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We present a novel constraint on light dark matter utilizing $1.54$ tonne$\cdot$year of data acquired from the PandaX-4T dual-phase xenon time projection chamber. This constraint is derived through detecting electronic recoil signals…

Electron diffusion in a liquid xenon time projection chamber has recently been used to infer the $z$ coordinate of a particle interaction, from the width of the electron signal. The goal of this technique is to reduce the background event…

Instrumentation and Methods for Astrophysics · Physics 2015-05-27 Peter Sorensen

The response of liquid xenon to various types of ionizing radiation has been extensively studied theoretically and experimentally. Recent progress in direct detection dark matter experiments highlights the significance of composite events,…

Searches for neutrinoless double-beta decay continue to expand our understanding of the lepton sector, with experiments now pursuing ton-scale target masses with sensitivity to $m_{\beta\beta}$ covering the allowed parameter space for the…

High Energy Physics - Experiment · Physics 2023-04-10 A. Mastbaum , F. Psihas , J. Zennamo

As liquid xenon TPCs increase in target mass while pursuing the direct detection of WIMP dark matter, the technical challenges arising due to their size call for new solutions and open the discussion on alternative detector concepts.…

Instrumentation and Detectors · Physics 2022-04-14 Fabian Kuger , Julia Dierle , Horst Fischer , Marc Schumann , Francesco Toschi

Two-phase xenon detectors, such as that at the core of the forthcoming LZ dark matter experiment, use photomultiplier tubes to sense the primary (S1) and secondary (S2) scintillation signals resulting from particle interactions in their…

Instrumentation and Methods for Astrophysics · Physics 2021-01-22 D. S. Akerib , A. K. Al Musalhi , S. K. Alsum , C. S. Amarasinghe , A. Ames , T. J. Anderson , N. Angelides , H. M. Araújo , J. E. Armstrong , M. Arthurs , X. Bai , J. Balajthy , S. Balashov , J. Bang , J. W. Bargemann , D. Bauer , A. Baxter , P. Beltrame , E. P. Bernard , A. Bernstein , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , G. M. Blockinger , B. Boxer , C. A. J. Brew , P. Brás , S. Burdin , J. K. Busenitz , M. Buuck , R. Cabrita , M. C. Carmona-Benitez , M. Cascella , C. Chan , N. I. Chott , A. Cole , M. V. Converse , A. Cottle , G. Cox , J. E. Cutter , C. E. Dahl , L. de Viveiros , J. E. Y. Dobson , E. Druszkiewicz , S. R. Eriksen , A. Fan , S. Fayer , N. M. Fearon , S. Fiorucci , H. Flaecher , E. D. Fraser , T. Fruth , R. J. Gaitskell , J. Genovesi , C. Ghag , E. Gibson , S. Gokhale , M. G. D. van der Grinten , C. B. Gwilliam , C. R. Hall , S. J. Haselschwardt , S. A. Hertel , M. Horn , D. Q. Huang , C. M. Ignarra , O. Jahangir , R. S. James , W. Ji , J. Johnson , A. C. Kaboth , A. C. Kamaha , K. Kamdin , K. Kazkaz , D. Khaitan , A. Khazov , I. Khurana , D. Kodroff , L. Korley , E. V. Korolkova , H. Kraus , S. Kravitz , L. Kreczko , B. Krikler , V. A. Kudryavtsev , E. A. Leason , K. T. Lesko , C. Levy , J. Li , J. Liao , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , X. Liu , M. I. Lopes , E. Lopez Asamar , B. López Paredes , W. Lorenzon , S. Luitz , P. A. Majewski , A. Manalaysay , L. Manenti , R. L. Mannino , N. Marangou , M. E. McCarthy , D. N. McKinsey , J. McLaughlin , E. H. Miller , E. Mizrachi , A. Monte , M. E. Monzani , J. A. Morad , J. D. Morales Mendoza , E. Morrison , B. J. Mount , A. St. J. Murphy , D. Naim , A. Naylor , C. Nedlik , H. N. Nelson , F. Neves , J. A. Nikoleyczik , I. Olcina , K. C. Oliver-Mallory , S. Pal , K. J. Palladino , J. Palmer , N. Parveen , E. K. Pease , B. Penning , G. Pereira , A. Piepke , Y. Qie , J. Reichenbacher , C. A. Rhyne , A. Richards , Q. Riffard , G. R. C. Rischbieter , R. Rosero , P. Rossiter , D. Santone , A. B. M. R. Sazzad , R. W. Schnee , P. R. Scovell , S. Shaw , T. A. Shutt , J. J. Silk , C. Silva , R. Smith , M. Solmaz , V. N. Solovov , P. Sorensen , I. Stancu , A. Stevens , K. Stifter , B. Suerfu , T. J. Sumner , N. Swanson , M. Szydagis , W. C. Taylor , R. Taylor , D. J. Temples , P. A. Terman , D. R. Tiedt , M. Timalsina , W. H. To , M. Tripathi , D. R. Tronstad , W. Turner , U. Utku , A. Vaitkus , B. Wang , J. J. Wang , W. Wang , J. R. Watson , R. C. Webb , R. G. White , T. J. Whitis , M. Williams , F. L. H. Wolfs , D. Woodward , C. J. Wright , X. Xiang , J. Xu , M. Yeh , P. Zarzhitsky

