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The High Luminosity Large Hadron Collider (HL-LHC) will have a peak luminosity of $5\times10^{34} $cm$^{-2} $\,s$^{-1}$, five times higher than the design luminosity of the LHC. The hadronic ATLAS Tile Calorimeter TileCal) is a sampling…

Instrumentation and Detectors · Physics 2020-10-29 Eduardo Valdes Santurio

As part of its HL-LHC upgrade program, the CMS Collaboration is developing a High Granularity Calorimeter (CE) to replace the existing endcap calorimeters. The CE is a sampling calorimeter with unprecedented transverse and longitudinal…

Instrumentation and Detectors · Physics 2020-12-14 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , M. Alhusseini , J. Alison , G. Altopp , M. Alyari , S. An , S. Anagul , I. Andreev , M. Andrews , P. Aspell , I. A. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , P. Bargassa , D. Barney , E. Becheva , P. Behera , A. Belloni , T. Bergauer , M. Besancon , S. Bhattacharya , S. Bhattacharya , D. Bhowmik , P. Bloch , A. Bodek , M. Bonanomi , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , D. Braga , J. Brashear , E. Brondolin , P. Bryant , J. Bueghly , B. Bilki , B. Burkle , A. Butler-Nalin , S. Callier , D. Calvet , X. Cao , B. Caraway , S. Caregari , L. Ceard , Y. C. Cekmecelioglu , G. Cerminara , N. Charitonidis , R. Chatterjee , Y. M. Chen , Z. Chen , K. y. Cheng , S. Chernichenko , H. Cheung , C. H. Chien , S. Choudhury , D. Čoko , G. Collura , F. Couderc , I. Dumanoglu , D. Dannheim , P. Dauncey , A. David , G. Davies , E. Day , P. DeBarbaro , F. De Guio , C. de La Taille , M. De Silva , P. Debbins , E. Delagnes , J. M. Deltoro , G. Derylo , P. G. Dias de Almeida , D. Diaz , P. Dinaucourt , J. Dittmann , M. Dragicevic , S. Dugad , V. Dutta , S. Dutta , J. Eckdahl , T. K. Edberg , M. El Berni , S. C. Eno , Yu. Ershov , P. Everaerts , S. Extier , F. Fahim , C. Fallon , B. A. Fontana Santos Alves , E. Frahm , G. Franzoni , J. Freeman , T. French , E. Gurpinar Guler , Y. Guler , M. Gagnan , P. Gandhi , S. Ganjour , A. Garcia-Bellido , Z. Gecse , Y. Geerebaert , H. Gerwig , O. Gevin , W. Gilbert , A. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , T. Gonzalez , N. Gorbounov , L. Gouskos , Y. Gu , F. Guilloux , E. Gülmez , M. Hammer , A. Harilal , K. Hatakeyama , A. Heering , V. Hegde , U. Heintz , V. Hinger , N. Hinton , J. Hirschauer , J. Hoff , W. S. Hou , C. Isik , J. Incandela , S. Jain , H. R. Jheng , U. Joshi , O. Kara , V. Kachanov , A. Kalinin , R. Kameshwar , A. Kaminskiy , A. Karneyeu , O. Kaya , M. Kaya , A. Khukhunaishvili , S. Kim , K. Koetz , T. Kolberg , A. Kristić , M. Krohn , K. Krüger , N. Kulagin , S. Kulis , S. Kunori , C. M. Kuo , V. Kuryatkov , S. Kyre , O. K. Köseyan , Y. Lai , K. Lamichhane , G. Landsberg , J. Langford , M. Y. Lee , A. Levin , A. Li , B. Li , J. -H. Li , H. Liao , D. Lincoln , L. Linssen , R. Lipton , Y. Liu , A. Lobanov , R. S. Lu , I. Lysova , A. M. Magnan , F. Magniette , A. A. Maier , A. Malakhov , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , P. Masterson , B. Meng , T. Mengke , A. Mestvirishvili , I. Mirza , S. Moccia , I. Morrissey , T. Mudholkar , J. Musić , I. Musienko , S. Nabili , A. Nagar , A. Nikitenko , D. Noonan , M. Noy , K. Nurdan , C. Ochando , B. Odegard , N. Odell , Y. Onel , W. Ortez , J. Ozegović , L. Pacheco Rodriguez , E. Paganis , D. Pagenkopf , V. Palladino , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , J. Parshook , N. Pastika , M. Paulini , P. Paulitsch , T. Peltola , R. Pereira Gomes , H. Perkins , P. Petiot , F. Pitters , F. Pitters , H. Prosper , M. Prvan , I. Puljak , T. Quast , R. Quinn , M. Quinnan , K. Rapacz , L. Raux , G. Reichenbach , M. Reinecke , M. Revering , A. Rodriguez , T. Romanteau , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , A. E. Simsek , U. Sozbilir , O. M. Sahin , A. Sanchez , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , E. Scott , C. Seez , F. Sefkow , S. Sharma , I. Shein , A. Shenai , R. Shukla , E. Sicking , P. Sieberer , Y. Sirois , V. Smirnov , E. Spencer , A. Steen , J. Strait , T. Strebler , N. Strobbe , J. W. Su , E. Sukhov , L. Sun , M. Sun , C. Syal , B. Tali , U. G. Tok , A. Kayis Topaksu , C. L. Tan , I. Tastan , T. Tatli , R. Thaus , S. Tekten , D. Thienpont , T. Pierre-Emile , E. Tiras , M. Titov , D. Tlisov , J. Troska , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , N. Tyurin , S. Undleeb , D. Urbanski , V. Ustinov , A. Uzunian , M. van de Klundert , J. Varela , M. Velasco , M. Vicente Barreto Pinto , P. M. da Silva , T. Virdee , R. Vizinho de Oliveira , J. Voelker , E. Voirin , Z. Wang , X. Wang , F. Wang , M. Wayne , S. N. Webb , M. Weinberg , A. Whitbeck , D. White , R. Wickwire , J. S. Wilson , H. Y. Wu , L. Wu , C. H Yeh , R. Yohay , G. B. Yu , S. S. Yu , D. Yu , F. Yumiceva , A. Zacharopoulou , N. Zamiatin , A. Zarubin , S. Zenz , H. Zhang , J. Zhang

