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Related papers: Precision timing calorimetry with the CMS HGCAL

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High precision timing, high rate calorimeters, and radiation resistance are becoming an important issue in particle physics especially in Energy and Intensity Frontiers. We discuss doped Zinc Oxide (ZnO:Ga or GZO; ZnO:X where X is Al, Cu or…

Instrumentation and Detectors · Physics 2022-03-21 David R Winn , Y. Onel , B. Bilki

We have developed an algorithm dedicated to timing reconstruction in highly granular calorimeters(HGC). The performance of this algorithm is evaluated on an electromagnetic calorimeter (ECAL) with geometries comparable to the…

Instrumentation and Detectors · Physics 2024-09-09 Yuzhi Che , Vincent Boudry , Henri Videau , Muchen He , Manqi Ruan

The Tile Calorimeter (TileCal) is the hadronic calorimeter covering the most central region of the ATLAS experiment at the LHC. It is a key detector for the measurement of hadrons, jets, tau leptons and missing transverse energy. The…

Instrumentation and Detectors · Physics 2013-05-03 Bernardo Sotto-Maior Peralva

We report on several versions of the calibration and monitoring system dedicated to scintillator tile calorimeters built within the CALICE collaboration and intended for future linear collider experiments. Whereas the first, a 1 m3 analogue…

Instrumentation and Detectors · Physics 2019-08-15 Jaroslav Zalesak

As part of its HL-LHC upgrade program, the CMS collaboration is replacing its existing endcap calorimeters with a high-granularity calorimeter (CE). The new calorimeter is a sampling calorimeter with unprecedented transverse and…

Instrumentation and Detectors · Physics 2023-08-30 CMS HGCAL Collaboration

During the high-luminosity phase of the LHC (HL-LHC), planned to start around 2027, the accelerator is expected to deliver an instantaneous peak luminosity of up to $7.5\times10^{34}$ cm$^{-2}$s$^{-1}$. A total integrated luminosity of…

Instrumentation and Detectors · Physics 2020-06-17 The Tracker Group of the CMS Collaboration

The CALICE collaboration investigates diferent technology options for highly granular calorimeters for detectors at a future electron-positron collider. One of the devices constructed and tested by this collaboration is a 1m3 prototype of a…

Instrumentation and Detectors · Physics 2019-08-15 Jaroslav Zalesak

Particle Flow Algorithms (PFAs) have been proposed as a method of improving the jet energy resolution of future colliding beam detectors. PFAs require calorimeters with high granularity to enable three-dimensional imaging of events. The…

Instrumentation and Detectors · Physics 2019-08-13 Kurt Francis

High-time-resolution counters based on plastic scintillator with silicon photomultiplier (SiPM) readout have been developed for applications to high energy physics experiments for which relatively large-sized counters are required. We have…

Instrumentation and Detectors · Physics 2014-10-17 Paolo W. Cattaneo , Matteo De Gerone , Flavio Gatti , Miki Nishimura , Wataru Ootani , Massimo Rossella , Yusuke Uchiyama

To face the higher levels of radiation due to the 10-fold increase in integrated luminosity during the High-Luminosity LHC, the CMS detector will replace the current Calorimeter Endcap (CE) using the High-Granularity Calorimeter (HGCAL)…

An analog hadron calorimeter (AHCAL) prototype of 5.3 nuclear interaction lengths thickness has been constructed by members of the CALICE Collaboration. The AHCAL prototype consists of a 38-layer sandwich structure of steel plates and…

