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We report the measurement of the time-of-flight of ~17 GeV muon neutrinos on the CNGS baseline (732 km) with the Large Volume Detector (LVD) at the Gran Sasso Laboratory. The CERN-SPS accelerator has been operated from May 10th to May 24th…

The MicroBooNE experiment is an 85 tonne active mass liquid argon time projection chamber neutrino detector exposed to the on-axis Booster Neutrino Beam (BNB) at Fermilab. One of MicroBooNE's physics goals is the precise measurement of…

High Energy Physics - Experiment · Physics 2025-12-24 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 , O. Benevides Rodrigues , S. Berkman , A. Bhat , M. Bhattacharya , 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 , G. A. Fiorentini Aguirre , 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 , P. Guzowski , L. Hagaman , M. D. Handley , O. Hen , C. Hilgenberg , G. A. Horton-Smith , A. Hussain , B. Irwin , M. S. Ismail , C. James , X. Ji , J. H. Jo , R. A. Johnson , Y. J. Jwa , D. Kalra , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , N. Lane , J. -Y. Li , Y. Li , K. Lin , B. R. Littlejohn , L. Liu , W. C. Louis , X. Luo , T. Mahmud , C. Mariani , D. Marsden , J. Marshall , N. Martinez , D. A. Martinez Caicedo , S. Martynenko , A. Mastbaum , I. Mawby , N. McConkey , V. Meddage , L. Mellet , J. Mendez , J. Micallef , K. Mistry , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , C. 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 , M. Reggiani-Guzzo , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , I. Safa , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , E. L. Snider , M. Soderberg , 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 , 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

The DANSS detector is located directly below a commercial reactor core at the Kalinin Nuclear Power Plant. Such a position provides an overburden about 50 m.w.e. in vertical direction. In terms of the cosmic rays it occupies an intermediate…

The pixel detector of the Compact Muon Solenoid experiment consists of three barrel layers and two disks for each endcap. The detector was installed in summer 2008, commissioned with charge injections, and operated in the 3.8 T magnetic…

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

Thorough modeling of the physics involved in liquid argon calorimetry is essential for accurately predicting the performance of DUNE and optimizing its design and analysis pipeline. At the fundamental level, it is essential to quantify the…

High Energy Physics - Phenomenology · Physics 2020-11-18 Alexander Friedland , Shirley Weishi Li

The ArDM experiment completed a single-phase commissioning run in 2015 with an active liquid argon target of nearly one tonne in mass. The analysis of the data and comparison to simulations allowed for a test of the crucial detector…

The ArgoNeuT liquid argon time projection chamber has collected thousands of neutrino and antineutrino events during an extended run period in the NuMI beam-line at Fermilab. This paper focuses on the main aspects of the detector layout and…

The Cryogenic Apparatus for Precision Tests of Argon Interactions with Neutrinos (CAPTAIN) program is designed to make measurements of scientific importance to long-baseline neutrino physics and physics topics that will be explored by large…

Instrumentation and Detectors · Physics 2015-09-28 Jianming Bian

Xenon dual-phase time projections chambers (TPCs) have proven to be a successful technology in studying physical phenomena that require low-background conditions. With 40t of liquid xenon (LXe) in the TPC baseline design, DARWIN will have a…

Instrumentation and Detectors · Physics 2024-07-26 M. Adrover , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , B. Antunovic , E. Aprile , M. Babicz , D. Bajpai , E. Barberio , L. Baudis , M. Bazyk , N. Bell , L. Bellagamba , R. Biondi , Y. Biondi , A. Bismark , C. Boehm , A. Breskin , E. J. Brookes , A. Brown , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , A. Chauvin , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , M. P. Decowski , A. Deisting , P. Di Gangi , S. Diglio , M. Doerenkamp , G. Drexlin , K. Eitel , A. Elykov , R. Engel , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , W. Fulgione , P. Gaemers , R. Gaior , M. Galloway , N. Garroum , S. Ghosh , F. Girard , R. Glade-Beucke , F. Glück , L. Grandi , J. Grigat , R. Größle , H. Guan , M. Guida , R. Hammann , V. Hannen , S. Hansmann-Menzemer , N. Hargittai , T. Hasegawa , C. Hils , A. Higuera , K. Hiraoka , L. Hoetzsch , M. Iacovacci , Y. Itow , J. Jakob , F. Jörg , M. Kara , P. Kavrigin , S. Kazama , M. Keller , B. Kilminster , M. Kleifges , M. Kobayashi , A. Kopec , B. von Krosigk , F. Kuger , H. Landsman , R. F. Lang , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , F. Lombardi , J. Loizeau , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , T. Marrodán Undagoitia , J. A. M. Lopes , F. Marignetti , K. Martens , J. Masbou , S. Mastroianni , S. Milutinovic , K. Miuchi , R. Miyata , A. Molinario , C. M. B. Monteiro , K. Morå , E. Morteau , Y. Mosbacher , J. Müller , M. Murra , J. L. Newstead , K. Ni , U. G. Oberlack , I. Ostrovskiy , B. Paetsch , M. Pandurovic , Q. Pellegrini , R. Peres , J. Pienaar , M. Pierre , M. Piotter , G. Plante , T. R. Pollmann , L. Principe , J. Qi , J. Qin , M. Rajado Silva , D. Ramírez García , A. Razeto , S. Sakamoto , L. Sanchez , P. Sanchez-Lucas , J. M. F. dos Santos , G. Sartorelli , A. Scaffidi , P. Schulte , H. -C. Schultz-Coulon , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Sharma , W. Shen , M. Silva , H. Simgen , R. Singh , M. Solmaz , O. Stanley , M. Steidl , P. L. Tan , A. Terliuk , D. Thers , T. Thümmler , F. Tönnies , F. Toschi , G. Trinchero , R. Trotta , C. Tunnell , P. Urquijo , K. Valerius , S. Vecchi , S. Vetter , G. Volta , D. Vorkapic , W. Wang , K. M. Weerman , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , J. Wolf , T. Wolf , V. H. S. Wu , M. Wurm , Y. Xing , M. Yamashita , J. Ye , G. Zavattini , K. Zuber

