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Liquid xenon particle detectors rely on excellent light collection efficiency for their performance. This depends on the high reflectivity of polytetrafluoroethylene (PTFE) at the xenon scintillation wavelength of 178 nm, but the angular…

Instrumentation and Detectors · Physics 2020-03-31 S. Kravitz , R. J. Smith , L. Hagaman , E. P. Bernard , D. N. McKinsey , L. Rudd , L. Tvrznikova , G. D. Orebi Gann , M. Sakai

Dark matter detectors that utilize liquid xenon have now achieved tonne-scale targets, giving them sensitivity to all flavours of supernova neutrinos via coherent elastic neutrino-nucleus scattering. Considering for the first time a…

High Energy Astrophysical Phenomena · Physics 2016-12-21 Rafael F. Lang , Christopher McCabe , Shayne Reichard , Marco Selvi , Irene Tamborra

PETALO (a Positron Emission Tof Apparatus based on Liquid xenOn) is a new approach for Positron Emission Tomography scanners, based on liquid xenon. The PETALO detector aims at capturing the light produced by the scintillation in LXe taking…

The use of gaseous Time Projection Chambers enables the detection and the detailed study of rare events due to particles interactions with the atoms of the gas with energy releases as low as a few keV. Due to this capability, these…

The NEXT experiment aims at searching for the hypothetical neutrinoless double-beta decay from the ${}^{136}$Xe isotope using a high-purity xenon TPC. Efficient discrimination of the events through pattern recognition of the topology of…

Scintillation light is used in liquid argon (LAr) neutrino detectors to provide a trigger signal, veto information against cosmic rays, and absolute event timing. In this work, we discuss additional opportunities offered by detectors with…

Instrumentation and Detectors · Physics 2015-01-27 M. Sorel

Scintillation light, produced alongside ionisation charge from particle interactions, plays a critical role in liquid argon time projection chamber (LArTPC) detectors. A detailed understanding of its production and detection mechanisms is…

Instrumentation and Detectors · Physics 2026-03-26 MicroBooNE collaboration , P. Abratenko , D. Andrade Aldana , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , A. Barnard , G. Barr , D. Barrow , J. Barrow , V. Basque , J. Bateman , B. Behera , O. Benevides Rodrigues , S. Berkman , A. Bhat , M. Bhattacharya , V. Bhelande , A. Binau , M. Bishai , A. Blake , B. Bogart , T. Bolton , M. B. Brunetti , L. Camilleri , D. Caratelli , F. Cavanna , G. Cerati , A. Chappell , Y. Chen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , R. Cross , M. Del Tutto , S. R. Dennis , P. Detje , R. Diurba , Z. Djurcic , K. Duffy , S. Dytman , B. Eberly , P. Englezos , A. Ereditato , J. J. Evans , C. Fang , B. T. Fleming , W. Foreman , D. Franco , A. P. Furmanski , F. Gao , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , E. Gramellini , P. Green , H. Greenlee , L. Gu , W. Gu , R. Guenette , L. Hagaman , M. D. Handley , O. Hen , A. Hergenhan , M. Harrison , S. Hawkins , C. Hilgenberg , G. A. Horton-Smith , A. Hussain , B. Irwin , M. S. Ismail , C. James , X. Ji , J. H. Jo , A. Johnson , R. A. Johnson , D. Kalra , G. Karagiorgi , W. Ketchum , A. Kelly , M. Kirby , T. Kobilarcik , K. Kumar , N. Lane , J. -Y. Li , Y. Li , K. Lin , B. R. Littlejohn , L. Liu , S. Liu , W. C. Louis , X. Luo , T. Mahmud , N. Majeed , C. Mariani , J. Marshall , D. A. Martinez Caicedo , F. Martinez Lopez , M. G. Manuel Alves , S. Martynenko , A. Mastbaum , I. Mawby , N. McConkey , B. McConnell , L. Mellet , J. Mendez , J. Micallef , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. A. Hernandez Morquecho , M. M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , C. Nguyen , L. Nguyen , J. Nowak , N. Oza , O. Palamara , N. Pallat , V. Paolone , A. Papadopoulou , V. Papavassiliou , H. Parkinson , S. F. Pate , N. Patel , Z. Pavlovic , E. Piasetzky , K. Pletcher , I. Pophale , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , R. Raymond , M. Reggiani-Guzzo , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , I. Safa , C. Sauer , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , L. Silva , E. L. Snider , S. Soldner-Rembold , J. Spitz , M. Stancari , J. St. John , T. Strauss , A. M. Szelc , N. Taniuchi , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , A. Trettin , Y. -T. Tsai , J. Tyler , M. A. Uchida , T. Usher , B. Viren , J. Wang , L. Wang , M. Weber , H. Wei , A. J. White , S. Wolbers , T. Wongjirad , K. Wresilo , W. Wu , E. Yandel , T. Yang , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang , Y. Zhang

