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At the High Luminosity LHC (HL-LHC), the CMS experiment will need to operate at up to 200 interactions per 25 ns beam crossing time and with up to 4000 fb-1 of integrated luminosity. To achieve the physics goals the experiment needs to…

Instrumentation and Detectors · Physics 2022-12-21 A. La Rosa , I. Ahmed , J. Almeida , G. Blanchot , S. Cooperstein , I. Dominguez , A. Honma , M. Kovacs , A. Zografos

The CALICE Semi-Digital Hadronic Calorimeter (SDHCAL) prototype, built in 2011, was exposed to beams of hadrons, electrons and muons in two short periods in 2012 on two different beam lines of the CERN SPS. The prototype with its 48 active…

Instrumentation and Detectors · Physics 2016-05-04 V. Buridon , C. Combaret , L. Caponetto , R. Eté , G. Garillot , G. Grenier , R. Han , J. C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , J. Berenguer Antequera , E. Calvo Alamillo , M. -C. Fouz , J. Marin , J. Puerta-Pelayo , A. Verdugo , E. Cortina Gil , S. Mannai , S. Cauwenbergh , M. Tytgat , A. Pingault , N. Zaganidis , M. Anduze , V. Balagura , K. Belkadhi , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , Y. Haddad , M. Ruan , K. Shpak , H. Videau , D. Yu , S. Callier , S. Conforti di Lorenzo , F. Dulucq , G. Martin-Chassard , Ch. de la Taille , L. Raux , N. Seguin-Moreau , D. Boumediene , C. Carloganu , V. Français , J. Bonis , B. Bouquet , P. Cornebise , Ph. Doublet , M. Faucci-Giannelli , T. Frisson , G. Guilhem , H. Li , F. Richard , R. Pöschl , J. Rouëné , F. Wicek , Z. Zhang , Z. Deng , Y. Li , Y. Wang , Q. Yue , Z. Yang , G. Cho , D-W. Kim , S. C. Lee , W. Park , S. Vallecorsa , E. Brianne , A. Ebrahimi , K. Gadow , P. Göttlicher , C. Günter , O. Hartbrich , B. Hermberg , A. Irles , F. Krivan , K. Krüger , J. Kvasnicka , S. Lu , B. Lutz , V. Morgunov , C. Neubüser A. Provenza , M. Reinecke , F. Sefkow , S. Schuwalow , H. L. Tran , E. Garutti , S. Laurien , M. Matysek , M. Ramilli , S. Schroeder , B. Bilki , E. Norbeck , D. Northacker , Y. Onel , N. Kirikova , V. Kozlov , P. Smirnov , Y. Soloviev , M. Chadeeva , M. Danilov , M. Gabriel , P. Goecke , C. Kiesling , N. van der Kolk , F. Simon , C. Soldner , M. Szalay , L. Weuste , D. Jeans , S. Komamiya , H. Nakanishi , D. Benchekroun , A. Hoummada , Y. Khoulaki

With the LHC successfully collecting data at 7 TeV, plans are actively advancing for a series of upgrades leading eventually to about five times the LHC design-luminosity some 10-years from now in the High-Luminosity LHC (HL-LHC) project.…

Instrumentation and Detectors · Physics 2015-06-03 Peter Vankov

This talk reports on recent progress concerning the development of a Digital Hadron Calorimeter with Resistive Plate Chambers as active elements. After the successful testing of a Digital Hadron Calorimeter prototype, the DHCAL, in the…

Instrumentation and Detectors · Physics 2013-12-16 J. Repond

The technological prototype of the CALICE highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) was tested in a beam at DESY in 2017. The setup comprised seven layers of silicon sensors. Each layer comprised four sensors,…

A highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) is the reference design of the ECAL for International Large Detector concept, one of the two detector concepts for the future International Linear Collider.…

