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This paper discusses the hadronic energy reconstruction of two combined electromagnetic and hadronic calorimeter systems using physics prototypes of the CALICE collaboration: the silicon-tungsten electromagnetic calorimeter (Si-W ECAL) and…

Instrumentation and Detectors · Physics 2018-07-01 Yasmine Israeli

Methods are presented for calibrating the hadron calorimeter system of the CMS detector at the LHC. The hadron calorimeters of the CMS experiment are sampling calorimeters of brass and scintillator, and are in the form of one central…

Instrumentation and Detectors · Physics 2020-05-07 CMS Collaboration

The calibration and performance of the LHCb Calorimeter system in Run 1 and 2 at the LHC are described. After a brief description of the sub-detectors and of their role in the trigger, the calibration methods used for each part of the…

The experimental requirements in near future accelerators (e.g. High Luminosity-LHC) has stimulated intense interest in development of detectors with high precision timing capabilities. With this as a goal, a new detection concept called…

The CALICE collaboration has constructed highly granular hadronic and electromagnetic calorimeter prototypes to evaluate technologies for the use in detector systems at a future Linear Collider. The hadron calorimeter uses 7608 small…

Instrumentation and Detectors · Physics 2010-06-21 Katja Seidel

The CMS endcap calorimeter upgrade for the High Luminosity LHC in 2027 uses silicon sensors to achieve radiation tolerance, with the further benefit of a very high readout granularity. Small scintillator tiles with individual SiPM readout…

Instrumentation and Detectors · Physics 2020-06-11 Antonio Di Pilato , Ziheng Chen , Felice Pantaleo , Marco Rovere

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

We present results on the performance of the first prototype of the CASTOR quartz-tungsten sampling calorimeter, to be installed in the very forward region of the CMS experiment at the LHC. This study includes GEANT Monte Carlo simulations…

Instrumentation and Detectors · Physics 2008-11-26 X. Aslanoglou , A. Cyz , N. Davis , D. d'Enterria , E. Gladysz-Dziadus , C. Kalfas , Y. Musienko , A. Kuznetsov , A. D. Panagiotou

The high-luminosity era of the LHC will offer greatly increased number of events for more precise Standard Model measurements and Beyond Standard Model searches, but will also pose unprecedented challenges to the detectors. To meet these…

High Energy Physics - Experiment · Physics 2025-12-09 Théo Cuisset

The original dual-readout calorimeter prototype (DREAM), constructed two decades ago, has proven instrumental in advancing our understanding of calorimetry. It has facilitated a multitude of breakthroughs by leveraging signals from…

Instrumentation and Detectors · Physics 2024-08-29 N. Akchurin , J. Cash , J. Damgov , X. Delashaw , K. Lamichhane , M. Harris , M. Kelley , S. Kunori , H. Mergate-Cacace , T. Peltola , O. Schneider , J. Sewell

To meet the stringent time calibration requirements for the Belle II experiment upgrade, particularly for its large-size KL and Muon Detector comprising tens of thousands of scintillator channels with time resolutions better than 100 ps, we…

Instrumentation and Detectors · Physics 2026-02-23 Ziyu Liu , Xiyang Wang , Shiming Zou , Xiaolong Wang , Junhao Yin , Minggang Zhao

Glass RPC detectors are an attractive candidate for the active part of a highly granular digital hadron calorimeter (DHCAL) at the ILC. A numerical study, based on the GEANT3 simulation package, of the performance of such a calorimeter is…

Instrumentation and Detectors · Physics 2007-05-23 A. Ghezzi , T. Tabarelli de Fatis , G. Tinti , M. Piccolo

The basic prototype of a tile hadron calorimeter (HCAL) for the International Linear Collider (ILC) has been realised and extensively tested. A major aspect of the proposed concept is the improvement of the jet energy resolution by…

Instrumentation and Detectors · Physics 2016-10-10 Aliakbar Ebrahimi

High performance calorimetry conducted at future hadron colliders, such as the FCC-hh, poses a significant challenge for applying current detector technologies due to unprecedented beam luminosities and radiation fields. Solutions include…

Next-generation high-energy electron-positron colliders, operating as Higgs factories, require an unprecedented jet energy resolution for precision measurements of Higgs and Z/W bosons. To address this challenge, a conceptual design is…

Instrumentation and Detectors · Physics 2026-03-10 Baohua Qi , Fangyi Guo , Shu Li , Yong Liu , Manqi Ruan , Weizheng Song , Shengsen Sun , Yifang Wang , Yuexin Wang , Haijun Yang , Yang Zhang , Zhiyu Zhao

The Tile hadronic calorimeter of the ATLAS detector has undergone extensive testing in the experimental hall since its installation in late 2005. The readout, control and calibration systems have been fully operational since 2007 and the…

Instrumentation and Detectors · Physics 2012-08-27 The ATLAS Collaboration

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

This paper presents results obtained with the combined CALICE Scintillator Electromagnetic Calorimeter, Analogue Hadronic Calorimeter and Tail Catcher & Muon Tracker, three high granularity scintillator-SiPM calorimeter prototypes. The…

Instrumentation and Detectors · Physics 2018-09-13 CALICE Collaboration , J. Repond , L. Xia , J. Apostolakis , G. Folger , V. Ivantchenko , A. Ribon , V. Uzhinskiy , D. Boumediene , V. Francais , G. C. Blazey , A. Dyshkant , K. Francis , V. Zutshi , O. Bach , E. Brianne , A. Ebrahimi , K. Gadow , P. Gttlicher , O. Hartbrich F. Krivan , K. Krüger , J. Kvasnicka , S. Lu , C. Neubüser , A. Provenza , M. Reinecke , F. Sefkow , S. Schuwalow , Y. Sudo , H. L. Tran , P. Buhmann , E. Garutti , S. Laurien , D. Lomidze , M. Matysek , A. Kaplan , H. -Ch. Schultz-Coulon , G. W. Wilson , D. Jeans , K. Kawagoe , I. Sekiya , T. Suehara , H. Yamashiro , T. Yoshioka , M. Wing , K. Kotera , M. Nishiyama , T. Sakuma , T. Takeshita , S. Tozuka , T. Tubokawa , S. Uozumi , E. Calvo Alamillo , M. C. Fouz , J. Marin , J. Navarrete , J. Puerta Pelayo , A. Verdugo , M. Chadeeva , M. Danilov , A. Drutskoy , E. Popova , V. Rusinov , E. Tarkovsky , L. Emberger , M. Gabriel , C. Graf , Y. Israeli , N. van der Kolk , F. Simon , M. Szalay , H. Windel , S. Bilokin J. Bonis , R. Pöschl , A. Irles , A. Thiebault , F. Richard , D. Zerwas , M. Anduze , V. Balagura , E. Becheva , V. Boudry , J-C. Brient , R. Cornat , E. Edy , M. Frotin F. Gastaldi , B. Li , F. Magniette , J. Nanni , M. Rubio-Roy , K. Shpak , T. H. Tran , H. Videau , J. Cvach , M. Janata , M. Kovalcuk , I. Polak , J. Smolik , V. Vrba , J. Zalesak , J. Zuklin , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , A. Elkhalii , M. Götze , C. Zeitnitz

The high frequency primary power standard is univocally realized by means of a coaxial microcalorimeter, at least up to 40 GHz. The coaxial microcalorimeter is a broadband measurement system adjusted for effec-tive efficiency measurement of…

Instrumentation and Detectors · Physics 2021-03-09 Luciano Brunetti , Luca Oberto , Marco Sellone