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Between 2025 and 2027, some essential components of the CMS (Compact Muon Solenoid) detector - most notably the tracker and the calorimeter endcap - will be upgraded to prepare for HL-LHC (High Luminosity Large Hadron Collider) conditions.…

Instrumentation and Detectors · Physics 2020-03-26 Viktoria Hinger

The measurement of the magnetic field in the tracking volume inside the superconducting coil of the Compact Muon Solenoid (CMS) detector under construction at CERN is done with a fieldmapper designed and produced at Fermilab. The…

The structure of the CMS inner tracking system has been studied using nuclear interactions of hadrons striking its material. Data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded in 2015 at the LHC are used to…

Instrumentation and Detectors · Physics 2018-11-01 CMS Collaboration

Gas Electron Multiplier (GEM) technology is being considered for the forward muon upgrade of the CMS experiment in Phase 2 of the CERN LHC. Its first implementation is planned for the GE1/1 system in the $1.5 < \mid\eta\mid < 2.2$ region of…

Instrumentation and Detectors · Physics 2014-12-10 D. Abbaneo , M. Abbas , M. Abbrescia , A. A. Abdelalim , M. Abi Akl , W. Ahmed , W. Ahmed , P. Altieri , R. Aly , C. Asawatangtrakuldee , A. Ashfaq , P. Aspell , Y. Assran , I. Awan , S. Bally , Y. Ban , S. Banerjee , P. Barria , L. Benussi , V. Bhopatkar , S. Bianco , J. Bos , O. Bouhali , S. Braibant , S. Buontempo , C. Calabria , M. Caponero , C. Caputo , F. Cassese , A. Castaneda , S. Cauwenbergh , F. R. Cavallo , A. Celik , M. Choi , K. Choi , S. Choi , J. Christiansen , A. Cimmino , S. Colafranceschi , A. Colaleo , A. Conde Garcia , M. M. Dabrowski , G. De Lentdecker , R. De Oliveira , G. de Robertis , S. Dildick , B. Dorney , W. Elmetenawee , G. Fabrice , M. Ferrini , S. Ferry , P. Giacomelli , J. Gilmore , L. Guiducci , A. Gutierrez , R. M. Hadjiiska , A. Hassan , J. Hauser , K. Hoepfner , M. Hohlmann , H. Hoorani , Y. G. Jeng , T. Kamon , P. E. Karchin , H. S. Kim , S. Krutelyov , A. Kumar , J. Lee , T. Lenzi , L. Litov , F. Loddo , T. Maerschalk , G. Magazzu , M. Maggi , Y. Maghrbi , A. Magnani , N. Majumdar , P. K. Mal , K. Mandal , A. Marchioro , A. Marinov , J. A. Merlin , A. K. Mohanty , A. Mohapatra , S. Muhammad , S. Mukhopadhyay , M. Naimuddin , S. Nuzzo , E. Oliveri , L. M. Pant , P. Paolucci , I. Park , G. Passeggio , B. Pavlov , B. Philipps , M. Phipps , D. Piccolo , H. Postema , G. Pugliese , A. Puig Baranac , A. Radi , R. Radogna , G. Raffone , S. Ramkrishna , A. Ranieri , C. Riccardi , A. Rodrigues , L. Ropelewski , S. RoyChowdhury , M. S. Ryu , G. Ryu , A. Safonov , A. Sakharov , S. Salva , G. Saviano , A. Sharma , S. K. Swain , J. P. Talvitie , C. Tamma , A. Tatarinov , N. Turini , T. Tuuva , J. Twigger , M. Tytgat , I. Vai , M. van Stenis , R. Venditi , E. Verhagen , P. Verwilligen , P. Vitulo , D. Wang , M. Wang , U. Yang , Y. Yang , R. Yonamine , N. Zaganidis , F. Zenoni , A. Zhang

A prototype of the CMOS pixel sensor named SUPIX-1 has been fabricated and tested in order to investigate the feasibility of a pixelated tracker for a proposed Higgs factory, namely, the Circular Electron-Positron Collider (CEPC). The…

Instrumentation and Detectors · Physics 2022-01-05 L. Li , L. Zhang , J. N. Dong , J. Liu , M. Wang

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

We report recent results on the use of charge division to obtain a longitudinal coordinate from silicon strip detectors, and on sources of electronic readout noise for long, thin strips. These results hold promise for the design of Linear…

Instrumentation and Detectors · Physics 2010-05-18 Jerome Carman , Kelsey Collier , Sean Crosby , Vitaliy Fadeyev , Bruce A. Schumm , Ned Spencer

We present the recent development of a lightweight detector capable of accurate spatial, timing, and amplitude resolution of charged particles. The technology is based on double-sided double-metal p+\,--\,n\,--\,n+ micro-strip silicon…

First of its kind, the barrel section of the MIP Timing Detector is a large area timing detector based on LYSO:Ce crystals and SiPMs which are required to operate in an unprecedentedly harsh radiation environment (up to an integrated…