Instrumentation and Detectors · Physics 2021-09-03 Fabricio Jimenez Morales

The next upgrade of the Large Hadron Collider (LHC) is planned from 2026 when the collider will move to its High Luminosity phase (HL-LHC). The CMS detector needs to be substantially upgraded during this period to exploit the fourfold…

Instrumentation and Detectors · Physics 2023-02-01 Tamas Almos Vami , Morris Swartz

The Large Hadron Collider (LHC) at CERN will undergo an upgrade in order to increase its luminosity to $7.5 \times 10^{34}$ cm$^{-2}$s$^{-1}$. The increased luminosity during this High-Luminosity running phase (HL-LHC), starting around…

Instrumentation and Detectors · Physics 2023-09-04 The Tracker Group of the CMS Collaboration

Maintaining the required performance of the CMS electromagnetic calorimeter (ECAL) barrel at the High-Luminosity Large Hadron Collider (HL-LHC) requires the replacement of the entire on-detector electronics. 12240 new very front end (VFE)…

Instrumentation and Detectors · Physics 2023-11-06 W. Lustermann , D. Abadjiev , G. Dissertori , M. Dejardin , T. Gadek , L. T. Martin , K. Stachon

The Circular Electron Positron Collider (CEPC) is a next-generation electron$-$positron collider proposed for the precise measurement of the properties of the Higgs boson. To emphasize boson separation and jet reconstruction, the baseline…

An extended version of the CALICE silicon-tungsten ECAL was tested in November 2021 at the DESY beam test facility. With 15 active layers, it featured some with a thin PCB design, and a new compact DAQ system handling all layers in a common…

High Energy Physics - Experiment · Physics 2023-04-28 Vincent Boudry

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

Chromatic calorimetry (CCAL) analyses particle detection by utilizing scintillators with distinct emission wavelengths to measure the longitudinal energy deposition of particle showers in high-energy physics, improving particle…

High Energy Physics - Experiment · Physics 2025-09-12 Devanshi Arora

The FCAL collaboration is preparing large-scale prototypes of special calorimeters to be used in the very forward region at future electron-positron colliders for a precise measurement of integrated luminosity and for instant luminosity…

Instrumentation and Detectors · Physics 2021-01-22 Maryna Borysova

Hybrid ECAL is a cost-conscious option of electromagnetic calorimeter (ECAL) for particle flow calorimetry to be used in a detector of International Linear Collider (ILC). It is a combination of silicon-tungsten ECAL, which realizes high…

Instrumentation and Detectors · Physics 2015-03-31 T. Suehara , H. Hirai , H. Sumida , H. Ueno , Y. Sudo , T. Yoshioka , K. Kawagoe

The CALICE collaboration is developing an engineering prototype of an analog hadron calorimeter for a future linear collider detector. The prototype has to prove the feasibility of building a realistic detector with fully integrated…

Instrumentation and Detectors · Physics 2019-08-13 Oskar Hartbrich , Mark Terwort

The reliability of bump connection structures has become a critical aspect of future silicon detectors for particle physics. The High Granularity Timing Detector (HGTD) for the ATLAS experiment at the High-Luminosity Large Hadron Collider…

