen , S. Wilde , X. M. Wu , H. Xu , H. B. Yang , L. Yang , O. Zeldovich , J. Zhao

We investigate the detection prospects for two-neutrino and neutrinoless second order weak decays of $^{124}$Xe -- double electron capture ($0/2\nu\text{ECEC}$), electron capture with positron emission ($0/2\nu\text{EC}\beta^+$) and…

Nuclear Experiment · Physics 2020-12-30 Christian Wittweg , Brian Lenardo , Alexander Fieguth , Christian Weinheimer

A high pressure xenon gas time projection chamber with electroluminescent amplification (EL HPGXe TPC) searching for the neutrinoless double beta ($0\nu\beta\beta$) decay offers: excellent energy resolution ($0.5-0.7\%$ FWHM at the…

Instrumentation and Detectors · Physics 2017-10-11 N. Lopez-March

Tagging barium ions in double beta decay experiments involving $^{136}$Xe offers a promising pathway to achieving an almost background-free environment, which is essential for addressing key unresolved questions in neutrino physics, such as…

Atomic Physics · Physics 2025-01-16 Álvaro Peralta Conde

Several efforts are ongoing for the development of spherical gaseous time projection chamber detectors for the observation of rare phenomena such as weakly interacting massive particles or neutrino interactions. The proposed detector,…

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

This article reviews the progress made over the last 20 years in the development and applications of liquid xenon detectors in particle physics, astrophysics and medical imaging experiments. We begin with a summary of the fundamental…

Instrumentation and Detectors · Physics 2010-12-01 E. Aprile , T. Doke

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

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

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

The next-generation of $0\nu\beta\beta$ searches are targeting half-life sensitivities towards 10$^{27}$--10$^{28}$ years. Gaseous xenon time projection chamber (GXeTPC) detectors may be able to meet this challenge due to their excellent…

Instrumentation and Detectors · Physics 2026-03-19 K. Mistry , Y. Mei , D. R. Nygren

$^{134}$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…

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

A search for instability of nucleons bound in $^{136}$Xe nuclei is reported with 223 kg$\cdot$yr exposure of $^{136}$Xe in the EXO-200 experiment. Lifetime limits of 3.3$\times 10^{23}$ and 1.9$\times 10^{23}$ yrs are established for…