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Related papers: CMS detector: Run 3 status and plans for Phase-2

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A new tracking detector will be installed as part of the Phase-2 upgrade of the CMS detector for the high-luminosity LHC era. This tracking detector includes the Inner Tracker, equipped with silicon pixel sensor modules, and the Outer…

Instrumentation and Detectors · Physics 2024-09-02 The Tracker Group of the CMS Collaboration

The High-Luminosity LHC will put significant demands on trigger systems. To control trigger thresholds, the CMS Collaboration is designing a novel Level-1 track trigger. The Outer Tracker will use modules with pairs of sensor layers to read…

Instrumentation and Detectors · Physics 2021-11-04 Brent R. Yates

The CMS pixel detector is the innermost component of the CMS tracker occupying the region around the centre of CMS, where the LHC beams are crossed, between 4.3 cm and 30 cm in radius and 46.5 cm along the beam axis. It operates in a…

Instrumentation and Detectors · Physics 2019-08-13 Viktor Veszpremi

The Compact Muon Solenoid (CMS) detector is one of two general-purpose detectors that reconstruct the products of high energy particle interactions at the Large Hadron Collider (LHC) at CERN. The silicon pixel detector is the innermost…

Instrumentation and Detectors · Physics 2019-08-13 Tamas Almos Vami

The upgrade of the ALICE TPC will allow the experiment to cope with the high interaction rates foreseen for the forthcoming Run 3 and Run 4 at the CERN LHC. In this article, we describe the design of new readout chambers and front-end…

Instrumentation and Detectors · Physics 2021-03-26 J. Adolfsson , M. Ahmed , S. Aiola , J. Alme , T. Alt , W. Amend , F. Anastasopoulos , C. Andrei , M. Angelsmark , V. Anguelov , A. Anjam , H. Appelshäuser , V. Aprodu , O. Arnold , M. Arslandok , D. Baitinger , M. Ball , G. G. Barnaföldi , E. Bartsch , P. Becht , R. Bellwied , A. Berdnikova , M. Berger , N. Bialas , P. Bialas , S. Biswas , B. Blidaru , L. Boldizsár , L. Bratrud , P. Braun-Munzinger , M. Bregant , C. L. Britton , S. Brucker , E. J. Brücken , H. Büsching , R. Soto Camacho , A. L. Campos , G. Caragheorgheopol , D. D. Carvalho , A. J. Castro , P. Chatzidaki , P. Christiansen , L. G. Clonts , T. M. Cormier , A. L. D. Couto , H. G. A. Cubas , A. Deisting , P. Dhankher , S. Dittrich , V. Duta , R. Ehlers , M. Engel , M. N. Ericson , N. B. Ezell , L. Fabbietti , F. Flor , G. Föhner , U. Frankenfeld , E. Futo , J. J. Gaardhøje , M. G. Munhoz , C. Garabatos , P. Gasik , T. Geiger , Á. Gera , P. Glässel , D. J. Q. Goh , O. Grachov , A. Grein , M. Gul , T. Gunji , M. Habib , H. Hamagaki , G. Hamar , J. C. Hansen , A. Harlenderova , J. W. Harris , S. Hassan , P. Hauer , S. Hayashi , S. T. Heckel , J. Hehner , J. K. Heino , E. Hellbär , H. Helstrup , A. Herghelegiu , L. Hernandes da Costa Porto , R. A. Hernandez , H. D. Hernandez Herrera , T. Herold , T. E. Hilden , B. Hohlweger , S. Hornung , C. Hughes , S. Hummel , M. Ivanov , J. Jung , M. Jung , D. Just , E. Kangasaho , L. Karayan , B. Ketzer , S. Kirsch , M. Kleiner , T. Klemenz , S. Klewin , A. G. Knospe , E. Koskinen , M. Kowalski , L. Kreis , M. Krüger , N. Kupfer , R. Lang , L. Lautner , M. Lesch , Y. Lesenechal , F. Liebske , C. Lippmann , V. Litichevskyi , M. Ljunggren , W. J. Llope , S. Mahmood , T. Mahmoud , R. D. Majka , C. Markert , J. Martinez , T. A. Martins , S. Masciocchi , A. Mathis , O. Matonoha , Y. Matsuyama , A. Matyja , M. Meres , D. L. Mihaylov , D. Miśkowiec , T. Mittelstaedt , L. S. Montali , D. M. Moraes , C. Mordasini , T. Morhardt , S. Muley , J. Mulligan , R. H. Munzer , H. Murakami , K. Münning , A. Nassirpour , H. Natal da Luz , C. Nattrass , R. A. Negrao De Oliveira , H. G. Neves , B. S. Nielsen , W. A. V. Noije , M. Ogino , A. C. Oliveira Da Silva , A. Oskarsson , J. Ottnad , K. Oyama , A. Önnerstad , L. Österman , A. A. Pabon , Y. Pachmayer , G. Paić , J. Parkkila , S. Pathak , R. N. Patra , V. Peskov , M. Petris , M. Petrovici , M. Planinic , F. Pompei , L. Prodan , A. Radu , L. Radulescu , J. Rak , J. Rasson , V. Ratza , K. F. Read , A. Rehman , R. Renfordt , K. Røed , D. Röhrich , E. Rubio , T. Rudzki , A. Rusu , M. Saleh , B. C. S. Sanches , J. Schambach , S. Scheid , C. Schmidt , A. Schmier , H. Schulte , K. Schweda , D. Sekihata , N. Shimizu , S. Siebig , R. W. D. Silva , D. Silvermyr , D. Simpson , B. Sitar , N. Smirnov , T. Snellman , H. K. Soltveit , S. P. Sorensen , F. Sozzi , J. Stachel , A. Szabo , L. Šerkšnytė , Y. Takeuchi , G. Tambave , Y. Tanaka , K. Terasaki , R. J. Turpeinen , K. Ullaland , B. Ulukutlu , E. Umaka , A. Utrobicic , D. Varga , A. Vargas , M. Vargyas , R. Varma , O. Vazquez Rueda , A. Velure , S. Vereschagin , S. Vergara Limón , L. Vergara Urrutia , O. Vorbach , B. Voss , D. Vranic , R. J. Warmack , T. O. Weber , C. Weidlich , J. Wiechula , B. Windelband , S. Winkler , W. Witt