The Neutrino Experiment with a Xenon TPC (NEXT) is intended to investigate the neutrinoless double beta decay of 136Xe, which requires a severe suppression of potential backgrounds. An extensive screening and material selection process is…

A comprehensive model for explaining scintillation yield in liquid xenon is introduced. We unify various definitions of work function which abound in the literature and incorporate all available data on electron recoil scintillation yield.…

Instrumentation and Detectors · Physics 2017-02-20 M. Szydagis , N. Barry , K. Kazkaz , J. Mock , D. Stolp , M. Sweany , M. Tripathi , S. Uvarov , N. Walsh , M. Woods

There exist well motivated models of particle dark matter which predominantly scatter inelastically off nuclei in direct detection experiments. This inelastic transition causes the DM to up-scatter in terrestrial experiments into an excited…

High Energy Physics - Phenomenology · Physics 2017-01-24 Joseph Bramante , Patrick J. Fox , Graham D. Kribs , Adam Martin

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

NEXT-100 is currently being constructed at the Laboratorio Subterr\'aneo de Canfranc in the Spanish Pyrenees and will search for neutrinoless double beta decay using a high-pressure gaseous time projection chamber (TPC) with 100 kg of…

Instrumentation and Detectors · Physics 2024-02-06 NEXT Collaboration , K. Mistry , L. Rogers , B. J. P. Jones , B. Munson , L. Norman , C. Adams , H. Almazán , 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 , T. Contreras , 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 , E. D. C. Freitas , Z. Freixa , J. J. Gómez-Cadenas , R. González , J. W. R. Grocott , R. Guenette , K. Hafidi , J. Hauptman , C. A. O. Henriques , J. A. Hernando~Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. P. Marques , J. Martín-Albo , G. Martínez-Lema , M. Martínez-Vara , Z. E. Meziani , R. L. Miller , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , P. Novella , A. Nuñez , D. R. Nygren , E. Oblak , D. Oliver , J. Palacio , B. Palmeiro , A. Para , I. Parmaksiz , J. Pelegrin , M. Pérez Maneiro , M. Querol , A. B. Redwine , J. Renner , I. Rivilla , C. Rogero , B. Romeo , C. Romo-Luque , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , A. Simón , S. R. Soleti , M. Sorel , J. Soto-Oton , J. M. R. Teixeira , J. F. Toledo , J. Torrent , A. Trettin , A. Usón , J. F. C. A. Veloso , J. Waiton , A. Yubero

Neutrinoless double beta decays in liquid xenon produce a significant amount of Cherenkov light, with a photon number and angular distribution that distinguishes these events from common backgrounds. A GEANT4 simulation was used to simulate…

Instrumentation and Detectors · Physics 2019-02-20 Jason Philip Brodsky , Samuele Sangiorgio , Michael Heffner , Tyana Stiegler

