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Related papers: The XeBRA platform for liquid xenon time projectio…

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We report on the calibration of an argon/isobutane (97.7 %/2.3 %)-filled GridPix detector with soft X-rays (277 eV to 8 keV) using the variable energy X-ray source of the CAST Detector Lab at CERN. We study the linearity and energy…

Instrumentation and Detectors · Physics 2018-04-18 Christoph Krieger , Jochen Kaminski , Theodoros Vafeiadis , Klaus Desch

Noble liquid radiation detectors have long been afflicted by spurious electron emission from their cathodic electrodes. This phenomenon must be understood and mitigated in the next generation of liquid xenon (LXe) experiments searching for…

Instrumentation and Detectors · Physics 2018-08-29 A. Tomás , H. M. Araújo , A. J. Bailey , A. Bayer , E. Chen , B. López Paredes , T. J. Sumner

The Liquid Xenon Gamma-Ray Imaging Telescope (LXeGRIT) is the first realization of a liquid xenon time projection chamber for Compton imaging of MeV gamma-ray sources in astrophysics. By measuring the energy deposit and the three spatial…

Instrumentation and Detectors · Physics 2008-11-26 E. Aprile , A. Curioni , K. L. Giboni , M. Kobayashi , U. G. Oberlack , S. Zhang

We propose a new detector concept, GraXe (to be pronounced as grace), to search for neutrinoless double beta decay in Xe-136. GraXe combines a popular detection medium in rare-event searches, liquid xenon, with a new, background-free…

Instrumentation and Detectors · Physics 2012-02-28 J. J. Gomez-Cadenas , F. Guinea , M. M. Fogler , M. I. Katsnelson , J. Martin-Albo , F. Monrabal , J. Muñoz-Vidal

The next generation of bolometric experiments searching for rave events, in particular for the neutrino-less double beta decay, needs fast, high-sensitivity and easy-to-scale cryogenic light detectors. The CALDER project (2014-2020)…

NEXT-100 is a high-pressure xenon time projection chamber with electroluminescent amplification, designed to operate with up to approximately 70.5 kg at 13.5 bar. It is the most recent detector developed by the NEXT collaboration to search…

Instrumentation and Detectors · Physics 2026-01-13 NEXT Collaboration , M. Pérez Maneiro , M. Martínez-Vara , S. Torelli , G. Martínez-Lema , P. Novella , J. A. Hernando Morata , J. J. Gómez-Cadenas , C. Adams , H. Almazán , V. Álvarez , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , Y. Ayyad , C. D. R. Azevedo , K. Bailey , F. Ballester , J. E. Barcelon , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodoline , N. Byrnes , A. Castillo , E. Church , L. Cid , M. Cid , X. Cid , C. A. N. Conde , C. Cortes-Parra , F. P. Cossío , R. Coupe , E. Dey , P. Dietz , C. Echeverria , M. Elorza , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , F. W. Foss , Z. Freixa , J. García-Barrena , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , A. F. B. Isabel , B. J. P. Jones , F. Kellerer , L. Larizgoitia , A. Larumbe , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. Marauri , A. P. Marques , J. Martín-Albo , A. Martínez , R. L. Miller , K. Mistry , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , D. R. Nygren , E. Oblak , J. Palacio , B. Palmeiro , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Querol , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , E. Ruiz-Chóliz , P. Saharia , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , A. L. M. Silva , 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 , P. R. G. Valle , M. Vanga , P. Vázquez Cabaleiro , J. F. C. A. Veloso , J. D. Villamil , J. Waiton , A. Yubero-Navarro

The XENON1T experiment aims for the direct detection of dark matter in a cryostat filled with 3.3 tons of liquid xenon. In order to achieve the desired sensitivity, the background induced by radioactive decays inside the detector has to be…

