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The Compact Muon Solenoid (CMS) detector at the CERN Large Hadron Collider (LHC) is undergoing an extensive Phase II upgrade program to prepare for the challenging conditions of the High-Luminosity LHC (HL-LHC). A new timing layer is…

仪器与探测器 · 物理学 2018-10-02 Irene Dutta

As part of the Phase II upgrade program, the Compact Muon Solenoid (CMS) detector will incorporate a new timing layer designed to measure minimum ionizing particles (MIPs) with a time resolution of $\sim$30 ps. Precision timing will…

仪器与探测器 · 物理学 2018-11-27 Olmo Cerri

The CMS detector will be upgraded for the HL-LHC to include a MIP Timing Detector (MTD). The MTD will consist of barrel and endcap timing layers, BTL and ETL respectively, providing precision timing of charged particles. The BTL sensors are…

The CMS-TOTEM Precision Proton Spectrometer (CT-PPS) is an approved project to add tracking and timing information at approximately $\pm$210~m from the interaction point around the CMS detector. It is designed to operate at high luminosity…

仪器与探测器 · 物理学 2017-04-05 Michele Gallinaro

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 $7.5 \times 10^{34} \text{cm}^{-2} \text{s}^{-1}$…

仪器与探测器 · 物理学 2023-01-26 Sascha Liechti

The PhaseII Upgrades of CMS are being planned for the High Luminosity LHC (HL-LHC) era when the mean number of interactions per beam crossing ("in-time pileup") is expected to reach ~140-200. The potential backgrounds arising from…

仪器与探测器 · 物理学 2014-09-18 Sebastian N. White

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$^{-1}$…

仪器与探测器 · 物理学 2020-04-22 Alessandro La Rosa

The MIP Timing Detector will provide additional timing capabilities for detection of minimum ionizing particles (MIPs) at CMS during the High Luminosity LHC era, improving event reconstruction and pileup rejection. The central portion of…

仪器与探测器 · 物理学 2021-07-19 R. Abbott , A. Abreu , F. Addesa , M. Alhusseini , T. Anderson , Y. Andreev , A. Apresyan , R. Arcidiacono , M. Arenton , E. Auffray , D. Bastos , L. A. T. Bauerdick , R. Bellan , M. Bellato , A. Benaglia , M. Benettoni , R. Bertoni , M. Besancon , S. Bharthuar , A. Bornheim , E. Brücken , J. N. Butler , C. Campagnari , M. Campana , R. Carlin , P. Carniti , N. Cartiglia , M. Casarsa , O. Cerri , P. Checchia , H. Chen , S. Chidzik , F. Chlebana , F. Cossutti , M. Costa , B. Cox , I. Dafinei , F. De Guio , P. Debbins , D. del Re , A. Dermenev , E. Di Marco , K. Dilsiz , K. F. Di Petrillo , G. Dissertori , S. Dogra , U. Dosselli , I. Dutta , F. Caleb , C. Fernandez Madrazo , M. Fernandez , M. Ferrero , Z. Flowers , W. Funk , M. Gallinaro , S. Ganjour , M. Gardner , F. Geurts , A. Ghezzi , S. Gninenko , F. Golf , J. Gonzalez , C. Gotti , L. Gray , F. Guilloux , S. Gundacker , E. Hazen , S. Hedia , A. Heering , R. Heller , T. Isidori , R. Isocrate , R. Jaramillo , M. Joyce , K. Kaadze , A. Karneyeu , H. Kim , J. King , G. Kopp , M. Korjik , O. K. Koseyan , A. Kozyrev , N. Kratochwil , M. Lazarovits , A. Ledovskoy , H. Lee , J. Lee , A. Li , S. Li , W. Li , T. Liu , N. Lu , M. Lucchini , W. Lustermann , C. Madrid , M. Malberti , I. Mandjavize , J. Mao , Y. Maravin , D. Marlow , B. Marsh , P. Martinez del Arbol , B. Marzocchi , R. Mazza , C. McMahon , V. Mechinsky , P. Meridiani , A. Mestvirishvili , N. Minafra , A. Mohammadi , F. Monti , C. S. Moon , R. Mulargia , M. Murray , Y. Musienko , J. Nachtman , S. Nargelas , L. Narvaez , O. Neogi , C. Neu , T. Niknejad , M. Obertino , H. Ogul , G. Oh , I. Ojalvo , Y. Onel , G. Organtini , T. Orimoto , J. Ott , I. Ovtin , M. Paganoni , F. Pandolfi , R. Paramatti , A. Peck , C. Perez , G. Pessina , C. Pena , S. Pigazzini , O. Radchenko , N. Redaelli , D. Rigoni , E. Robutti , C. Rogan , R. Rossin , C. Rovelli , C. Royon , M. Ö. Sahin , W. Sands , F. Santanastasio , U. Sarica , I. Schmidt , R. Schmitz , J. Sheplock , J. C. Silva , F. Siviero , L. Soffi , V. Sola , G. Sorrentino , M. Spiropulu , D. Spitzbart , A. G. Stahl Leiton , A. Staiano , D. Stuart , I. Suarez , T. Tabarelli de Fatis , G. Tamulaitis , Y. Tang , B. Tannenwald , R. Taylor , E. Tiras , M. Titov , S. Tkaczyk , D. Tlisov , I. Tlisova , M. Tornago , M. Tosi , R. Tramontano , J. Trevor , C. G. Tully , B. Ujvari , J. Varela , S. Ventura , I. Vila , T. Wamorkar , C. Wang , X. Wang , M. Wayne , J. Wetzel , S. White , D. Winn , S. Wu , S. Xie , Z. Ye , G. B. Yu , G. Zhang , L. Zhang , Y. Zhang , Z. Zhang , R. Zhu

