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Nuclear physics experiments are always in need of more and more advanced detection systems. During the last years relevant technological developments have come out with many improvements in terms of performance and compactness of detector…

Instrumentation and Detectors · Physics 2021-01-26 Paolo Finocchiaro

In this paper we address a class of ``ultimate'' generation experiments for the search of CP-violation in neutrino oscillations. Neutrino factories require large magnetized detectors. New generation superbeams or beta-beams need giant…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Rubbia

We discuss the use of Low Gain Avalanche (LGAD) silicon detectors for two specific applications, namely measuring cosmic rays in space in collaboration with NASA] and beam properties and received doses for patients undergoing cancer…

High Energy Physics - Experiment · Physics 2023-11-09 C. Royon , F. Gautier

Thin Film technology has widespread applications in everyday electronics, notably Liquid Crystal Display screens, solar cells, and organic light emitting diodes. We explore the potential of this technology as charged particle radiation…

Instrumentation and Detectors · Physics 2014-11-10 J. Metcalfe , I. Mejia , J. Murphy , M. Quevedo , L. Smith , J. Alvarado , B. Gnade , H. Takai

The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be…

High Energy Physics - Experiment · Physics 2007-05-23 Felicitas Pauss , Michael Dittmar

3D silicon detectors, in which the electrodes penetrate the sensor bulk perpendicular to the surface, have recently undergone a rapid development from R\&D over industrialisation to their first installation in a real high-energy-physics…

Instrumentation and Detectors · Physics 2015-11-09 Jörn Lange

The nature of dark matter and properties of neutrinos are among the most pressing issues in contemporary particle physics. The dual-phase xenon time-projection chamber is the leading technology to cover the available parameter space for…