Instrumentation and Detectors · Physics 2017-05-09 XENON Collaboration , E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , F. D. Amaro , M. Anthony , F. Arneodo , P. Barrow , L. Baudis , B. Bauermeister , M. L. Benabderrahmane , T. Berger , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , L. Bütikofer , J. Calvén , J. M. R. Cardoso , M. Cervantes , D. Cichon , D. Coderre , A. P. Colijn , J. Conrad , J. P. Cussonneau , M. P. Decowski , P. de Perio , P. Di Gangi , A. Di Giovanni , S. Diglio , E. Duchovni , G. Eurin , J. Fei , A. D. Ferella , A. Fieguth , D. Franco , W. Fulgione , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , C. Geis , L. W. Goetzke , L. Grandi , Z. Greene , C. Grignon , C. Hasterok , E. Hogenbirk , R. Itay , B. Kaminsky , G. Kessler , A. Kish , H. Landsman , R. F. Lang , D. Lellouch , L. Levinson , M. Le Calloch , Q. Lin , S. Lindemann , M. Lindner , J. A. M. Lopes A. Manfredini , I. Maris , T. Marrodán Undagoitia , J. Masbou , F. V. Massoli , D. Masson , D. Mayani , Y. Meng , M. Messina , K. Micheneau , B. Miguez , A. Molinario , M. Murra , J. Naganoma , K. Ni , U. Oberlack , S. E. A. Orrigo , P. Pakarha , B. Pelssers , R. Persiani , F. Piastra , J. Pienaar , M. -C. Piro , V. Pizzella , G. Plante , N. Priel , L. Rauch , S. Reichard , C. Reuter , A. Rizzo , S. Rosendahl , N. Rupp , R. Saldanha , J. M. F. dos Santos , G. Sartorelli , M. Scheibelhut , S. Schindler , J. Schreiner , M. Schumann , L. Scotto Lavina , M. Selvi , P. Shagin , E. Shockley , M. Silva , H. Simgen , M. v. Sivers , A. Stein , D. Thers , A. Tiseni , G. Trinchero , C. Tunnell , N. Upole , H. Wang , Y. Wei , C. Weinheimer , J. Wulf , J. Ye , Y. Zhang , I. Cristescu

We present a review of the current experimental and theoretical understanding of electron transport in noble liquids. Special attention is given to recent measurements that coincide with the development of time projection chambers (TPCs)…

Applied Physics · Physics 2025-04-24 G. J. Boyle , N. A. Garland , D. L. Muccignat , I. Simonović , D. Bošnjaković , S. Dujko , R. D. White

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

The Beam Instrumentation group at CERN has developed a new scintillating fibre beam monitor for the measurement of secondary particle beams in the CERN Experimental Areas. The monitor has a simple design that stands out for its low material…

Instrumentation and Detectors · Physics 2019-10-29 I. Ortega , L. Fosse , J. Franchi , A. Frassier , J. Fullerton , J. Kral , J. Lauener , T. Schneider , G. Tranquille

A new technique for medical imaging, "3{\gamma} imaging", is studied by our group at SUBATECH for few years. A small liquid xenon time projection chamber prototype has been built in order to demonstrate the feasibility of this technique.…