An estimate of environmental background hit rate on triple-GEM chambers is performed using Monte Carlo (MC) simulation and compared to data taken by test chambers installed in the CMS experiment (GE1/1) during Run-2 at the Large Hadron…

Instrumentation and Detectors · Physics 2022-01-05 M. Abbas , M. Abbrescia , H. Abdalla , A. Abdelalim , S. AbuZeid , A. Agapitos , A. Ahmad , A. Ahmed , W. Ahmed , C. Aimè , C. Aruta , I. Asghar , P. Aspell , C. Avila , I. Azhgirey , J. Babbar , Y. Ban , R. Band , S. Bansal , L. Benussi , V. Bhatnagar , M. Bianco , S. Bianco , K. Black , L. Borgonovi , O. Bouhali , A. Braghieri , S. Braibant , S. Butalla , S. Calzaferri , M. Caponero , F. Cassese , A. Castaneda , N. Cavallo , S. S. Chauhan , A. Colaleo , A. Conde Garcia , M. Dalchenko , A. De Iorio , G. De Lentdecker , D. Dell Olio , G. De Robertis , W. Dharmaratna , S. Dildick , B. Dorney , R. Erbacher , F. Fabozzi , F. Fallavollita , A. Ferraro , D. Fiorina , E. Fontanesi , M. Franco , C. Galloni , P. Giacomelli , S. Gigli , J. Gilmore , M. Gola , M. Gruchala , A. Gutierrez , R. Hadjiiska , T. Hakkarainen , J. Hauser , K. Hoepfner , M. Hohlmann , H. Hoorani , T. Huang , P. Iaydjiev , A. Irshad , A. Iorio , F. Ivone , J. Jaramillo , V. Jha , A. Juodagalvis , E. Juska , B. Kailasapathy , T. Kamon , Y. Kang , P. Karchin , A. Kaur , H. Kaur , H. Keller , H. Kim , J. Kim , S. Kim , B. Ko , A. Kumar , S. Kumar , H. Kumawat , N. Lacalamita , J. S. H. Lee , A. Levin , Q. Li , F. Licciulli , L. Lista , K. Liyanage , F. Loddo , M. Luhach , M. Maggi , Y. Maghrbi , N. Majumdar , K. Malagalage , S. Malhotra , S. Mallows , S. Martiradonna , N. Mccoll , C. McLean , J. Merlin , M. Misheva , D. Mishra , G. Mocellin , L. Moureaux , A. Muhammad , S. Muhammad , S. Mukhopadhyay , M. Naimuddin , P. Netrakanti , S. Nuzzo , R. Oliveira , L. Pant , P. Paolucci , I. C. Park , L. Passamonti , G. Passeggio , A. Peck , A. Pellecchia , N. Perera , L. Petre , H. Petrow , D. Piccolo , D. Pierluigi , G. Raffone , M. Rahmani , F. Ramirez , A. Ranieri , G. Rashevski , B. Regnery , M. Ressegotti , C. Riccardi , M. Rodozov , E. Romano , C. Roskas , B. Rossi , P. Rout , D. Roy , J. D. Ruiz , A. Russo , A. Safonov , A. K. Sahota , D. Saltzberg , G. Saviano , A. Shah , A. Sharma , R. Sharma , T. Sheokand , M. Shopova , F. Simone , J. Singh , U. Sonnadara , E. Starling , B. Stone , J. Sturdy , G. Sultanov , Z. Szillasi , D. Teague , D. Teyssier , T. Tuuva , M. Tytgat , I. Vai , N. Vanegas , R. Venditti , P. Verwilligen , W. Vetens , A. K. Virdi , P. Vitulo , A. Wajid , D. Wang , K. Wang , I. J. Watson , N. Wickramage , W. Jang , D. D. C. Wickramarathna , S. Yang , Y. Yang , U. Yang , J. Yongho , I. Yoon , Z. You , I. Yu , S. Zaleski

