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Radiation damage in the plastic scintillator and/or readout WLS fibers in the HE endcap calorimeter 1.4<y<4 in the CMS experiment at LHC and SLHC will require remediation after 2018. We describe one alternative using the existing brass…

Instrumentation and Detectors · Physics 2013-08-28 Burak Bilki , Yasar Onel , David R. Winn , Taylan Yetkin

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

The existing CMS endcap calorimeters will be replaced with a High Granularity Calorimeter (HGCAL) for operation at the High Luminosity (HL) LHC. Radiation hardness and excellent physics performance will be achieved by utilising silicon pad…

Instrumentation and Detectors · Physics 2020-08-26 Artur Lobanov

The CMS Collaboration is preparing to build replacement endcap calorimeters for the HL-LHC era. The new high-granularity calorimeter (HGCAL) is, as the name implies, a highly-granular sampling calorimeter with approximately six million…

Instrumentation and Detectors · Physics 2022-12-21 Thorben Quast

Measurements are presented of the reduction of signal output due to radiation damage for plastic scintillator tiles used in the hadron endcap (HE) calorimeter of the CMS detector. The tiles were exposed to particles produced in…

Instrumentation and Detectors · Physics 2020-06-15 CMS Collaboration

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

High-Luminosity running at the LHC, which is planned for 2022 and beyond, will imply an order of magnitude increase in radiation levels and particle fluences with respect to the present LHC running conditions. The performance evolution of…

Instrumentation and Detectors · Physics 2014-09-11 Andrea Massironi

The CMS detector at the LHC requires a major upgrade to cope with the higher instantaneous luminosity and the elevated radiation levels. The active media of the forward backing hadron calorimeters is projected to be radiation-hard, high…

Instrumentation and Detectors · Physics 2015-10-30 Emrah Tiras

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 High-Luminosity LHC (HL-LHC) era, set to begin in 2029, will provide the general-purpose experiments with an instantaneous luminosity of up to $\mathcal{L} = 7.5 \times 10^{34}$ cm$^{-2}$ s$^{-1}$ from pp collisions at a centre-of-mass…

High Energy Physics - Experiment · Physics 2025-01-08 Thiago R. F. P. Tomei

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

A study has been performed to understand the effects of radiation damage on various plastic scintillator tiles considered for a possible upgrade of the hadron calorimeter of the CMS detector. Measurements were made with unirradiated tiles…

Instrumentation and Detectors · Physics 2024-09-30 The CMS HCAL Collaboration

The Tile Calorimeter (TileCal) is the central hadronic calorimeter of the ATLAS experiment at the Large Hadron Collider (LHC). The LHC is scheduled to undergo a major upgrade, in 2022, for the High Luminosity LHC (HL-LHC). The ATLAS upgrade…

Instrumentation and Detectors · Physics 2019-08-14 A. S. Cerqueira

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

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

The High Luminosity LHC (HL-LHC) will integrate 10 times more luminosity than the LHC, posing significant challenges for radiation tolerance and event pileup on detectors, especially for forward calorimetry, and hallmarks the issue for…

Instrumentation and Detectors · Physics 2018-07-01 Florian Pitters

The ATLAS hadronic Tile Calorimeter will undergo major upgrades to the on- and off-detector electronics in preparation for the High Luminosity program of the Large Hadron Collider (HL-LHC) in 2026, so that the system can cope with the…

Instrumentation and Detectors · Physics 2020-08-26 Jalal Abdallah

The HL-LHC and the corresponding detector upgrades for the CMS experiment will present extreme challenges for the full simulation. In particular, increased precision in models of physics processes may be required for accurate reproduction…

Computational Physics · Physics 2020-11-19 Kevin Pedro

The CMS detector will undergo significant improvements to face the 10-fold increase in integrated luminosity of LHC, the so-called High-Luminosity LHC, scheduled to start in 2027. This will include a completely new calorimeter in the CMS…

Instrumentation and Detectors · Physics 2020-06-24 Erica Brondolin

The High Luminosity LHC (HL-LHC) will integrate 10 times more luminosity than the LHC, posing significant challenges for radiation tolerance and event pileup on detectors, especially for forward calorimetry, and hallmarks the issue for…

Instrumentation and Detectors · Physics 2018-02-18 Arabella Martelli
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