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

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The CMS muon system has played a key role for many physics results obtained from the LHC Run-1 data. During the Long Shutdown (2013-2014) significant upgrades have been carried out on the muon detectors and on the L1 muon trigger. In…

Instrumentation and Detectors · Physics 2019-08-13 Giovanni Abbiendi

The ALICE Collaboration completed the upgrade of the detector and is now commissioning for the beginning of the data taking during LHC Run 3. In parallel, R&D activities and simulation studies are being performed to define the future of the…

High Energy Physics - Experiment · Physics 2022-11-09 Domenico Colella , for the ALICE Collaboration

The High Luminosity Large Hadron Collider (HL-LHC) at CERN is expected to collide protons at a centre-of-mass energy of 14\,TeV and to reach the unprecedented peak instantaneous luminosity of 5\,$-$\,7.5\,x\,$10^{34}$\,cm$^{-2}$s$^{-1}$…

Instrumentation and Detectors · Physics 2020-04-22 Alessandro La Rosa

The current CMS silicon pixel detector as the innermost component of the CMS experiment is performing well at LHC design luminosity, but would be subject to severe inefficiencies at LHC peak luminosities of 2x10e34 cm^-2 s^-1. Therefore, an…

Instrumentation and Detectors · Physics 2015-05-15 Simon Spannagel

The High Luminosity Large Hadron Collider (HL-LHC) at CERN is expected to collide protons at a center-of-mass energy of 14 TeV and to reach the unprecedented peak instantaneous luminosity of $7.5 \times 10^{34} \text{cm}^{-2} \text{s}^{-1}$…

Instrumentation and Detectors · Physics 2023-01-26 Sascha Liechti

The CMS detector at the CERN LHC features a silicon pixel detector as its innermost subdetector. The original CMS pixel detector has been replaced with an upgraded pixel system (CMS Phase-1 pixel detector) in the extended year-end technical…

Instrumentation and Detectors · Physics 2020-12-29 The Tracker Group of the CMS Collaboration

The Large Hadron Collider has entered a new era in Run 2, with centre-of-mass energy of 13 TeV and instantaneous luminosity reaching $\mathcal{L}_\textrm{inst} = 1.4\times$10$^{34}$ cm$^{-2}$ s$^{-1}$ for pp collisions. In order to cope…

High Energy Physics - Experiment · Physics 2017-11-09 Thiago R. F. P. Tomei

During Phase-2 of the LHC, known as the High Luminosity LHC (HL-LHC), the accelerator will increase its instantaneous luminosity to 5 $\times$ 10$^{34}$ cm$^{-2}$ s$^{-1}$, delivering an integrated luminosity of 3000 fb$^{-1}$ over 10 years…

Instrumentation and Detectors · Physics 2020-07-24 Priyanka Kumari

The CMS inner pixel detector system is planned to be replaced during the first phase of the LHC luminosity upgrade. The plans foresee an ultra low mass system with four barrel layers and three disks on either end. With the expected increase…

Instrumentation and Detectors · Physics 2019-08-13 Carlotta Favaro

The present Compact Muon Solenoid silicon pixel tracking system has been designed for a peak luminosity of 1034cm-2s-1 and total dose corresponding to two years of the Large Hadron Collider (LHC) operation. With the steady increase of the…

Instrumentation and Detectors · Physics 2011-10-11 N. Parashar

A new pixel detector for the CMS experiment was built in order to cope with the instantaneous luminosities anticipated for the Phase~I Upgrade of the LHC. The new CMS pixel detector provides four-hit tracking with a reduced material budget…

