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Excellent jet energy measurement is important at the International Linear Collider (ILC) because most of interesting physics processes decay into multi-jet final states. We employ a particle flow method to reconstruct particles, hence…

The long slab is a new prototype for the SiW-Ecal, a silicon tungsten electromagnetic calorimeter for the ILD detector of the future International Linear Collider. This new prototype has been designed to demonstrate the ability to build a…

The foreseen upgrade of the LHC to its high luminosity phase (HL-LHC), will maximize the physics potential of the facility. The upgrade is expected to increase the instantaneous luminosity by a factor of 5 and deliver an integrated…

Instrumentation and Detectors · Physics 2018-12-19 Timo Peltola

The replacement of the existing endcap calorimeter in the Compact Muon Solenoid (CMS) detector for the high-luminosity LHC (HL-LHC), scheduled for 2027, will be a high granularity calorimeter. It will provide detailed position, energy, and…

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)…

The CALICE Semi-Digital Hadron Calorimeter technological prototype completed in 2011 is a sampling calorimeter using Glass Resistive Plate Chamber (GRPC) detectors as the active medium. This technology is one of the two options proposed for…

We outline a physics program at Fermilab that would significantly improve our ability to understand the behavior of hadronic showers in calorimeters. This would involve a two-pronged approach designed to measure particle production cross…

Instrumentation and Detectors · Physics 2007-09-07 Rajendran Raja

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)…

The HL-LHC will challenge the detectors with a nearly 10-fold increase in integrated luminosity compared to the previous LHC runs combined, thus the CMS detector will be upgraded to face the higher levels of radiation and the larger amounts…

Instrumentation and Detectors · Physics 2026-03-10 CMS HGCAL 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

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 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

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 instant luminosity measurement and a precise measurement of integrated…

Instrumentation and Detectors · Physics 2022-08-10 Veta Ghenescu

This paper describes a comprehensive experimental study on viability and prospects for the measurement of electroweak observables in $e^{+}e^{-}\rightarrow b\bar{b}$ and $e^{+}e^{-}\rightarrow c\bar{c}$ processes at the International Linear…

High Energy Physics - Experiment · Physics 2023-12-20 A. Irles , R. Pöschl , F. Richard

The upgrade of the CMS experiment for the high luminosity operation of the LHC comprises the replacement of the current endcap calorimeter by a high granularity sampling calorimeter (HGCAL). The electromagnetic section of the HGCAL is based…

