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In the ILD detector, HCAL is inside the coil. The HCAL is about 5 interaction length thick, and ECAL is about 1 interaction length thick. For example, an eighty GeV hadron, it is only 95% energy will be contained in ECAL plus HCAL. We need…

Instrumentation and Detectors · Physics 2019-08-13 Shaojun Lu

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

CEPC (Circular Electron and Positron Collider) is a large experiment facility proposed by Chinese particle physics community. One of its running option is being the Higgs factory. Calorimeter is the main part of this experiment to measure…

Instrumentation and Detectors · Physics 2019-09-04 Yu Wang , Shubin Liu , Changqing Feng , Zhongtao Shen , Junbin Zhang , Daojin Hong , Jianbei Liu , Yi Zhou

During the scheduled high luminosity upgrade of LHC, the world's largest particle physics accelerator at CERN, the position sensitive silicon detectors installed in the vertex and tracking part of the CMS experiment will face more intense…

The CALICE collaboration is currently developing an engineering prototype of an analog hadron calorimeter for a future linear collider detector. It is based on scintillating tiles that are individually read out by silicon photomultipliers.…

Instrumentation and Detectors · Physics 2019-08-14 Mark Terwort

A prototype silicon-tungsten electromagnetic calorimeter for an ILC detector was tested in 2007 at the CERN SPS test beam. Data were collected with electron and hadron beams in the energy range 8 to 80 GeV. The analysis described here…

Instrumentation and Detectors · Physics 2014-11-20 C. Adloff , Y. Karyotakis , J. Repond , J. Yu , G. Eigen , Y. Mikami , N. K. Watson , J. A. Wilson , T. Goto , G. Mavromanolakis , M. A. Thomson , D. R. Ward , W. Yan , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , A. Ribon , V. Uzhinskiy , M. Benyamna , C. Cârloganu , F. Fehr , P. Gay , G. C. Blazey , D. Chakraborty , A. Dyshkant , K. Francis , D. Hedin , J. G. Lima , V. Zutshi , J. -Y. Hostachy , K. Krastev , L. Morin , N. D'Ascenzo , U. Cornett , D. David , R. Fabbri , G. Falley , K. Gadow , E. Garutti , P. Göttlicher , T. Jung , S. Karstensen , A. -I. Lucaci-Timoce , B. Lutz , N. Meyer , V. Morgunov , M. Reinecke , F. Sefkow , P. Smirnov , A. Vargas-Trevino , N. Wattimena , O. Wendt , N. Feege , M. Groll , J. Haller , R. -D. Heuer , S. Morozov , 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 , P. D. Dauncey , A. -M. Magnan , H. Yilmaz , O. Zorba , V. Bartsch , M. Postranecky , M. Warren , M. Wing , M. G. Green , F. Salvatore , M. Bedjidian , R. Kieffer , I. Laktineh , M. -C. Fouz , D. S. Bailey , R. J. Barlow , M. Kelly , R. J. Thompson , M. Danilov , E. Tarkovsky , N. Baranova , D. Karmanov , M. Korolev , M. Merkin , A. Voronin , A. Frey , S. Lu , K. Seidel , F. Simon , C. Soldner , L. Weuste , J. Bonis , B. Bouquet , S. Callier , P. Cornebise , Ph. Doublet , M. Faucci Giannelli , J. Fleury , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , N. Seguin-Moreau , F. Wicek , M. Anduze , V. Boudry , J-C. Brient , G. Gaycken , D. Jeans , P. Mora de Freitas , G. Musat , M. Reinhard , A. Rougé , M. Ruan , J-Ch. Vanel , H. Videau , K-H. Park , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , M. Belmir , S. W. Nam , I. H. Park , J. Yang , Jong-Seo Chai , Jong-Tae Kim , Geun-Bum Kim , J. Kang , Y. -J. Kwon

As a future Higgs or Z factory, construction of the circular electron positron collider(CEPC) has been proposed to precisely measure Higgs bosons. A particle flow-oriented electromagnetic calorimeter (ECAL) and a hadronic calorimeter…

Instrumentation and Detectors · Physics 2020-06-17 YZ. Niu

The ILD Si-W ECAL is a sampling calorimeter with tungsten absorber and highly segmented silicon layers for the International Large Detector (ILD), one of the two detector concepts for the International Linear Collider. SKIROC2 is an ASIC…

Detectors at future $e^+e^-$ colliders need special calorimeters in the very forward region for a fast estimate and precise measurement of the luminosity, to improve the hermeticity and mask the central tracking detectors from backscattered…

High Energy Physics - Experiment · Physics 2023-01-24 Ivan Smiljanic

LumiCal is a sampling electromagnetic calorimeter designed for the precise measurement of integrated luminosity in electron positron linear collider experiments. The present report contains a description and results of the first beam test…

Instrumentation and Detectors · Physics 2019-08-13 Oleksandr Borysov

The Tile Calorimeter (TileCal) is one detector of the ATLAS experiment at the Large Hadron Collider (LHC). TileCal is a sampling calorimeter made of steel plates and plastic scintillators which are readout using approximately 10,000…

Instrumentation and Detectors · Physics 2019-09-04 F. Carrió , A. Valero

We present the results of the characterization of novel n-in-p planar pixel detectors, designed for the future upgrades of the ATLAS pixel system. N-in-p silicon devices are a promising candidate to replace the n-in-n sensors thanks to…

Instrumentation and Detectors · Physics 2012-03-01 A. Macchiolo , C. Gallrapp , A. La Rosa , R. Nisius , H. Pernegger , R. H. Richter , P. Weigell

The Circular Electron Positron Collider (CEPC) has been proposed to enable more thorough and precise measurements of the properties of Higgs, W, and Z bosons, as well as to search for new physics. In response to the stringent performance…

Detectors proposed for the International Linear Collider (ILC) incorporate a tungsten sampling calorimeter (`BeamCal') intended to reconstruct showers of electrons, positrons and photons that emerge from the interaction point of the…

Low Gain Avalanche Detectors (LGADs) are n-on-p silicon sensors with an extra p-layer below the collection electrode which provides signal amplification. When the primary electrons reach the amplification region new electron-hole pairs are…

The next generation of collider detectors will make full use of Particle Flow Algorithms, requiring high-precision tracking and full imaging calorimeters. The latter, thanks to granularity improvements by two to three orders of magnitude…

Instrumentation and Detectors · Physics 2022-11-15 Roman Pöschl

The CALICE collaboration has constructed highly granular electromagnetic and hadronic calorimeter prototypes to evaluate technologies for the use in detector systems at the future International Linear Collider. These calorimeters have been…

Instrumentation and Detectors · Physics 2019-08-13 Frank Simon

New generation high-energy physics experiments demand high precision tracking and accurate measurements of a large number of particles produced in the collisions of lementary particles and heavy-ions. Silicon-tungsten (Si-W) calorimeters…

The ALICE Collaboration completed the upgrade of the detector and is now commissioning for the beginning of the data taking during LHC Run 3. In parallel, R&D activities and simulation studies are being performed to define the future of the…

High Energy Physics - Experiment · Physics 2022-11-09 Domenico Colella , for the ALICE Collaboration