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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 muon detectors of the experiments at the Large Hadron Collider (LHC) have to cope with unprecedentedly high neutron and gamma ray background rates. In the forward regions of the muon spectrometer of the ATLAS detector, for instance,…

Instrumentation and Detectors · Physics 2016-10-04 B. Bittner , J. Dubbert , O. Kortner , H. Kroha , F. Legger , R. Richter , O. Biebel , A. Engl , R. Hertenberger , F. Rauscher

Muon identification is of paramount importance for the physics programme of LHCb. In the upgrade phase, starting from Run 3 of the LHC, the trigger of the experiment will be solely based on software. The luminosity increase to…

The muon trigger system of the CMS experiment uses a combination of hardware and software to identify events containing a muon. During Run 2 (covering 2015-2018) the LHC achieved instantaneous luminosities as high as 2 $\times$…

High Energy Physics - Experiment · Physics 2021-07-06 CMS Collaboration

The CMS drift tubes (DT) muon detector, built for withstanding the LHC expected integrated and instantaneous luminosities, will be used also in the High Luminosity LHC (HL-LHC) at a 5 times larger instantaneous luminosity and, consequently,…

Instrumentation and Detectors · Physics 2019-12-16 G. Abbiendi , J. Alcaraz Maestre , A. Álvarez Fernández , B. Álvarez González , N. Amapane , I. Bachiller , J. M. Barcala , L. Barcellan , C. Battilana , M. Bellato , G. Bencze , M. Benettoni , N. Beni , A. Benvenuti , L. C. Blanco Ramos , A. Boletti , A. Bragagnolo , J. A. Brochero Cifuentes , V. Cafaro , A. Calderon , E. Calvo , A. Cappati , R. Carlin , C. A. Carrillo Montoya , F. R. Cavallo , J. M. Cela Ruiz , M. Cepeda , M. Cerrada , B. Chazin Quero , P. Checchia , L. Ciano , N. Colino , D. Corti , G. Cotto , J. Cuevas , M. Cuffiani , G. M. Dallavalle , D. Dattola , B. De La Cruz , P. DeRemigis , C. Erice Cid , F. Fabbri , A. Fanfani , D. Fasanella , C. F. Bedoya , J. F. de Trocóniz , P. Fernandez Manteca , J. Fernández Menéndez , J. P. Fernández Ramos , S. Folgueras , M. C. Fouz , D. Francia Ferrero , J. García Romero , F. Gasparini , U. Gasparini , S. Ghosh , V. Giordano , F. Gomez Casademunt , F. Gonella , I. González Caballero , J. R. González Fernández , O. González López , S. Goy López , A. Gozzelino , A. Griggio , G. Grosso , C. Guandalini , L. Guiducci , M. Gulmini , T. Hebbeker , C. Heidemann , J. M. Hernández , K. Hoepfner , F. Iemmi , R. Isocrate , M. I. Josa , B. Kiani , S. Lacaprara , S. Lo Meo , S. Marcellini , M. Margoni , J. Marín , C. Mariotti , I. Martín Martín , J. J. Martínez Morales , C. Martínez Rivero , S. Maselli , G. Masetti , A. T. Meneguzzo , M. Merschmeyer , G. Mocellin , L. Modenese , A. Molinero , J. Molnar , F. Montecassiano , D. Moran , J. J. Navarrete , F. Navarria , Á. Navarro Tobar , J. C. Oller , M. Passaseo , J. Pazzini , M. Pegoraro , J. Puerta Pelayo , M. Pelliccioni , B. Philipps , J. Piedra Gomez , G. L. Pinna Angioni , N. Pozzobon , M. Presilla , C. Prieels , F. Primavera , J. C. Puras Sánchez , I. Redondo , D. D. Redondo Ferrero , H. Reithler , T. Rodrigo , V. Rodríguez Bouza , J. Roemer , P. Ronchese , R. Rossin , F. Rotondo , T. Rovelli , S. Sánchez Cruz , S. Sánchez Navas , J. Sastre , L. Scodellaro , F. Simonetto , M. S. Soares , A. Staiano , Z. Szillasi , D. F. Teyssier , N. Toniolo , E. Torassa , D. Trocino , B. Ujvari , S. Ventura , R. Vilar Cortabitarte , J. Vizan Garcia , M. Zanetti , F. P. Zantis , G. Zilizi , P. Zotto

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 CMS muon detector system, muon reconstruction software, and high-level trigger underwent significant changes in 2013-2014 in preparation for running at higher LHC collision energy and instantaneous luminosity. The performance of the…

Instrumentation and Detectors · Physics 2018-06-21 CMS Collaboration

The High-Luminosity LHC (HL-LHC, or Phase 2 LHC) will deliver proton-proton collisions at 5-7.5 times the nominal LHC luminosity, with an expected number of 140-200 pp-interactions per bunch crossing (Pile-up or PU). To maintain the…

Instrumentation and Detectors · Physics 2023-07-19 Piet Verwilligen

"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

In the High Luminosity Large Hadron Collider (HL-LHC) program, during the next years, the instantaneous luminosity will increase up to 5 $\times$ 10$^{34}$ cm$^{-2}$ s$^{-1}$ which means a factor five higher than the nominal LHC. In that…

Instrumentation and Detectors · Physics 2021-11-30 R. Aly

Renewed international interest in muon colliders motivates the continued investigation of the impacts of beam-induced background on detector performance. This continues the effort initiated by the Muon Accelerator Program and carried out…

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

Long-lived charged particles are predicted by various theories beyond the Standard Model, leading to unique signatures that could reveal new physics. At the LHC, the CMS detector enables searches for these massive particles, identifiable by…

High Energy Physics - Experiment · Physics 2025-11-06 Tamas Almos Vami

The CMS experiment collected around 150 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV during the Run-2 data taking period of LHC. The CMS RPC system provided redundant information for robust muon triggering,…

Instrumentation and Detectors · Physics 2022-12-01 Kevin Mota Amarilo

The High Luminosity LHC (HL-LHC) phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. The foreseen gradual increase of the instantaneous luminosity of up to more than twice its…

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 hit response of silicon vertex and tracking detectors to muon collider beam background and results of a study of hit reducing techniques are presented. The background caused by decays of the 750 GeV/c m+ and m- beams was simulated using…

Instrumentation and Detectors · Physics 2018-09-26 V. Di Benedetto , C. Gatto , A. Mazzacane , N. V. Mokhov , S. I. Striganov , N. K. Terentiev

The CMS experiment, located at the CERN Large Hadron Collider, has a redundant muon system composed by three different detector technologies: Cathode Strip Chambers (in the forward regions), Drift Tubes (in the central region) and Resistive…

The high-luminosity upgrade of the CERN LHC requires the replacement of the CMS tracking detector to cope with the increased radiation fluence while maintaining its excellent performance. An extensive R\&D program, aiming at using 3D pixel…

Instrumentation and Detectors · Physics 2025-10-16 The Tracker Group of the CMS Collaboration