MicroBooNE is a liquid argon time projection chamber (LArTPC) neutrino detector located along the Fermilab Booster Neutrino Beam and 8 degrees off-axis to the Neutrinos at the Main Injector beam. MicroBooNE collected data from both beams…

High Energy Physics - Experiment · Physics 2026-02-02 Liang Liu

We present the first prototype of a novel thermal neutron detector using the time projection method. The system consists of 8 TimePix ASICS with postprocessed InGrid meshes. Each ASIC has 256 x 256 pixels of 55 mum x 55mum in size with the…

Instrumentation and Detectors · Physics 2018-12-26 M. Köhli , K. Desch , M. Gruber , J. Kaminski , F. P. Schmidt , T. Wagner

A search for long-lived particles decaying into muon pairs is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS experiment at the LHC in 2017 and 2018, corresponding to an integrated…

High Energy Physics - Experiment · Physics 2022-04-19 CMS Collaboration

Pressurized drift-tube chambers are efficient detectors for high-precision tracking over large areas. The Monitored Drift-Tube (MDT) chambers of the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC) reach a spatial…

Instrumentation and Detectors · Physics 2016-10-04 B. Bittner , J. Dubbert , S. Horvat , O. Kortner , H. Kroha , F. Legger , R. Richter , S. Adomeit , O. Biebel , A. Engl , R. Hertenberger , F. Rauscher , A. Zibell

ColdADC is a custom ASIC digitizer implemented in 65 nm CMOS technology using specialized techniques for long-term reliability in cryogenic environments. ColdADC was developed for use in the DUNE Far Detector complex, which will consist of…

Instrumentation and Detectors · Physics 2025-10-09 Wenjie Wu , Benjamin Jargowsky , Yiwen Xiao , Alejandro Yankelevich , Jianming Bian , Cheng-Ju Lin , Tarun Prakash , David Christian

A small liquid argon Time Projection Chamber (LAr TPC) was operated for the first time in a magnetic field of 0.55 Tesla. The imaging properties of the detector were not affected by the magnetic field. In a test run with cosmic rays a…

Instrumentation and Detectors · Physics 2008-11-26 A. Badertscher , M. Laffranchi , A. Meregaglia , A. Mueller , A. Rubbia

The Deep Underground Neutrino Experiment (DUNE) Phase-II Far Detector is considering an approximately 2000\,m$^2$ photon detection system to achieve a target mean light yield of 180\,PE/MeV. Meeting this requirement demands scalable,…

A prototype detection unit of the KM3NeT deep-sea neutrino telescope has been installed at 3500m depth 80km offshore the Italian coast. KM3NeT in its final configuration will contain several hundreds of detection units. Each detection unit…