Instrumentation and Detectors · Physics 2023-02-10 J. Aalbers , K. Abe , V. Aerne , F. Agostini , S. Ahmed Maouloud , D. S. Akerib , D. Yu. Akimov , J. Akshat , A. K. Al Musalhi , F. Alder , S. K. Alsum , L. Althueser , C. S. Amarasinghe , F. D. Amaro , A. Ames , T. J. Anderson , B. Andrieu , N. Angelides , E. Angelino , J. Angevaare , V. C. Antochi , D. Antón Martin , B. Antunovic , E. Aprile , H. M. Araújo , J. E. Armstrong , F. Arneodo , M. Arthurs , P. Asadi , S. Baek , X. Bai , D. Bajpai , A. Baker , J. Balajthy , S. Balashov , M. Balzer , A. Bandyopadhyay , J. Bang , E. Barberio , J. W. Bargemann , L. Baudis , D. Bauer , D. Baur , A. Baxter , A. L. Baxter , M. Bazyk , K. Beattie , J. Behrens , N. F. Bell , L. Bellagamba , P. Beltrame , M. Benabderrahmane , E. P. Bernard , G. F. Bertone , P. Bhattacharjee , A. Bhatti , A. Biekert , T. P. Biesiadzinski , A. R. Binau , R. Biondi , Y. Biondi , H. J. Birch , F. Bishara , A. Bismark , C. Blanco , G. M. Blockinger , E. Bodnia , C. Boehm , A. I. Bolozdynya , P. D. Bolton , S. Bottaro , C. Bourgeois , B. Boxer , P. Brás , A. Breskin , P. A. Breur , C. A. J. Brew , J. Brod , E. Brookes , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , T. K. Bui , S. Burdin , S. Buse , J. K. Busenitz , D. Buttazzo , M. Buuck , A. Buzulutskov , R. Cabrita , C. Cai , D. Cai , C. Capelli , J. M. R. Cardoso , M. C. Carmona-Benitez , M. Cascella , R. Catena , S. Chakraborty , C. Chan , S. Chang , A. Chauvin , A. Chawla , H. Chen , V. Chepel , N. I. Chott , D. Cichon , A. Cimental Chavez , B. Cimmino , M. Clark , R. T. Co , A. P. Colijn , J. Conrad , M. V. Converse , M. Costa , A. Cottle , G. Cox , O. Creaner , J. J. Cuenca Garcia , J. P. Cussonneau , J. E. Cutter , C. E. Dahl , V. D'Andrea , A. David , M. P. Decowski , J. B. Dent , F. F. Deppisch , L. de Viveiros , P. Di Gangi , A. Di Giovanni , S. Di Pede , J. Dierle , S. Diglio , J. E. Y. Dobson , M. Doerenkamp , D. Douillet , G. Drexlin , E. Druszkiewicz , D. Dunsky , K. Eitel , A. Elykov , T. Emken , R. Engel , S. R. Eriksen , M. Fairbairn , A. Fan , J. J. Fan , S. J. Farrell , S. Fayer , N. M. Fearon , A. Ferella , C. Ferrari , A. Fieguth , A. Fieguth , S. Fiorucci , H. Fischer , H. Flaecher , M. Flierman , T. Florek , R. Foot , P. J. Fox , R. Franceschini , E. D. Fraser , C. S. Frenk , S. Frohlich , T. Fruth , W. Fulgione , C. Fuselli , P. Gaemers , R. Gaior , R. J. Gaitskell , M. Galloway , F. Gao , I. Garcia Garcia , J. Genovesi , C. Ghag , S. Ghosh , E. Gibson , W. Gil , D. Giovagnoli , F. Girard , R. Glade-Beucke , F. Glück , S. Gokhale , A. de Gouvêa , L. Gráf , L. Grandi , J. Grigat , B. Grinstein , M. G. D. van der Grinten , R. Grössle , H. Guan , M. Guida , R. Gumbsheimer , C. B. Gwilliam , C. R. Hall , L. J. Hall , R. Hammann , K. Han , V. Hannen , S. Hansmann-Menzemer , R. Harata , S. P. Hardin , E. Hardy , C. A. Hardy , K. Harigaya , R. Harnik , S. J. Haselschwardt , M. Hernandez , S. A. Hertel , A. Higuera , C. Hils , S. Hochrein , L. Hoetzsch , M. Hoferichter , N. Hood , D. Hooper , M. Horn , J. Howlett , D. Q. Huang , Y. Huang , D. Hunt , M. Iacovacci , G. Iaquaniello , R. Ide , C. M. Ignarra , G. Iloglu , Y. Itow , E. Jacquet , O. Jahangir , J. Jakob , R. S. James , A. Jansen , W. Ji , X. Ji , F. Joerg , J. Johnson , A. Joy , A. C. Kaboth , A. C. Kamaha , K. Kanezaki , K. Kar , M. Kara , N. Kato , P. Kavrigin , S. Kazama , A. W. Keaveney , J. Kellerer , D. Khaitan , A. Khazov , G. Khundzakishvili , I. Khurana , B. Kilminster , M. Kleifges , P. Ko , M. Kobayashi , M. Kobayashi , D. Kodroff , G. Koltmann , A. Kopec , A. Kopmann , J. Kopp , L. Korley , V. N. Kornoukhov , E. V. Korolkova , H. Kraus , L. M. Krauss , S. Kravitz , L. Kreczko , V. A. Kudryavtsev , F. Kuger , J. Kumar , B. López Paredes , L. LaCascio , Q. Laine , H. Landsman , R. F. Lang , E. A. Leason , J. Lee , D. S. Leonard , K. T. Lesko , L. Levinson , C. Levy , I. Li , S. C. Li , T. Li , S. Liang , C. S. Liebenthal , J. Lin , Q. Lin , S. Lindemann , M. Lindner , A. Lindote , R. Linehan , W. H. Lippincott , X. Liu , K. Liu , J. Liu , J. Loizeau , F. Lombardi , J. Long , M. I. Lopes , E. Lopez Asamar , W. Lorenzon , C. Lu , S. Luitz , Y. Ma , P. A. N. Machado , C. Macolino , T. Maeda , J. Mahlstedt , P. A. Majewski , A. Manalaysay , A. Mancuso , L. Manenti , A. Manfredini , R. L. Mannino , N. Marangou , J. March-Russell , F. Marignetti , T. Marrodán Undagoitia , K. Martens , R. Martin , I. Martinez-Soler , J. Masbou , D. Masson , E. Masson , S. Mastroianni , M. Mastronardi , J. A. Matias-Lopes , M. E. McCarthy , N. McFadden , E. McGinness , D. N. McKinsey , J. McLaughlin , K. McMichael , P. Meinhardt , J. Menéndez , Y. Meng , M. Messina , R. Midha , D. Milisavljevic , E. H. Miller , B. Milosevic , S. Milutinovic , S. A. Mitra , K. Miuchi , E. Mizrachi , K. Mizukoshi , A. Molinario , A. Monte , C. M. B. Monteiro , M. E. Monzani , J. S. Moore , K. Morå , J. A. Morad , J. D. Morales Mendoza , S. Moriyama , E. Morrison , E. Morteau , Y. Mosbacher , B. J. Mount , J. Mueller , A. St. J. Murphy , M. Murra , D. Naim , S. Nakamura , E. Nash , N. Navaieelavasani , A. Naylor , C. Nedlik , H. N. Nelson , F. Neves , J. L. Newstead , K. Ni , J. A. Nikoleyczik , V. Niro , U. G. Oberlack , M. Obradovic , K. Odgers , C. A. J. O'Hare , P. Oikonomou , I. Olcina , K. Oliver-Mallory , A. Oranday , J. Orpwood , I. Ostrovskiy , K. Ozaki , B. Paetsch , S. Pal , J. Palacio , K. J. Palladino , J. Palmer , P. Panci , M. Pandurovic , A. Parlati , N. Parveen , S. J. Patton , V. Pěč , Q. Pellegrini , B. Penning , G. Pereira , R. Peres , Y. Perez-Gonzalez , E. Perry , T. Pershing , R. Petrossian-Byrne , J. Pienaar , A. Piepke , G. Pieramico , M. Pierre , M. Piotter , V. Pizella , G. Plante , T. Pollmann , D. Porzio , J. Qi , Y. Qie , J. Qin , N. Raj , M. Rajado Silva , K. Ramanathan , D. Ramírez García , J. Ravanis , L. Redard-Jacot , D. Redigolo , S. Reichard , J. Reichenbacher , C. A. Rhyne , A. Richards , Q. Riffard , G. R. C. 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Yuan , G. Zavattini , S. Zerbo , Y. Zhang , M. Zhong , N. Zhou , X. Zhou , T. Zhu , Y. Zhu , Y. Zhuang , J. P. Zopounidis , K. Zuber , J. Zupan