Instrumentation and Detectors · Physics 2017-06-02 M. Dragicevic , M. Friedl , J. Hrubec , H. Steininger , A. Gädda , J. Härkönen , T. Lampén , P. Luukka , T. Peltola , E. Tuominen , E. Tuovinen , A. Winkler , P. Eerola , T. Tuuva , G. Baulieu , G. Boudoul , L. Caponetto , C. Combaret , D. Contardo , T. Dupasquier , G. Gallbit , N. Lumb , L. Mirabito , S. Perries , M. Vander Donckt , S. Viret , C. Bonnin , L. Charles , L. Gross , J. Hosselet , D. Tromson , L. Feld , W. Karpinski , K. Klein , M. Lipinski , G. Pierschel , M. Preuten , M. Rauch , M. Wlochal , M. Aldaya , C. Asawatangtrakuldee , K. Beernaert , D. Bertsche , C. Contreras-Campana , G. Eckerlin , D. Eckstein , T. Eichhorn , E. Gallo , J. Garay Garcia , K. Hansen , M. Haranko , A. Harb , J. Hauk , J. Keaveney , A. Kalogeropoulos , C. Kleinwort , W. Lohmann , R. Mankel , H. Maser , G. Mittag , C. Muhl , A. Mussgiller , D. Pitzl , O. Reichelt , M. Savitskyi , P. Schütze , V. Sola , S. Spannagel , R. Walsh , A. Zuber , H. Biskop , P. Buhmann , M. Centis-Vignali , E. Garutti , J. Haller , M. Hoffmann , R. Klanner , T. Lapsien , M. Matysek , A. Perieanu , Ch. Scharf , P. Schleper , A. Schmidt , J. Schwandt , J. Sonneveld , G. Steinbrück , B. Vormwald , J. Wellhausen , M. Abbas , C. Amstutz , T. Barvich , Ch. Barth , F. Boegelspacher , W. De Boer , E. Butz , M. Casele , F. Colombo , A. Dierlamm , B. Freund , F. Hartmann , S. Heindl , U. Husemann , A. Kornmeyer , S. Kudella , Th. Muller , H. J. Simonis , P. Steck , M. Weber , Th. Weiler , T. Kiss , F. Siklér , T. Tölyhi , V. Veszprémi , P. Cariola , D. Creanza , M. De Palma , G. De Robertis , L. Fiore , M. Franco , F. Loddo , G. Sala , L. Silvestris , G. Maggi , S. My , G. Selvaggi , S. Albergo , G. Cappello , S. Costa , A. Di Mattia , F. Giordano , R. Potenza , M. A. Saizu , A. Tricomi , C. Tuve , E. Focardi , M. E. Dinardo , S. Fiorendi , S. Gennai , S. Malvezzi , R. A. Manzoni , D. Menasce , L. Moroni , D. Pedrini , P. Azzi , N. Bacchetta , D. Bisello , M. Dall'Osso , N. Pozzobon , M. Tosi , L. Alunni Solestizi , M. Biasini , G. M. Bilei , C. Cecchi , B. Checcucci , D. Ciangottini , L. Fanò , C. Gentsos , M. Ionica , R. Leonardi , E. Manoni , G. Mantovani , S. Marconi , V. Mariani , M. Menichelli , A. Modak , A. Morozzi , F. Moscatelli , D. Passeri , P. Placidi , V. Postolache , A. Rossi , A. Saha , A. Santocchia , L. Storchi , D. Spiga , K. Androsov , P. Azzurri , G. Bagliesi , A. Basti , T. Boccali , L. Borrello , F. Bosi , R. Castaldi , M. Ceccanti , M. A. Ciocci , R. Dell'Orso , S. Donato , G. Fedi , A. Giassi , M. T. Grippo , F. Ligabue , G. Magazzu , P. Mammini , F. Mariani , E. Mazzoni , A. Messineo , A. Moggi , F. Morsani , F. Palla , F. Palmonari , A. Profeti , F. Raffaelli , A. Ragonesi , A. Rizzi , A. Soldani , P. Spagnolo , R. Tenchini , G. Tonelli , A. Venturi , P. G. Verdini , D. Abbaneo , I. Ahmed , E. Albert , G. Auzinger , G. Berruti , J. Bonnaud , J. Daguin , A. D'Auria , S. Detraz , O. Dondelewski , B. Engegaard , F. Faccio , N. Frank , K. Gill , A. Honma , A. Kornmayer , A. Labaza , F. Manolescu , I. McGill , S. Mersi , S. Michelis , A. Onnela , M. Ostrega , S. Pavis , A. Peisert , J. -F. Pernot , P. Petagna , H. Postema , K. Rapacz , C. Sigaud , P. Tropea , J. Troska , A. Tsirou , F. Vasey , B. Verlaat , P. Vichoudis , L. Zwalinski , F. Bachmair , R. Becker , D. di Calafiori , B. Casal , P. Berger , L. Djambazov , M. Donega , C. Grab , D. Hits , J. Hoss , G. Kasieczka , W. Lustermann , B. Mangano , M. Marionneau , P. Martinez Ruiz del Arbol , M. Masciovecchio , M. Meinhard , L. Perozzi , U. Roeser , A. Starodumov , V. Tavolaro , R. Wallny , D. Zhu , K. Bösiger , L. Caminada , F. Canelli , V. Chiochia , A. de Cosa , C. Galloni , T. Hreus , B. Kilminster , C. Lange , R. Maier , J. Ngadiuba , D. Pinna , P. Robmann , S. Taroni , Y. Yang , W. Bertl , K. Deiters , W. Erdmann , R. Horisberger , H. -C. Kaestli , D. Kotlinski , U. Langenegger , B. Meier , T. Rohe , S. Streuli , P. -H. Chen , C. Dietz , F. Fiori , U. Grundler , W. -S. Hou , R. -S. Lu , M. Moya , J. -F. Tsai , Y. M. Tzeng , D. Cussans , J. Goldstein , M. Grimes , D. Newbold , P. Hobson , I. D. Reid , G. Auzinger , R. Bainbridge , P. Dauncey , G. Hall , T. James , A. -M. Magnan , M. Pesaresi , D. M. Raymond , K. Uchida , T. Durkin , K. Harder , C. Shepherd-Themistocleous , M. Chertok , J. Conway , R. Conway , C. Flores , R. Lander , D. Pellett , F. Ricci-Tam , M. Squires , J. Thomson , R. Yohay , K. Burt , J. Ellison , G. Hanson , M. Olmedo , W. Si , B. R. Yates , A. Dominguez , R. Bartek , B. Bentele , J. P. Cumalat , W. T. Ford , F. Jensen , A. Johnson , M. Krohn , S. Leontsinis , T. Mulholland , K. Stenson , S. R. Wagner , A. Apresyan , G. Bolla , K. Burkett , J. N. Butler , A. Canepa , H. W. K. Cheung , D. Christian , W. E. Cooper , G. Deptuch , G. Derylo , C. Gingu , S. Grünendahl , S. Hasegawa , J. Hoff , J. Howell , M. Hrycyk , S. Jindariani , M. Johnson , F. Kahlid , S. Kwan , C. M. Lei , R. 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In Run 3 of the LHC, the instantaneous luminosity at the LHCb interaction point has been increased by a factor of five, from $4\times 10^{32}\rm{cm}^{-2}\rm{s}^{-1}$ to $2\times 10^{33}\rm{cm}^{-2}\rm{s}^{-1}$. Several hardware…