Instrumentation and Detectors · Physics 2025-08-14 F. Addesa , P. Akrap , A. Albert , B. Allmond , T. Anderson , J. Babbar , D. Baranyai , P. Barria , C. Basile , A. Benaglia , A. Benato , M. Benettoni , M. Besancon , N. Bez , S. Bhattacharya , R. Bianco , D. Blend , A. Boletti , A. Bornheim , R. Bugalho , A. Bulla , B. Cardwell , R. Carlin , M. Casarsa , F. Cetorelli , F. Cossutti , B. Cox , G. Da Molin , F. De Guio , K. De Leo , F. De Riggi , P. Debbins , D. Del Re , R. Delli Gatti , J. Dervan , P. Devouge , K. Dreimanis , O. M. Eberlins , F. Errico , E. Fernandez , W. Funk , A. Gaile , M. Gallinaro , R. Gargiulo , R. Gerosa , A. Ghezzi , B. Gyongyosi , Z. Hao , A. H. Heering , Z. Hu , R. Isocrate , M. Jose , A. Karneyeu , M. S. Kim , A. Krishna , B. Kronheim , O. K. Köseyan , A. Ledovskoy , L. Li , Z. Li , V. Lohezic , F. Lombardi , M. T. Lucchini , M. Malberti , Y. Mao , Y. Maravin , B. Marzocchi , D. Mazzaro , R. Menon Raghunandanan , P. Meridiani , C. Munoz Diaz , Y. Musienko , S. Nargelas , L. L. Narváez , C. Neu , G. Organtini , T. Orimoto , D. Osite , M. Paganoni , S. Palluotto , C. Palmer , N. Palmeri , F. Pandolfi , R. Paramatti , T. Pauletto , A. Perego , G. Pikurs , G. Pizzati , R. Plese , C. Quaranta , G. Reales Gutiérrez , N. Redaelli , S. Ronchi , R. Rossin , M. Ö. Sahin , F. Santanastasio , I. Schmidt , D. Sidiropoulos Kontos , T. Sievert , R. Silva , P. Simmerling , L. Soffi , P. Solanki , G. Sorrentino , M. Spiropulu , N. R. Strautnieks , X. Sun , D. D. Szabo , T. Tabarelli de Fatis , G. Tamulaitis , R. Taylor , M. Titov , M. Tosi , G. Trabucco , A. Tsirou , C. Tully , M. Turcato , B. Ujvari , J. Varela , F. Veronese , V. Vladimirov , J. Wang , M. Wayne , S. White , Z. Wu , J. W. Wulff , R. A. Wynne , L. Zhang , M. Zhang , G. Zilizi

After the successful installation and first operation of the upgraded Inner Tracking System (ITS2), which consists of about $10\,$m$^2$ of monolithic silicon pixel sensors, ALICE is pioneering the usage of bent, wafer-scale pixel sensors…

Instrumentation and Detectors · Physics 2022-12-07 Alperen Yüncü

The ATLAS Inner Tracker, the future innermost part of the ATLAS detector, is an all-silicon tracker composed of pixel and strip modules, designed to cope with the extreme conditions expected during High-Luminosity LHC runs. Thorough testing…

The evolution of particle detectors has always pushed the technological limit in order to provide enabling technologies to researchers in all fields of science. One archetypal example is the evolution of silicon detectors, from a system…

Instrumentation and Detectors · Physics 2017-07-04 Hartmut F. -W. Sadrozinski , Abraham Seiden , Nicolò Cartiglia

The CMS detector is one of the two general purpose experiments that will study the collisions produced by the Large Hadron Collider (LHC). The LHC is supposed to start its operation in 2007 at an instantaneous luminosity of 2 x 10^33 cm-2…

High Energy Physics - Experiment · Physics 2019-08-14 G. Bruno

The Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) is a heavy-ion experiment designed to study nuclear matter at the highest baryonic density. For high-statistics measurements of…

Instrumentation and Detectors · Physics 2025-05-28 The CBM Collaboration

The pixel detector of the Compact Muon Solenoid experiment consists of three barrel layers and two disks for each endcap. The detector was installed in summer 2008, commissioned with charge injections, and operated in the 3.8 T magnetic…

Instrumentation and Detectors · Physics 2012-08-27 CMS Collaboration

In the high luminosity scenario of the LHC (HL-LHC), which will bring the instantaneous luminosity up to 7.5\,$\times$\,$10^{34}$\,cm$^{-2}$s$^{-1}$, ATLAS and CMS will need to operate at up to 200 interactions per 25\,ns beam crossing and…

Instrumentation and Detectors · Physics 2021-06-11 Alessandro La Rosa

With the High Luminosity LHC upgrades, incorporating tracking information into the CMS Level-1 trigger becomes necessary in order to maintain a manageable trigger rate and good trigger performance e.g. to retain thresholds for electroweak…

Instrumentation and Detectors · Physics 2019-04-02 Zhengcheng Tao

To cope with the challenging environment of the planned high luminosity upgrade of the Large Hadron Collider (HL-LHC), scheduled to start operation in 2029, CMS will replace its entire tracking system. The requirements for the tracker are…

Instrumentation and Detectors · Physics 2022-12-12 The Tracker Group of the CMS Collaboration