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Related papers: The CMS Trigger Upgrade for the HL-LHC

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The factor of four increase in the LHC luminosity, from $0.5\times 10^{34}\,\textrm{cm}^{-2}\textrm{s}^{-1}$ to $2.0\times 10^{34}\textrm{cm}^{-2}\textrm{s}^{-1}$, and the corresponding increase in pile-up collisions during the 2015-2018…

High Energy Physics - Experiment · Physics 2021-01-12 ATLAS Collaboration

In hadron collider experiments, triggering the detector to store interesting events for offline analysis is a challenge due to the high rates and multiplicities of particles produced. Maintaining high trigger efficiency for the physics we…

High Energy Physics - Experiment · Physics 2019-08-13 Mark S. Neubauer

We report on the design and test results of a prototype processor for the CMS Level-1 trigger that performs 3-D track reconstruction and measurement from data recorded by the cathode strip chambers of the endcap muon system. The tracking…

Instrumentation and Detectors · Physics 2007-05-23 D. Acosta , V. Golovtsov , M. Kan , A. Madorsky , B. Scurlock , H. Stoeck , L. Uvarov , S. M. Wang

ALICE (A Large Heavy Ion Experiment) is one of the four major experiments at the Large Hadron Collider (LHC) at CERN. The High Level Trigger (HLT) is an online compute farm which reconstructs events measured by the ALICE detector in…

Instrumentation and Detectors · Physics 2019-08-14 David Rohr , Sergey Gorbunov , Volker Lindenstruth

The CMS collaboration used the past year to greatly improve the level of detector readiness for the first collisions data. The acquired operational experience over this year, large gains in understanding the detector and improved…

High Energy Physics - Experiment · Physics 2010-03-23 A. Safonov

The expected radiation background in the CMS RPC system has been studied using the MC prediction with the CMS FLUKA simulation of the detector and the cavern. The MC geometry used in the analysis describes very accurately the present RPC…

Instrumentation and Detectors · Physics 2020-12-15 R. Hadjiiska , A. Samalan , M. Tytgat , N. Zaganidis , G. A. Alves , F. Marujo , F. Torres Da Silva De Araujo , E. M. Da Costa , D. De Jesus Damiao , H. Nogima , A. Santoro , S. Fonseca De Souza , A. Aleksandrov , P. Iaydjiev , M. Rodozov , M. Shopova , G. Sultanov , M. Bonchev , A. Dimitrov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , S. J. Qian , C. Bernal , A. Cabrera , J. Fraga , A. Sarkar , S. Elsayed , Y. Assran , M. El Sawy , M. A. Mahmoud , Y. Mohammed , C. Combaret , M. Gouzevitch , G. Grenier , I. Laktineh , L. Mirabito , K. Shchablo , I. Bagaturia , D. Lomidze , I. Lomidze , V. Bhatnagar , R. Gupta , P. Kumari , J. Singh , V. Amoozegar , B. Boghrati , M. Ebraimi , R. Ghasemi , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , R. Aly , W. Elmetenawee , N. De Filippis , A. Gelmi , G. Iaselli , S. Leszki , F. Loddo , I. Margjeka , G. Pugliese , D. Ramos , M. Caponero , L. Benussi , S. Bianco , S. Colafranceschi , A. Russo , L. Passamonti , D. Piccolo , D. Pierluigi , G. Saviano , S. Buontempo , A. Di Crescenzo , F. Fienga , G. De Lellis , L. Lista , S. Meola , P. Paolucci , A. Braghieri , P. Salvini , P. Montagna , C. Riccardi , P. Vitulo , B. Francois , T. J. Kim , J. Park , S. Y. Choi , B. Hong , K. S. Lee , J. Goh , H. Lee , J. Eysermans , C. Uribe Estrada , I. Pedraza , H. Castilla-Valdez , A. Sanchez-Hernandez , C. A. Mondragon Herrera , D. A. Perez Navarro , G. A. Ayala Sanchez , S. Carrillo , E. Vazquez , A. Radi , A. Ahmad , I. Asghar , H. Hoorani , S. Muhammad , M. A. Shah , I. Crotty

The LHCb experiment at CERN is undergoing an upgrade in preparation for the Run 3 data taking period of the LHC. As part of this upgrade the trigger is moving to a fully software implementation operating at the LHC bunch crossing rate. We…