Instrumentation and Methods for Astrophysics · Physics 2016-04-06 KM3NeT Collaboration , S. Adrián-Martínez , M. Ageron , F. Aharonian , S. Aiello , A. Albert , F. Ameli , E. G. Anassontzis , G. C. Androulakis , M. Anghinolfi , G. Anton , S. Anvar , M. Ardid , T. Avgitas , K. Balasi , H. Band , G. Barbarino , E. Barbarito , F. Barbato , B. Baret , S. Baron , J. Barrios , A. Belias , E. Berbee , A. M. van den Berg , A. Berkien , V. Bertin , S. Beurthey , V. van Beveren , N. Beverini , S. Biagi , A. Biagioni , S. Bianucci , M. Billault , A. Birbas , H. Boer Rookhuizen , R. Bormuth , V. Bouché , B. Bouhadef , G. Bourlis , C. Boutonnet , M. Bouwhuis , C. Bozza , R. Bruijn , J. Brunner , G. Cacopardo , L. Caillat , M. Calamai , D. Calvo , A. Capone , L. Caramete , F. Caruso , S. Cecchini , A. Ceres , R. Cereseto , C. Champion , F. Château , T. Chiarusi , B. Christopoulou , M. Circella , L. Classen , R. Cocimano , A. Coleiro , S. Colonges , R. Coniglione , A. Cosquer , M. Costa , P. Coyle , A. Creusot , G. Cuttone , C. D'Amato , A. D'Amico , G. De Bonis , G. De Rosa , N. Deniskina , J. -J. Destelle , C. Distefano , F. Di Capua , C. Donzaud , D. Dornic , Q. Dorosti-Hasankiadeh , E. Drakopoulou , D. Drouhin , L. Drury , D. Durand , T. Eberl , D. Elsaesser , A. Enzenhöfer , P. Fermani , L. A. Fusco , D. Gajanana , T. Gal , S. Galatà , F. Garufi , M. Gebyehu , V. Giordano , N. Gizani , R. GraciaRuiz , K. Graf , R. Grasso , G. Grella , A. Grmek , R. Habel , H. van Haren , T. Heid , A. Heijboer , E. Heine , S. Henry , J. J. Hernández-Rey , B. Herold , M. A. Hevinga , M. van der Hoek , J. Hofestädt , J. Hogenbirk , C. Hugon , J. Hößl , M. Imbesi , C. W. James , P. Jansweijer , J. Jochum , M. de Jong , M. Jongen , M. Kadler , O. Kalekin , A. Kappes , E. Kappos , U. Katz , O. Kavatsyuk , P. Keller , G. Kieft , E. Koffeman , H. Kok , P. Kooijman , J. Koopstra , A. Korporaal , A. Kouchner , I. Kreykenbohm , V. Kulikovskiy , R. Lahmann , P. Lamare , G. Larosa , D. Lattuada , H. Le Provost , K. P. Leismüller , A. Leisos , D. Lenis , E. Leonora , M. LindseyClark , C. D. Llorens Alvarez , H. Löhner , A. Lonardo , S. Loucatos , F. Louis , E. Maccioni , K. Mannheim , K. Manolopoulos , A. Margiotta , O. Mariş , C. Markou , J. A. Martínez-Mora , A. Martini , R. Masullo , K. W. Melis , T. Michael , P. Migliozzi , E. Migneco , A. Miraglia , C. M. Mollo , M. Mongelli , M. Morganti , S. Mos , Y. Moudden , P. Musico , M. Musumeci , C. Nicolaou , C. A. Nicolau , A. Orlando , A. Orzelli , A. Papaikonomou , R. Papaleo , G. E. Păvălaş , H. Peek , C. Pellegrino , M. G. Pellegriti , C. Perrina , P. Piattelli , K. Pikounis , V. Popa , Th. Pradier , M. Priede , G. Pühlhofer , S. Pulvirenti , C. Racca , F. Raffaelli , N. Randazzo , P. A. Rapidis , P. Razis , D. Real , L. Resvanis , J. Reubelt , G. Riccobene , A. Rovelli , M. Saldaña , D. F. E. Samtleben , M. Sanguineti , A. Santangelo , P. Sapienza , J. Schmelling , J. Schnabel , V. Sciacca , M. Sedita , T. Seitz , I. Sgura , F. Simeone , V. Sipala , A. Spitaleri , M. Spurio , G. Stavropoulos , J. Steijger , T. Stolarczyk , D. Stransky , M. Taiuti , G. Terreni , D. Tézier , S. Théraube , L. F. Thompson , P. Timmer , L. Trasatti , A. Trovato , M. Tselengidou , A. Tsirigotis , S. Tzamarias , E. Tzamariudaki , B. Vallage , V. Van Elewyck , J. Vermeulen , P. Vernin , P. Vicini , S. Viola , D. Vivolo , P. Werneke , L. Wiggers , J. Wilms , E. de Wolf , R. H. L. van Wooning , E. Zonca , J. D. Zornoza , J. Zúñiga , A. Zwart

The alignment system for the muon spectrometer of the CMS detector comprises three independent subsystems of optical and analog position sensors. It aligns muon chambers with respect to each other and to the central silicon tracker. System…

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

A muon-flux measurement behind the beam dump of the J-PARC Hadron Experimental Facility was performed with a compact muon detector that can be inserted into a vertical observing hole with 81 mm in diameter which was dug underground. The…

Instrumentation and Detectors · Physics 2024-10-30 T. Matsumura , Y. Hirayama , G. Y. Lim , H. Nanjo , T. Nomura , K. Shiomi , H. Watanabe

Large liquid argon time projection chambers (LArTPCs) require stable and well-characterized delivery of ultraviolet (UV) light for in situ calibration of photosensors at cryogenic temperatures. This article reports bench-top and cryogenic…

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