Sensors fabricated from high resistivity, float zone, silicon material have been the basis of vertex detectors and trackers for the last 30 years. The areas of these devices have increased from a few square cm to $\> 200\ m^2$ for the…

Throughout the year 2011, the Large Hadron Collider (LHC) has operated with an instantaneous luminosity that has risen continually to around 4x10^33cm-2 s-1. With this prodigious high-energy proton collisions rate, efficient triggering on…

Instrumentation and Detectors · Physics 2015-06-04 Alexandre Zabi

After the Large Hadron Collider (LHC) upgrade into High Luminosity LHC (HL-LHC), the instantaneous luminosity is expected to reach values up to 7.5x10^34cm^2/s, causing a harsher radiation environment as well as a significant increase in…

Instrumentation and Detectors · Physics 2026-05-07 Giorgia Bonomelli

Within the CALICE collaboration, several concepts for the hadronic calorimeter of a future linear collider detector are studied. After having demonstrated the capabilities of the measurement methods in "physics prototypes", the focus now…

Instrumentation and Detectors · Physics 2019-04-26 Christian Graf

During the upcoming High Luminosity phase of the Large Hadron Collider (HL-LHC), the integrated luminosity of the accelerator will increase to 3000 fb$^{-1}$. The expected experimental conditions in that period in terms of background rates,…