The Liquid Argon Time Projection Chambers (LArTPCs) are a choice for the next generation of large neutrino detectors due to their optimal performance in particle tracking and calorimetry. The detection of Argon scintillation light plays a…

Instrumentation and Detectors · Physics 2018-04-18 G. Cancelo , F. Cavanna , C. O. Escobar , E. Kemp , A. A. Machado , A. Para , E. Segreto , D. Totani , D. Warner

The ArDM project aims at operating a large noble liquid detector to search for direct evidence of Weakly Interacting Massive Particles (WIMP) as Dark Matter in the universe. Background sources relevant to ton-scale liquid and gaseous argon…

High Energy Physics - Phenomenology · Physics 2016-11-09 L. Kaufmann , A. Rubbia

The capabilities of liquid argon time projection chambers (LArTPCs) to reconstruct the spatial and calorimetric information of neutrino events have made them the detectors of choice in a number of experiments, specifically those looking to…

Liquid argon time projection chambers have emerged as a competitive technology for detecting solar neutrinos. The SoLAr collaboration was formed to explore argon detectors with pixelated light and charge readout, aiming for high detection…

We have developed a new detector of photons and charged particles- a hole-type structure with electrodes made of a double layered resistive material: a thin low resistive layer coated with a layer having a much higher resistivity. One of…

Instrumentation and Detectors · Physics 2008-11-26 G. Charpak , P. Benaben , P. Breuil , A. Di Mauro , P. Martinengo , V. Peskov

The Dark Matter part of the universe presumably consists of WIMPs (Weakly Interacting Massive Particles). The ArDM project aims at measuring signals induced by WIMPs in a liquid argon detector. A 1-ton prototype is currently developed with…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Kaufmann , A. Rubbia

A search for millicharged particles, a simple extension of the standard model, has been performed with the ArgoNeuT detector exposed to the Neutrinos at the Main Injector beam at Fermilab. The ArgoNeuT Liquid Argon Time Projection Chamber…

It is widely accepted that the next lepton collider beyond a Higgs factory would require center-of-mass energy of the order of up to 15 TeV. Since, given reasonable space and cost restrictions, conventional accelerator technology reaches…

Pixel vertex detectors are THE instrument of choice for the tracking of charged particles close to the interaction point at the LHC. Hybrid pixel detectors, in which sensor and read-out IC are separate entities, constitute the present state…

Instrumentation and Detectors · Physics 2009-09-29 Norbert Wermes

The ICARUS T600, a liquid argon time projection chamber (LAr-TPC) detector mainly devoted to neutrino physics, underwent a major overhauling at CERN in 2016-2017, which included also a new design of the read-out electronics, in view of its…

Experiments searching for weak interacting massive particles with noble gases such as liquid argon require very low detection thresholds for nuclear recoils. A determination of the scintillation efficiency is crucial to quantify the…

Instrumentation and Detectors · Physics 2015-09-02 W. Creus , Y. Allkofer , C. Amsler , A. D. Ferella , J. Rochet , L. Scotto-Lavina , M. Walter

The ATLAS Inner Detector is responsible for particle tracking in ATLAS experiment at CERN Large Hadron Collider (LHC) and comprises silicon and gas based detectors. The combination of both silicon and gas based detectors provides high…

Instrumentation and Detectors · Physics 2019-08-13 Ewa Stanecka

The Deep Underground Neutrino Experiment (DUNE) will be the first mega-science program on the US soil and will shade light on some of the open questions in neutrino physics. The experiment foresees the realization of an intense neutrino…

Instrumentation and Detectors · Physics 2026-02-17 H. V. Souza