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 search for neutrinoless double beta decay ($0\nu\beta\beta$) remains one of the most compelling experimental avenues for the discovery in the neutrino sector. Electroluminescent gas-phase time projection chambers are well suited to…

Instrumentation and Detectors · Physics 2023-08-04 NEXT Collaboration , N. K. Byrnes , I. Parmaksiz , C. Adams , J. Asaadi , J Baeza-Rubio , K. Bailey , E. Church , D. González-Díaz , A. Higley , B. J. P. Jones , K. Mistry , I. A. Moya , D. R. Nygren , P. Oyedele , L. Rogers , K. Stogsdill , H. Almazán , V. Álvarez , B. Aparicio , A. I. Aranburu , L. Arazi , I. J. Arnquist , S. Ayet , C. D. R. Azevedo , F. Ballester , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , S. Bounasser , S. Cárcel , J. V. Carrión , S. Cebrián , L. Cid , C. A. N. Conde , T. Contreras , F. P. Cossío , E. Dey , G. Díaz , T. Dickel , M. Elorza , J. Escada , R. Esteve , A. Fahs , R. Felkai , L. M. P. Fernandes , P. Ferrario , A. L. Ferreira , F. W. Foss , E. D. C. Freitas , Z. Freixa , J. Generowicz , A. Goldschmidt , J. J. Gómez-Cadenas , R. González , J. Grocott , R. Guenette , J. Haefner , K. Hafidi , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , J. Ho , P. Ho , Y. Ifergan , L. Labarga , L. Larizgoitia , P. Lebrun , F Lopez , D. Lopez Gutierrez , 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 , F. Monrabal , C. M. B. Monteiro , F. J. Mora , J. Muñoz Vidal , K. E. Navarro , P. Novella , A. Nuñez , E. Oblak , M. Odriozola-Gimeno , J. Palacio , B. Palmeiro , A. Para , J Pelegrin , M. Pérez Maneiro , M. Querol , A. B. Redwine , J. Renner , I. Rivilla , J. Rodríguez , C. Rogero , B. Romeo , C. Romo-Luque , F. P. Santos , J. M. F. dos Santos , A. Simón , S. R. Soleti , M. Sorel , C. Stanford , J. M. R. Teixeira , J. F. Toledo , J. Torrent , A. Usón , J. F. C. A. Veloso , T. T. Vuong , J. Waiton , J. T. White

We report on the study of a new liquid scintillator target for neutrino interactions in the framework of the research and development program of the BOREXINO solar neutrino experiment. The scintillator consists of…

Instrumentation and Detectors · Physics 2012-08-27 Borexino Collaboration

Presented here are first tests of a Gaseous Photomultiplier based on a cascade of Thick GEM structures intended for gamma-ray position reconstruction in liquid Argon. The detector has a MgF$_2$ window, transparent to VUV light, and a CsI…

Instrumentation and Detectors · Physics 2015-09-02 B. Lopez Paredes , C. D. R. Azevedo , S. Paganis , A. L. M. Silva , N. J. C. Spooner , J. F. C. A. Veloso

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

Vacuum ultraviolet light emission from xenon-doped liquid argon is described in the context of liquid noble gas particle detectors. Xenon concentrations in liquid argon from 0.1 ppm to 1000 ppm were studied. The energy transfer from the…

Instrumentation and Detectors · Physics 2015-11-25 A. Neumeier , T. Dandl , T. Heindl , A. Himpsl , L. Oberauer , W. Potzel , S. Roth , S. Schönert , J. Wieser , A. Ulrich

The baseline technology for the Surrounding Background Tagger of the recently approved SHiP experiment relies on liquid scintillator composed of linear alkylbenzene and 2,5-diphenyloxazole as active detector material. The primary…

Basic R & D have been carried out with one small straw tube detector prototype with premixed gas of Ar+CO2 in 70:30 and 90:10 ratio. The gain and the energy resolution are measured with Fe55 X-ray source. Effect of temperature and pressure…

Instrumentation and Detectors · Physics 2017-09-26 S. Roy , N. Nandi , R. P. Adak , S. Biswas , S. Das , S. K. Ghosh , S. K. Prasad , S. Raha

An 800L liquid xenon scintillation $\gamma$ ray detector is being developed for the MEG experiment which will search for $\mu^+\to\mathrm{e}^+\gamma$ decay at the Paul Scherrer Institut. Absorption of scintillation light of xenon by…

A presentation at the SciNeGHE conference of the past achievements, of the present activities and of the perspectives for the future of the HARPO project, the development of a time projection chamber as a high-performance gamma-ray…

Instrumentation and Methods for Astrophysics · Physics 2018-02-14 Denis Bernard

Background: we develop the concept of a Micromegas (MICRO-MEsh GAseous Structure) readout plane with an additional GEM (Gas Electron Multiplier) preamplification stage placed a few mm above it, to increase the maximum effective gain of the…