The South Pole Telescope (SPT) has probed an expanded angular range of the CMB temperature power spectrum. Their recent analysis of the latest cosmological data prefers nonzero neutrino masses, mnu = 0.32+-0.11 eV. This result, if confirmed…

High Energy Physics - Phenomenology · Physics 2013-04-01 J. J. Gomez-Cadenas , J. Martin-Albo , J. Muñoz Vidal , C. Peña-Garay

We study a possible calibration technique for the nEXO experiment using a $^{127}$Xe electron capture source. nEXO is a next-generation search for neutrinoless double beta decay ($0\nu\beta\beta$) that will use a 5-tonne, monolithic liquid…

Instrumentation and Detectors · Physics 2022-08-03 B. G. Lenardo , C. A. Hardy , R. H. M. Tsang , J. C. Nzobadila Ondze , A. Piepke , S. Triambak , A. Jamil , G. Adhikari , S. Al Kharusi , E. Angelico , I. J. Arnquist , V. Belov , E. P. Bernard , A. Bhat , T. Bhatta , A. Bolotnikov , P. A. Breur , J. P. Brodsky , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Cao , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , J. R. Cohen , R. Collister , J. Dalmasson , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , Y. Y. Ding , M. J. Dolinski , J. Echevers , B. Eckert , M. Elbeltagi , L. Fabris , D. Fairbank , W. Fairbank , J. Farine , Y. S. Fu , G. Gallina , P. Gautam , G. Giacomini , W. Gillis , C. Gingras , R. Gornea , G. Gratta , K. Harouaka , M. Heffner , E. Hein , J. Hößl , A. House , A. Iverson , X. S. Jiang , A. Karelin , L. J. Kaufman , R. Krücken , A. Kuchenkov , K. S. Kumar , A. Larson , K. G. Leach , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , J. Masbou , K. McMichael , M. Medina Peregrina , B. Mong , D. C. Moore , K. Murray , J. Nattress , C. R. Natzke , X. E. Ngwadla , K. Ni , Z. Ning , J. L. Orrell , G. S. Ortega , I. Ostrovskiy , C. T. Overman , A. Perna , T. Pinto Franco , A. Pocar , J. F. Pratte , N. Priel , E. Raguzin , G. J. Ramonnye , H. Rasiwala , K. Raymond , G. Richardson , M. Richman , J. Ringuette , P. C. Rowson , R. Saldanha , S. Sangiorgio , X. Shang , A. K. Soma , F. Spadoni , V. Stekhanov , X. L. Sun , S. Thibado , A. Tidball , J. Todd , T. Totev , O. A. Tyuka , F. Vachon , V. Veeraraghavan , S. Viel , K. Wamba , Y. Wang , Q. Wang , W. Wei , L. J. Wen , U. Wichoski , S. Wilde , W. H. Wu , W. Yan , L. Yang , O. Zeldovich , J. Zhao , T. Ziegler

For the last decade numerous researchers have been trying to develop experimental techniques to use X-ray Thomson scattering as a method to measure the temperature, electron density, and ionization state of high energy density plasmas such…

Plasma Physics · Physics 2012-10-02 J. Nilsen , W. R. Johnson , K. T. Cheng

We present evidence of non-excimer-based secondary scintillation in gaseous xenon, obtained using both the NEXT-White TPC and a dedicated setup. Detailed comparison with first-principle calculations allows us to assign this scintillation…

The Deep Underground Neutrino Experiment (DUNE) will be the next generation long-baseline neutrino experiment. The far detector is designed as a complex of four LAr-TPC (Liquid Argon Time Projection Chamber) modules with 17 kt of liquid…

Instrumentation and Detectors · Physics 2022-01-11 Niccolò Gallice

The performance of an electroluminescence (EL) Time Projection Chamber (TPC) with a multi avalanche photodiode (APD) readout was studied in pure xenon at 3.8 bar. Intercalibration and reconstruction methods were developed and applied to the…

Dual-phase xenon time projection chamber (TPC) detectors offer heightened sensitivities for dark matter detection across a spectrum of particle masses. To broaden their capability to low-mass dark matter interactions, we investigated the…

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