Instrumentation and Detectors · Physics 2016-12-13 C. Adloff , Y. Karyotakis , J. Repond , A. Brandt , H. Brown , K. De , C. Medina , J. Smith , J. Li , M. Sosebee , A. White , J. Yu , T. Buanes , G. Eigen , Y. Mikami , O. Miller , N. K. Watson , J. A. Wilson , T. Goto , G. Mavromanolakis , M. A. Thomson , D. R. Ward , W. Yan , D. Benchekroun , A. Hoummada , Y. Khoulaki , M. Oreglia , M. Benyamna , C. Cârloganu , P. Gay , J. Ha , G. C. Blazey , D. Chakraborty , A. Dyshkant , K. Francis , D. Hedin , G. Lima , V. Zutshi , V. A. Babkin , S. N. Bazylev , Yu. I. Fedotov , V. M. Slepnev , I. A. Tiapkin , S. V. Volgin , J. -Y. Hostachy , L. Morin , N. D?Ascenzo , U. Cornett , D. David , R. Fabbri , G. Falley , N. Feege , K. Gadow , E. Garutti , P. Göttlicher , T. Jung , S. Karstensen , V. Korbel , A. -I. Lucaci-Timoce , B. Lutz , N. Meyer , V. Morgunov , M. Reinecke , S. Schätzel , S. Schmidt , F. Sefkow , P. Smirnov , A. Vargas-Trevino , N. Wattimena , O. Wendt , M. Groll , R. -D. Heuer , S. Richter , J. Samson , A. Kaplan , H. -Ch. Schultz-Coulon , W. Shen , A. Tadday , B. Bilki , E. Norbeck , Y. Onel , E. J. Kim , G. Kim , D-W. Kim , K. Lee , S. C. Lee , K. Kawagoe , Y. Tamura , J. A. Ballin , P. D. Dauncey , A. -M. Magnan , H. Yilmaz , O. Zorba , V. Bartsch , M. Postranecky , M. Warren , M. Wing , M. Faucci Giannelli , M. G. Green , F. Salvatore , R. Kieffer , I. Laktineh , M. C Fouz , D. S. Bailey , R. J. Barlow , R. J. Thompson , M. Batouritski , O. Dvornikov , Yu. Shulhevich , N. Shumeiko , A. Solin , P. Starovoitov , V. Tchekhovski , A. Terletski , B. Bobchenko , M. Chadeeva , M. Danilov , O. Markin , R. Mizuk , V. Morgunov , E. Novikov , V. Rusinov , E. Tarkovsky , V. Andreev , N. Kirikova , A. Komar , V. Kozlov , P. Smirnov , Y. Soloviev , A. Terkulov , P. Buzhan , B. Dolgoshein , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , S. Smirnov , N. Baranova , E. Boos , L. Gladilin , D. Karmanov , M. Korolev , M. Merkin , A. Savin , A. Voronin , A. Topkar , A. Freyk , C. Kiesling , S. Lu , K. Prothmann , K. Seidel , F. Simon , C. Soldner , L. Weuste , B. Bouquet , S. Callier , P. Cornebise , F. Dulucq , J. Fleury , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , M. Ruan , N. Seguin-Moreau , F. Wicek , M. Anduze , V. Boudry , J-C. Brient , G. Gaycken , R. Cornat , D. Jeans , P. Mora de Freitas , G. Musat , M. Reinhard , A. Rougé , J-Ch. Vanel , H. Videau , K-H. Park , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , Yu. Arestov , V. Ammosov , B. Chuiko , V. Gapienko , Y. Gilitski , V. Koreshev , A. Semak , Yu. Sviridov , V. Zaets , B. Belhorma , M. Belmir , A. Baird , R. N. Halsall , S. W. Nam , I. H. Park , J. Yang , Jong-Seo Chai , Jong-Tae Kim , Geun-Bum Kim , Y. Kim , J. Kang , Y. -J. Kwon , Ilgoo Kim , Taeyun Lee , Jaehong Park , Jinho Sung , S. Itoh , K. Kotera , M. Nishiyama , T. Takeshita , S. Weber , C. Zeitnitz

First of its kind, the barrel section of the MIP Timing Detector is a large area timing detector based on LYSO:Ce crystals and SiPMs which are required to operate in an unprecedentedly harsh radiation environment (up to an integrated…