Instrumentation and Detectors · Physics 2022-01-19 A. Samalan , M. Tytgat , G. A. Alves , F. Marujo , F. Torres Da Silva De Araujo , E. M. DaCosta , D. De Jesus Damiao , H. Nogima , A. Santoro , S. Fonseca De Souza , A. Aleksandrov , R. Hadjiiska , P. Iaydjiev , M. Rodozov , M. Shopova , G. Soultanov , M. Bonchev , A. Dimitrov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , S. J. Qian , C. Bernal , A. Cabrera , J. Fraga , A. Sarkar , S. Elsayed , Y. Assran , M. El Sawy , M. A. Mahmoud , Y. Mohammed , C. Combaret , M. Gouzevitch , G. Grenier , I. Laktineh , L. Mirabito , K. Shchablo , I. Bagaturia , D. Lomidze , I. Lomidze , V. Bhatnagar , R. Gupta , P. Kumari , J. Singh , V. Amoozegar , B. Boghrati , M. Ebraimi , R. Ghasemi , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , R. Aly , W. Elmetenawee , N. DeFilippis , A. Gelmi , G. Iaselli , S. Leszki , F. Loddo , I. Margjeka , G. Pugliese , D. Ramos , M. Caponero , L. Benussi , S. Bianco , S. Colafranceschi , A. Russo , L. Passamonti , D. Piccolo , D. Pierluigi , G. Saviano , S. Buontempo , A. Di Crescenzo , F. Fienga , G. DeLellis , L. Lista , S. Meola , P. Paolucci , A. Braghieri , P. Salvini , P. Montagna , C. Riccardi , P. Vitulo , B. Francois , T. J. Kim , J. Park , S. Y. Choi , B. Hong , K. S. Lee , J. Goh , H. Lee , J. Eysermans , C. Uribe Estrada , I. Pedraza , H. Castilla-Valdez , A. Sanchez-Hernandez , C. A. Mondragon Herrera , D. A. Perez Navarro , G. A. AyalaSanchez , S. Carrillo , E. Vazquez , N. Zaganidis , A. Radi , A. Ahmad , I. Asghar , H. Hoorani , S. Muhammad , M. A. Shah , B. Mandelli , R. Guida , I. Crotty

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 electromagnetic ealorimeter (ECAL) of the CMS detector has played an important role in the physics program of the experiment, delivering outstanding performance throughout data taking. The High-Luminosity LHC will pose new challenges.…

Instrumentation and Detectors · Physics 2021-06-10 Stefano Argiro

The operation and performance of the Compact Muon Solenoid (CMS) electromagnetic calorimeter (ECAL) are presented, based on data collected in pp collisions at $\sqrt{s}$ = 13 TeV at the CERN LHC, in the years from 2015 to 2018 (LHC Run 2),…

Instrumentation and Detectors · Physics 2024-09-06 CMS Collaboration

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

It is foreseen to significantly increase the luminosity of the LHC in order to harvest the maximum physics potential. Especially the Phase-II-Upgrade foreseen for 2023 will mean unprecedented radiation levels, significantly beyond the…

Instrumentation and Detectors · Physics 2019-10-15 Marco Mandurrino

More than a thousand 8" silicon sensors will be visually inspected to look for anomalies on their surface during the quality control preceding assembly into the High-Granularity Calorimeter for the CMS experiment at CERN. A deep…

Instrumentation and Detectors · Physics 2023-03-28 Sonja Grönroos , Maurizio Pierini , Nadezda Chernyavskaya

Hybrid silicon pixel detectors are currently used in the innermost tracking system of the Compact Muon Solenoid (CMS) experiment. Radiation tolerance up to fluences expected for a few years of running of the Large Hadron Collider (LHC) has…

Instrumentation and Detectors · Physics 2011-10-07 Gemma Tinti

The increased particle flux at the high luminosity phase of the Large Hadron Collider (HL-LHC), with instantaneous luminosities of up to 7.5 times the original design value, will have an impact on many sub-systems of the ATLAS detector.…

Instrumentation and Detectors · Physics 2016-12-22 Thomas G. McCarthy

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 Tile Calorimeter (TileCal) is the hadronic calorimeter covering the central region of the ATLAS detector at the LHC. It is a sampling calorimeter consisting of alternating thin steel plates and scintillating tiles. Wavelength shifting…

Instrumentation and Detectors · Physics 2017-09-04 Michaela Mlynarikova

Silicon pad sensors are proposed as active material in highly granular sampling calorimeters of future collider experiments such as the Compact Linear Collider (CLIC) or the International Linear Collider (ILC). The electromagnetic section…

Instrumentation and Detectors · Physics 2021-03-01 Erica Brondolin , Dominik Dannheim , Szymon Kulis , Andreas A. Maier , Florian Pitters , Thorben Quast , Eva Sicking

While the CMS experiment is currently harvesting LHC collision data at CERN, the performance of its electromagnetic calorimeter (ECAL) is being constantly monitored, and work has started to assess the need for changes to the detector to…

Instrumentation and Detectors · Physics 2019-08-13 Francesca Nessi Tedaldi

Within the CALICE collaboration, several concepts for the hadronic calorimeter of a future lepton collider detector are studied. After having demonstrated the capabilities of the measurement methods in "physics prototypes", the focus now…

Instrumentation and Detectors · Physics 2019-08-13 Yong Liu