Instrumentation and Detectors · Physics 2023-05-30 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , M. Alhusseini , J. Alison , J. P. Figueiredo de sa Sousa de Almeida , P. G. Dias de Almeida , A. Alpana , M. Alyari , I. Andreev , U. Aras , P. Aspell , I. O. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , S. Banerjee , P. DeBarbaro , P. Bargassa , D. Barney , F. Beaudette , F. Beaujean , E. Becheva , A. Becker , P. Behera , A. Belloni , T. Bergauer , M. El Berni , M. Besancon , S. Bhattacharya , S. Bhattacharya , D. Bhowmik , B. Bilki , S. Bilokin , G. C. Blazey , F. Blekman , P. Bloch , A. Bodek , M. Bonanomi , J. Bonis , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , N. Bower , D. Braga , L. Brennan , E. Brianne , E. Brondolin , P. Bryant , E. Buhmann , P. Buhmann , A. Butler-Nalin , O. Bychkova , S. Callier , D. Calvet , K. Canderan , K. Cankocak , X. Cao , A. Cappati , B. Caraway , S. Caregari , C. Carty , A. Cauchois , L. Ceard , D. S. Cerci , S. Cerci , G. Cerminara , M. Chadeeva , N. Charitonidis , R. Chatterjee , J. A. Chen , Y. M. Chen , H. J. Cheng , K. Y. Cheng , H. Cheung , D. Chokheli , M. Cipriani , D. Čoko , F. Couderc , E. Cuba , M. Danilov , D. Dannheim , W. Daoud , I. Das , P. Dauncey , G. Davies , O. Davignon , E. Day , P. Debbins , M. M. Defranchis , E. Delagnes , Z. Demiragli , U. Demirbas , G. Derylo , D. Diaz , L. Diehl , P. Dinaucourt , G. G. Dincer , J. Dittmann , M. Dragicevic , S. Dugad , F. Dulucq , I. Dumanoglu , M. Dünser , S. Dutta , V. Dutta , T. K. Edberg , F. Elias , L. Emberger , S. C. Eno , Yu. Ershov , S. Extier , F. Fahim , C. Fallon , K. Sarbandi Fard , G. Fedi , L. Ferragina , L. Forthomme , E. Frahm , G. Franzoni , J. Freeman , T. French , K. Gadow , P. Gandhi , S. Ganjour , X. Gao , M. T. Ramos Garcia , A. Garcia-Bellido , E. Garutti , F. Gastaldi , D. Gastler , Z. Gecse , A. Germer , H. Gerwig , O. Gevin , S. Ghosh , A. Gilbert , W. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , B. Gonultas , N. Gorbounov , P. Göttlicher , L. Gouskos , C. Graf , A. B. Gray , C. Grieco , S. Gr\"önroos , Y. Gu , F. Guilloux , E. Gurpinar Guler , Y. Guler , E. Gülmez , J. Guo , H. Gutti , A. Hakimi , M. Hammer , O. Hartbrich , H. M. Hassanshahi , K. Hatakeyama , E. Hazen , A. Heering , V. Hegde , U. Heintz , D. Heuchel , N. Hinton , J. Hirschauer , J. Hoff , W. S. Hou , X. Hou , H. Hua , S. Huck , A. Hussain , J. Incandela , A. Irles , A. Irshad , C. Isik , S. Jain , J. Jaroslavceva , H. R. Jheng , U. Joshi , K. Kaadze , V. Kachanov , L. Kalipoliti , A. Kaminskiy , A. R. Kanuganti , Y. W. Kao , A. Kapoor , O. Kara , A. Karneyeu , O. Kałuzińska , M. Kaya , O. Kaya , Y. Kazhykharim , F. A. Khan , A. Khukhunaishvili , J. Kieseler , M. Kilpatrick , S. Kim , K. Koetz , T. Kolberg , M. Komm , O. K. Köseyan , V. Kraus , M. Krawczyk , K. Kristiansen , A. Kristić , M. Krohn , B. Kronheim , K. Krüger , S. Kulis , M. Kumar , S. Kunori , C. M. Kuo , V. Kuryatkov , J. Kvasnicka , S. Kyre , Y. Lai , K. Lamichhane , G. Landsberg , C. Lange , J. Langford , S. Laurien , M. Y. Lee , S. W. Lee , A. G. Stahl Leiton , A. Levin , A. Li , J. H. Li , Y. Y. Li , Z. Liang , H. Liao , Z. Lin , D. Lincoln , L. Linssen , R. Lipton , G. Liu , Y. Liu , A. Lobanov , V. Lohezic , D. Lomidze , R. S. Lu , S. Lu , M. Lupi , I. Lysova , A. -M. Magnan , F. Magniette , A. Mahjoub , S. Martens , M. Matysek , B. Meier , A. Malakhov , S. Mallios , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , G. Martinez , P. Masterson , M. Matthewman , S. N. Mayekar , A. David , S. Coco , B. Meng , A . Menkel , A. Mestvirishvili , G. Milella , I. Mirza , S. Moccia , G. B. Mohanty , F. Monti , F. W. Moortgat , I. Morrissey , J. Motta , S. Murthy , J. Musić , Y. Musienko , S. Nabili , M. Nguyen , A. Nikitenko , D. Noonan , D. Noonan , M. Noy , K. Nurdan , M. Wulansatiti Nursanto , C. Ochando , N. Odell , H. Okawa , Y. Onel , W. Ortez , J. Ozegović , S. Ozkorucuklu , E. Paganis , C. A. Palmer , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , M. Paranjpe , J. Parshook , N. Pastika , M. Paulini , T. Peitzmann , T. Peltola , N. Peng , A. Buchot Perraguin , P. Petiot , T. Pierre-Emile , M. Vicente Barreto Pinto , E. Popova , R. Pöschl , H. Prosper , M. Prvan , I. Puljak , S. R. Qasim , H. Qu , T. Quast , R. Quinn , M. Quinnan , A. Rane , K. K. Rao , K. Rapacz , L. Raux , W. Redjeb , M. Reinecke , M. Revering , F. Richard , A. Roberts , A. M. Sanchez , J. Rohlf , J. Rolph , T. Romanteau , M. Rosado , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , V. Rusinov , V. Ryjov , O. M. Sahin , R. Salerno , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , S. Schuwalow , E. Scott , C. Seez , F. Sefkow , D. Selivanova , S. Sharma , M. Shelake , A. Shenai , R. Shukla , E. Sicking , M. De , P. Silva , P. Simkina , F. Simon , A. E. Simsek , Y. Sirois , V. Smirnov , T. J. Sobering , E. Spencer , N. Srimanobhas , A. Steen , J. Strait , N. Strobbe , X. F. Su , Y. Sudo , C. Mantilla Suarez , E. Sukhov , L. Sulak , L. Sun , P. Suryadevara , C. Syal , C. de La Taille , B. Tali , C. L. Tan , J. Tao , A. Tarabini , T. Tatli , R. Thaus , R. D. Taylor , S. Tekten , A. Thiebault , D. Thienpont , C. Tiley , E. Tiras , M. Titov , D. Tlisov , U. G. Tok , A. Kayis , J. Troska , L. S. Tsai , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , S. Undleeb , D. Urbanski , E. Uslan , V. Ustinov , A. Uzunian , J. Varela , M. Velasco , E. Vernazza , O. Viazlo , P. Vichoudis , T. Virdee , E. Voirin , M. Vojinovi\c , M. Vojinovic , A. Wade , C. Wang , C. C. Wang , D. Wang , F. Wang , X. Wang , X. Wang , Z. Wang , M. Wayne , S. N. Webb , A. Whitbeck , R. Wickwire , J. S. Wilson , H. Y. Wu , L. Wu , M. Xiao , J. Yang , C. H Yeh , R. Yohay , D. Yu , S. S. Yu , C. Yuan , Y. Miao , F. Yumiceva , I. Yusuff , A. Zabi , A. Zacharopoulou , N. Zamiatin , A. Zarubin , P. Zehetner , D. Zerwas , H. Zhang , J. Zhang , Y. Zhang , Z. Zhang , X. Zhao

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

Instrumentation and Detectors · Physics 2020-04-28 Adrian Irles

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

The precise measurement of hadronic jet energy is crucial to maximise the physics reach of a future Linear Collider. An important ingredient required to achieve this is the efficient identification of photons within hadronic showers. One…

Instrumentation and Detectors · Physics 2015-06-04 Daniel Jeans , Jean-Claude Brient , Marcel Reinhard

A silicon-based fine granularity calorimeter is a potential technology for the future International Linear Collider ILC, the future circular collider CEPC, and is also the chosen technology for the upgraded CMS experiment of the Large…

Instrumentation and Detectors · Physics 2017-08-02 Stathes Paganis , Andreas Psallidas , Arnaud Steen

Studies of the response of the SiD silicon-tungsten electromagnetic calorimeter (ECal) are presented. Layers of highly granular (13 mm^2 pixels) silicon detectors embedded in thin gaps (~ 1 mm) between tungsten alloy plates give the SiD…

Instrumentation and Detectors · Physics 2017-03-28 Amanda Steinhebel , James Brau