Instrumentation and Detectors · Physics 2025-08-14 F. Addesa , P. Akrap , A. Albert , B. Allmond , T. Anderson , J. Babbar , D. Baranyai , P. Barria , C. Basile , A. Benaglia , A. Benato , M. Benettoni , M. Besancon , N. Bez , S. Bhattacharya , R. Bianco , D. Blend , A. Boletti , A. Bornheim , R. Bugalho , A. Bulla , B. Cardwell , R. Carlin , M. Casarsa , F. Cetorelli , F. Cossutti , B. Cox , G. Da Molin , F. De Guio , K. De Leo , F. De Riggi , P. Debbins , D. Del Re , R. Delli Gatti , J. Dervan , P. Devouge , K. Dreimanis , O. M. Eberlins , F. Errico , E. Fernandez , W. Funk , A. Gaile , M. Gallinaro , R. Gargiulo , R. Gerosa , A. Ghezzi , B. Gyongyosi , Z. Hao , A. H. Heering , Z. Hu , R. Isocrate , M. Jose , A. Karneyeu , M. S. Kim , A. Krishna , B. Kronheim , O. K. Köseyan , A. Ledovskoy , L. Li , Z. Li , V. Lohezic , F. Lombardi , M. T. Lucchini , M. Malberti , Y. Mao , Y. Maravin , B. Marzocchi , D. Mazzaro , R. Menon Raghunandanan , P. Meridiani , C. Munoz Diaz , Y. Musienko , S. Nargelas , L. L. Narváez , C. Neu , G. Organtini , T. Orimoto , D. Osite , M. Paganoni , S. Palluotto , C. Palmer , N. Palmeri , F. Pandolfi , R. Paramatti , T. Pauletto , A. Perego , G. Pikurs , G. Pizzati , R. Plese , C. Quaranta , G. Reales Gutiérrez , N. Redaelli , S. Ronchi , R. Rossin , M. Ö. Sahin , F. Santanastasio , I. Schmidt , D. Sidiropoulos Kontos , T. Sievert , R. Silva , P. Simmerling , L. Soffi , P. Solanki , G. Sorrentino , M. Spiropulu , N. R. Strautnieks , X. Sun , D. D. Szabo , T. Tabarelli de Fatis , G. Tamulaitis , R. Taylor , M. Titov , M. Tosi , G. Trabucco , A. Tsirou , C. Tully , M. Turcato , B. Ujvari , J. Varela , F. Veronese , V. Vladimirov , J. Wang , M. Wayne , S. White , Z. Wu , J. W. Wulff , R. A. Wynne , L. Zhang , M. Zhang , G. Zilizi

The High Energy Physics (HEP) experiments, such as those at the Large Hadron Collider (LHC), traditionally consume large amounts of CPU cycles for detector simulations and data analysis, but rarely use compute accelerators such as GPUs. As…

High Energy Physics - Experiment · Physics 2022-03-17 Zhihua Dong , Heather Gray , Charles Leggett , Meifeng Lin , Vincent R. Pascuzzi , Kwangmin Yu

The general-purpose Compact Muon Solenoid (CMS) detector at the Large Hadron Collider (LHC) at CERN includes the hadronic calorimeter to register the energies of the charged and neutral hadrons produced in the proton-proton collisions at…

Instrumentation and Detectors · Physics 2024-01-09 Vyacheslav Klyukhin

The CALICE Analogue Hadron CALorimeter (AHCAL) at the International Linear Collider (ILC) is a high-granularity hadron calorimeter based on scintillator tiles readout by MPPCs. Toward the construction of ILC, the optimization of the AHCAL…

Instrumentation and Detectors · Physics 2019-04-08 Naoki Tsuji

The Large Hadron Collider (LHC) experiments ATLAS and CMS have established hybrid pixel detectors as the instrument of choice for particle tracking and vertexing in high rate and radiation environments, as they operate close to the LHC…

Instrumentation and Detectors · Physics 2018-06-27 Maurice Garcia-Sciveres , Norbert Wermes

The CMS-TOTEM Precision Proton Spectrometer (CT-PPS) is an approved project to add tracking and timing information at approximately $\pm$210~m from the interaction point around the CMS detector. It is designed to operate at high luminosity…

Instrumentation and Detectors · Physics 2017-04-05 Michele Gallinaro

TileCal, the central hadronic calorimeter of the ATLAS detector is composed of plastic scintillators interleaved by steel plates, and wavelength shifting optical fibres. The optical properties of these components are known to suffer from…

Instrumentation and Detectors · Physics 2019-05-06 R. Pedro

The SDHCAL technological prototype is a $1 \times 1 \times 1.3$~m$^3$ high-granularity Semi-Digital Hadronic CALorimeter using Glass Resistive Plate Chambers as sensitive medium. It is one of the two HCAL options considered by the ILD…

Instrumentation and Detectors · Physics 2016-08-03 Gérald Grenier
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