This paper describes the design and construction of the MicroBooNE liquid argon time projection chamber and associated systems. MicroBooNE is the first phase of the Short Baseline Neutrino program, located at Fermilab, and will utilize the…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE Collaboration , R. Acciarri , C. Adams , R. An , A. Aparicio , S. Aponte , J. Asaadi , M. Auger , N. Ayoub , L. Bagby , B. Baller , R. Barger , G. Barr , M. Bass , F. Bay , K. Biery , M. Bishai , A. Blake , V. Bocean , D. Boehnlein , V. D. Bogert , T. Bolton , L. Bugel , C. Callahan , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , S. Chappa , H. Chen , K. Chen , C. Y. Chi , C. S. Chiu , E. Church , D. Cianci , G. H. Collin , J. M. Conrad , M. Convery , J. Cornele , P. Cowan , J. I. Crespo-Anadon , G. Crutcher , C. Darve , R. Davis , M. Del Tutto , D. Devitt , S. Duffin , S. Dytman , B. Eberly , A. Ereditato , D. Erickson , L. Escudero Sanchez , J. Esquivel , S. Farooq , J. Farrell , D. Featherston , B. T. Fleming , W. Foreman , A. P. Furmanski , V. Genty , M. Geynisman , D. Goeldi , B. Goff , S. Gollapinni , N. Graf , E. Gramellini , J. Green , A. Greene , H. Greenlee , T. Griffin , R. Grosso , R. Guenette , A. Hackenburg , R. Haenni , P. Hamilton , P. Healey , O. Hen , E. Henderson , V Hewes , C. Hill , K. Hill , L. Himes , J. Ho , G. Horton-Smith , D. Huffman , C. M. Ignarra , C. James , E. James , J. Jan de Vries , W. Jaskierny , C. M. Jen , L. Jiang , B. Johnson , M. Johnson , R. A. Johnson , B. J. P. Jones , J. Joshi , H. Jostlein , D. Kaleko , L. N. Kalousis , G. Karagiorgi , T. Katori , P. Kellogg , W. Ketchum , J. Kilmer , B. King , B. Kirby , M. Kirby , E. Klein , T. Kobilarcik , I. Kreslo , R. Krull , R. Kubinski , G. Lange , F. Lanni , A. Lathrop , A. Laube , W. M. Lee , Y. Li , D. Lissauer , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , G. Lukhanin , M. Luethi , B. Lundberg , X. Luo , G. Mahler , I. Majoros , D. Makowiecki , A. Marchionni , C. Mariani , D. Markley , J. Marshall , D. A. Martinez Caicedo , K. T. McDonald , D. McKee , A. McLean , J. Mead , V. Meddage , T. Miceli , G. B. Mills , W. Miner , J. Moon , M. Mooney , C. D. Moore , Z. Moss , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , B. Norris , N. Norton , J. Nowak , M. OBoyle , T. Olszanowski , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , R. Pelkey , M. Phipps , S. Pordes , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , R. A Rameika , B. Rebel , R. Rechenmacher , S. Rescia , L. Rochester , C. Rudolf von Rohr , A. Ruga , B. Russell , R. Sanders , W. R. Sands , M. Sarychev , D. W. Schmitz , A. Schukraft , R. Scott , W. Seligman , M. H. Shaevitz , M. Shoun , J. Sinclair , W. Sippach , T. Smidt , A. Smith , E. L. Snider , M. Soderberg , M. Solano-Gonzalez , S. Soldner-Rembold , S. R. Soleti , J. Sondericker , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , K. Sutton , A. M. Szelc , K. Taheri , N. Tagg , K. Tatum , J. Teng , K. Terao , M. Thomson , C. Thorn , J. Tillman , M. Toups , Y. T. Tsai , S. Tufanli , T. Usher , M. Utes , R. G. Van de Water , C. Vendetta , S. Vergani , E. Voirin , J. Voirin , B. Viren , P. Watkins , M. Weber , T. Wester , J. Weston , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , K. C. Wu , T. Yang , B. Yu , G. P. Zeller , J. Zennamo , C. Zhang , M. Zuckerbrot

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

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

The prevalent use of large volume liquid argon detectors strongly motivates the development of novel readout and monitoring technology which functions at cryogenic temperatures. This paper presents the development of a cryogenic CMOS camera…

Instrumentation and Detectors · Physics 2017-04-05 Nicola McConkey , Neil Spooner , Matthew Thiesse , Michael Wallbank , Thomas Karl Warburton

The two-phase xenon detector is at the frontier of dark matter direct search. This kind of detector uses liquid xenon as the sensitive target and is operated in two-phase (liquid/gas) mode, where the liquid level needs to be monitored and…

Instrumentation and Detectors · Physics 2014-05-08 J. Hu , H. Gong , Q. Lin , K. Ni , A. Tan , Y. Wei , M. Xiao , X. Xiao , L. Zhao

Challenges in scaling up noble-liquid time projection chambers prompted the exploration of new detection concepts. The liquid hole-multiplier (LHM) was introduced as a potential component, enabling the detection of ionization electrons and…

Instrumentation and Detectors · Physics 2024-09-24 G. Martínez-Lema , A. Roy , A. Breskin , L. Arazi

PET is a functional imaging technique based on detection of annihilation photons following beta decay producing positrons. In this paper, we present the concept of a new PET system for preclinical applications consisting of a ring of twelve…

Instrumentation and Detectors · Physics 2015-03-19 A. Miceli , P. Amaudruz , F. Benard , D. A. Bryman , L. Kurchaninov , J. P. Martin , A. Muennich , F. Retiere , T. J. Ruth , V. Sossi , A. J. Stoessl

Experimental results for the reflection coefficient of shock-compressed dense Xenon plasmas at pressures of 1.6 - 17 GPa and temperatures around 30 000 K using a laser beam with \lambda = 1.06 10^-6 m are compared with calculations based on…

Plasma Physics · Physics 2009-11-07 H. Reinholz , G. Roepke , A. Wierling , V. Mintsev , V. Gryaznov

A Nd:YAG laser was used to simulate charged particle tracks at known positions in the CERES Time Projection Chamber at the CERN SPS. The system was primarily developed to study the response of the readout electronics and to calibrate the…

Nuclear Experiment · Physics 2008-11-26 Dariusz Miskowiec , Peter Braun-Munzinger