Instrumentation and Detectors · Physics 2025-09-18 Y. Li , A. Aboulhorma , M. Ait Tamlihat , H. M. Alfanda , N. Atanov , O. Atanova , I. Azzouzi , J. Barreiro Guimarães Da Costa , T. Beau , D. Benchekroun , F. Bendebba , Y. Bimgdi , A. Blot , A. Boikov , J. Bonis , D. Boumediene , C. Brito , A. S. Brogna , A. M. Burger , L. Cadamuro , Y. Cai , N. Cartalade , R. Casanova Mohr , Y. Che , X. Chen , R. Cherkaoui El Moursli , E. Y. S. Chow , L. D. Corpe , C. G. Crozatier , L. D'Eramo , S. Dahbi , D. Dannheim , G. Daubard , Y. I. Davydov , C. de La Taille , J. Debevc , Y. Degerli , E. Delagnes , F. Deliot , M. Dhellot , G. Di Gregorio , P. Dinaucourt , P. J. Dos Santos De Assis , C. Duan , O. Duarte , F. Dulucq , J. Ehrecke , Y. El Ghazali , A. El Moussaouy , R. Estevam , A. Falou , L. Fan , Z. Fan , Y. Fan , K. Farman , F. Fassi , Y. Feng , M. Ferreira , F. Filthaut , F. Fischer , J. Fu , P. Fusté , G. Gaspar De Andrade , Z. Ge , R. Gonçalo , M. Gouighri , S. Grinstein , K. Gritsay , F. Guilloux , S. Guindon , A. Haddad , S. E. D. Hammoud , L. Han , A. M. Henriques Correia , M. Hidaoui , B. Hiti , J. Hofner , S. Hou , P. J. Hsu , K. Hu , Y. Huang , X. Huang , C. Insa , J. Jeglot , X. Jia , G. Kramberger , M. Kuriyama , B. Y. Ky , D. Lacour , A. Lafarge , B. Lakssir , A. Lantheaume , D. Laporte , A. Leopold , M. Li , S. Li , L. Li , S. Li , H. Li , Z. Li , Z. Liang , S. Liang , M. A. Lisboa Leite , B. Liu , Y. L. Liu , K. Liu , K. Liu , Y. W. Liu , M. Lu , Y. J. Lu , F. L. Lucio Alves , F. Lyu , X. Ma , K. Ma , D. Macina , R. Madar , N. Makovec , S. Malyukov , I. Mandić , T. Manoussos , S. Manzoni , G. Martin-Chassard , F. Martins , L. Masetti , R. Mazini , E. Mazzeo , R. Menegasso , J. -P. Meyer , Y. Miao , A. Migayron , M. Mihovilovic , M. Milovanovic , M. Missio , V. Moskalenko , N. Mouadili , A. Moussa , I. Nikolic-Audit , C. C. Ohm , H. Okawa , S. Okkerman , M. Ouchrif , C. Pénélaud , A. Parreira , B. Pascual Dias , J. Pinol Bel , P. -O. Puhl , M. Puklavec , M. Qi , J. Qin , H. Ren , H. Riani , S. Ridaouni , V. Rogozin , L. Royer , F. Rudnyckyj , E. F. Saad , G. T. Saito , A. Salem , H. Santos , Ph. Schwemling , N. Seguin-Moreau , L. Serin , R. P. Serrano Fernandez , Q. Sha , A. Shaikovskii , L. Shan , R. Shen , X. Shi , P. Skomina , H. Smitmanns , H. L. Snoek , A. P. Soulier , A. Stein , H. Stenzel , J. Strandberg , W. Sun , X. Sun , Y. Sun , Y. Tan , K. Tariq , Y. Tayalati , S. Terzo , A. Torrento Coello , S. Trincaz-Duvoid , U. M. Vande Voorde , I. Velkovska , R. P. Vieira , L. A. Vieira Lopes , A. Visibile , J. Wan , W. Wang , C. Wang , Y. Wang , Y. Wang , A. Wang , T. Wang , T. Wang , S. M. Wang , Q. Weitzel , J. Wu , W. Wu , Y. Wu , M. Wu , L. Xia , H. Xu , D. Xu , L. Xu , Z. Yan , X. Yang , X. Yang , H. Yang , H. Yang , J. Ye , I. Youbi , J. Yuan , I. Zahir , H. Zeng , T. Zhang , J. Zhang , Z. Zhang , L. Zhang , D. Zhang , M. Zhao , Z. Zhao , X. Zheng , Z. Zhou , Y. Zhu , X. Zhuang

A highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) is the reference design of the ECAL of the International Large Detector (ILD) concept, one of the two detector concepts for the detector(s) at the future…

Instrumentation and Detectors · Physics 2020-06-17 D. Breton , A. Irles , J. Jeglot , J. Maalmi , R. Pöschl , D. Zerwas

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