The CMS experiment is a multi-purpose detector successfully operated at the LHC where predominantly pp collisions take place at various centre of mass energies up to sqrt(s)=8 TeV at present. Discussed are pp collision results until end of…

High Energy Physics - Experiment · Physics 2012-10-16 Lars Sonnenschein

(Abridged version) The CMS experiment at the LHC will begin operation in 2007. The CMS Tracker sub-detector, comprises ~10 million detector channels read out by ~40 000 analog optical links. The optoelectronic components have been designed…

Instrumentation and Detectors · Physics 2010-05-03 Stefanos Dris

A wealth of physics results have already been obtained from the LHC, due to the excellent performance of the collider and its experiments. Even more results are expected to be achievable in the phase of the high-luminosity LHC (HL-LHC). It…

High Energy Physics - Experiment · Physics 2021-05-26 Susanne Kuehn

The Large Hadron Collider (LHC) started the Run 3 operation in 2022, and the peak instantaneous luminosity in Run 3 may reach 3 x 10^34 cm-2s-1. The ATLAS Monitored Drift Tube (MDT) chambers are the main component of the precision tracking…

Instrumentation and Detectors · Physics 2026-02-04 Jiajin Ge , Bing Li , Markus Fras , Junjie Zhu , Bing Zhou , Tiesheng Dai

With the increases in the LHC instantaneous luminosity, maintaining effective triggering and avoiding dead time will become especially challenging. As the sensitivity of many physics studies, depends critically on the ability to maintain…

Instrumentation and Detectors · Physics 2013-10-09 A. Castaneda

The High Luminosity upgrade of the CERN Large Hadron Collider will be able to reach a peak instantaneous luminosity of 5E34/cm2 s. The innermost detectors of the CMS and ATLAS experiments will have to cope with unprecedented requirements on…

Instrumentation and Detectors · Physics 2021-06-16 Jordi Duarte-Campderros

At the High Luminosity LHC (HL-LHC), the CMS experiment will face a harsh environment with a high instantaneous luminosity up to 7x10$^{34}$/cm$^2$/s corresponding to an average of 140-200 multiple proton-proton collisions per bunch…

Instrumentation and Detectors · Physics 2018-12-04 Chang-Seong Moon

"Soft" muons with a transverse momentum below 10 GeV are featured in many processes studied by the CMS experiment, such as decays of heavy-flavor hadrons or rare tau lepton decays. Maximizing the selection efficiency for these muons, while…

High Energy Physics - Experiment · Physics 2025-04-22 CMS Collaboration

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 Level-1 trigger of the CMS experiment at CERN has been designed to select proton-proton interactions whose final state includes signatures of new physics in the form of high transverse energy electrons, photons, jets, or high missing…

Instrumentation and Detectors · Physics 2008-10-23 C. Foudas

In planning for the Phase II upgrades of CMS and ATLAS major considerations are: 1)being able to deal with degradation of tracking and calorimetry up to the radiation doses to be expected with an integrated luminosity of 3000 $fb^{-1}$ and…

Instrumentation and Detectors · Physics 2013-10-08 Sebastian White

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 HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of…

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