Precision timing has played a critical role in high-energy physics experiments, particularly for particle identification and the suppression of pileup under the challenging conditions expected at future colliders like the High-Luminosity…

仪器与探测器 · 物理学 2026-03-31 Martina Malberti , Xiaohu Sun

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…

高能物理 - 实验 · 物理学 2022-11-17 Thiago R. F. P. Tomei

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…

高能物理 - 实验 · 物理学 2025-01-08 Thiago R. F. P. Tomei

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…

仪器与探测器 · 物理学 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

The barrel section of the novel MIP Timing Detector (MTD) will be constructed as part of the upgrade of the CMS experiment to provide a time resolution for single charged tracks in the range of $30-60$ ps using LYSO:Ce crystal arrays read…

A full replacement of the existing muon trigger system in the CMS (Compact Muon Solenoid) detector is planned for operating at the maximum instantaneous luminosities of about $5-7.5\times10^{34}$ cm$^{-2}$ s$^{-1}$ expected in HL-LHC (High…

仪器与探测器 · 物理学 2019-11-01 Silvia Goy López

During the High Luminosity programme of the LHC collider (called HL-LHC), planned to start in 2030, the instantaneous luminosity will be increased from \num{\sim 2e34}~\si{cm^{-2}s^{-1}} to an unprecedented figure of about \num{\sim…

仪器与探测器 · 物理学 2025-09-07 Lorenzo Damenti

The high-luminosity phase of LHC operations (HL-LHC), will feature a large increase in simultaneous proton-proton interactions per bunch crossing up to 200, compared with a typical leveling target of 64 in Run 3. Such an increase will…

高能物理 - 实验 · 物理学 2025-02-25 ATLAS Collaboration

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…

仪器与探测器 · 物理学 2013-10-08 Sebastian White

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…

仪器与探测器 · 物理学 2022-12-21 A. La Rosa , I. Ahmed , J. Almeida , G. Blanchot , S. Cooperstein , I. Dominguez , A. Honma , M. Kovacs , A. Zografos

The upgrades of ATLAS and CMS for the High Luminosity LHC (HL-LHC) highlighted physics objects timing as a tool to resolve primary interactions within a bunch crossing. Since the expected pile-up is around 200, with an r.m.s. time spread of…

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