In these proceedings we review the physics objects used by the CMS experiment during LHC Run 3 at 13.6 TeV, including charged leptons, photons, jets, and missing transverse momentum. Their performance and calibration is critical for physics…

High Energy Physics - Experiment · Physics 2026-01-28 Markus Seidel

The High-Luminosity LHC (HL-LHC) will usher in a new era in high-energy physics. The HL-LHC experimental conditions entail an instantaneous luminosity of up to $7.5 \times 10^{34}$ cm$^{-2}$ s$^{-1}$ and up to 200 simultaneous collisions…

High Energy Physics - Experiment · Physics 2022-11-17 Thiago R. F. P. Tomei

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

Instrumentation and Detectors · Physics 2018-04-03 Tamas Almos Vami , Viktor Veszpremi , the CMS Collaboration

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

Instrumentation and Detectors · Physics 2019-10-01 Tamas Almos Vami

The Large Hadron Collider is currently undergoing its High Luminosity upgrade, which is set to increase the instantaneous luminosity by about a factor of five. Consequently, the Compact Muon Solenoid experiment is upgrading its muon…

Instrumentation and Detectors · Physics 2022-05-18 Stephen D. Butalla , Marcus Hohlmann

The trigger systems of the CERN LHC detectors play a crucial role in determining the physics capabilities of the experiments. A reduction of several orders of magnitude of the event rate is needed to reach values compatible with the…

Instrumentation and Detectors · Physics 2014-09-18 Juliette Alimena

The High Luminosity upgrade of the CERN Large Hadron Collider (HL-LHC) requires new high-radiation tolerant silicon pixel sensors for the innermost part of the tracking detector in the CMS experiment. The innermost layer of the tracker,…

High Energy Physics - Experiment · Physics 2025-02-11 Clara Lasaosa