Instrumentation and Detectors · Physics 2022-01-06 R. Aaij , M. Adinolfi , S. Aiola , S. Akar , J. Albrecht , M. Alexander , S. Amato , Y. Amhis , F. Archilli , M. Bala , G. Bassi , L. Bian , M. P. Blago , T. Boettcher , A. Boldyrev , S. Borghi , A. Brea Rodriguez , L. Calefice , M. Calvo Gomez , D. H. Cámpora Pérez , A. Cardini , M. Cattaneo , V. Chobanova , G. Ciezarek , X. Cid Vidal , J. L. Cobbledick , J. A. B. Coelho , T. Colombo , A. Contu , B. Couturier , D. C. Craik , R. Currie , P. d'Argent , M. De Cian , D. Derkach , F. Dordei , M. Dorigo , L. Dufour , P. Durante , A. Dziurda , A. Dzyuba , S. Easo , S. Esen , P. Fernandez Declara , S. Filippov , C. Fitzpatrick , M. Frank , P. Gandini , V. V. Gligorov , E. Golobardes , G. Graziani , L. Grillo , P. A. Günther , S. Hansmann-Menzemer , A. M. Hennequin , L. Henry , D. Hill , S. E. Hollitt , J. Hu , W. Hulsbergen , R. J. Hunter , M. Hushchyn , B. K. Jashal , C. R. Jones , S. Klaver , K. Klimaszewski , R. Kopecna , W. Krzemien , M. Kucharczyk , R. Lane , F. Lazzari , R. Le Gac , P. Li , J. H. Lopes , M. Lucio Martinez , A. Lupato , O. Lupton , X. Lyu , F. Machefert , O. Madejczyk , S. Malde , J. F. Marchand , S. Mariani , C. Marin Benito , D. Martinez Santos , F. Martinez Vidal , R. Matev , M. Mazurek , B. Mitreska , D. S. Mitzel , M. J. Morello , H. Mu , P. Muzzetto , P. Naik , M. Needham , N. Neri , N. Neufeld , N. S. Nolte , D. O'Hanlon , A. Oyanguren , M. Pepe Altarelli , S. Petrucci , M. Petruzzo , L. Pica , F. Pisani , A. Piucci , F. Polci , A. Poluektov , E. Polycarpo , C. Prouve , G. Punzi , R. Quagliani , R. I. Rabadan Trejo , M. Ramos Pernas , M. S. Rangel , F. Ratnikov , G. Raven , F. Reiss , V. Renaudin , P. Robbe , A. Ryzhikov , M. Santimaria , M. Saur , M. Schiller , R. Schwemmer , B. Sciascia , A. Solomin , F. Suljik , N. Skidmore , M. D. Sokoloff , P. Spradlin , M. Stahl , S. Stahl , H. Stevens , L. Sun , A. Szabelski , T. Szumlak , M. Szymanski , D. Y. Tou , G. Tuci , A. Usachov , N. Valls Canudas , R. Vazquez Gomez , S. Vecchi , M. Vesterinen , X. Vilasis-Cardona , D. Vom Bruch , Z. Wang , T. Wojton , M. Whitehead , M. Williams , M. Witek , Y. Xie , A. Xu , H. Yin , M. Zdybal , O. Zenaiev , D. Zhang , L. Zhang , X. Zhu

As experiments in high energy physics aims to measure increasingly rare processes, the experiments continually strive to increase the expected signal yields. In the case of the High Luminosity upgrade of the LHC, the luminosity is raised by…

Instrumentation and Detectors · Physics 2018-05-09 Joakim Gradin , Mikael Mårtensson , Richard Brenner

Highly selective first-level triggers are essential to exploit the full physics potential of the ATLAS experiment at High-Luminosity LHC (HL-LHC). The concept for a new muon trigger stage using the precision monitored drift tube (MDT)…

Instrumentation and Detectors · Physics 2016-11-15 P. Gadow , O. Kortner , S. Kortner , H. Kroha , F. Müller , R. Richter

We describe plans for a search for long-lived particles which will become stopped by the CMS detector. We will look for the subsequent decay of these particles during time intervals where there are no $pp$ collisions in CMS: during gaps…

High Energy Physics - Experiment · Physics 2014-11-20 Fedor Ratnikov , for CMS Collaboration

A new concept, the Triplet Track Trigger (TTT), is proposed for stand-alone tracking at the first trigger level of the FCC-hh detector. The concept is based on a highly scalable monolithic pixel sensor technology and uses a very simple and…

Instrumentation and Detectors · Physics 2025-01-16 T. Kar , A. Schöning

The ALICE High-Level Trigger processes data online, to either select interesting (sub-) events, or to compress data efficiently by modeling techniques. Focusing on the main data source, the Time Projection Chamber, the architecure of the…

Instrumentation and Detectors · Physics 2009-11-10 V. Lindenstruth , C. Loizides , D. Roehrich , B. Skaali , T. Steinbeck , R. Stock , H. Tilsner , K. Ullaland , A. Vestbo , T. Vik

The CMS Resistive Plate Chamber (RPC) system has been certified for 10 years of LHC operation. In the next years, during the High luminosity LHC (HL-LHC) phase, the LHC instantaneous luminosity will increase to a factor five more than the…

Instrumentation and Detectors · Physics 2022-08-31 R. Aly

The Resistive Plate Chambers detector system at the CMS experiment at the LHC provides robustness and redundancy to the muon trigger. A total of 1056 double-gap chambers cover the pseudo-rapidity region < 1.6. The main detector parameters…

Instrumentation and Detectors · Physics 2016-05-31 Mehar Ali Shah

Collider experiments are equipped with trigger systems that rapidly inspect the physics content emerging from collisions to decide whether the resulting products are worth saving for later analysis. One crucial aspect for analyzing the…

High Energy Physics - Experiment · Physics 2026-04-14 Andrea Coccaro , Carlo Schiavi , Alessandro Zaio

The High Luminosity Large Hadron Collider (HL-LHC) will have a peak luminosity of $5\times10^{34} $cm$^{-2} $\,s$^{-1}$, five times higher than the design luminosity of the LHC. The hadronic ATLAS Tile Calorimeter TileCal) is a sampling…

Instrumentation and Detectors · Physics 2020-10-29 Eduardo Valdes Santurio

The electronics used in the data readout and triggering system for the Compact Muon Solenoid (CMS) experiment at the Large Hadron Collider (LHC) particle accelerator at CERN are exposed to high radiation levels. This radiation can cause…

The LHC upgrade is planned to enhance the instantaneous luminosity during Run 3 from 2021 through 2023. The Phase-I upgrade of the trigger readout electronics for the ATLAS Liquid Argon (LAr) Calorimeters will be installed during the second…

At the Large Hadron Collider (LHC), the trigger systems for the detectors must be able to process a very large amount of data in a very limited amount of time, so that the nominal collision rate of 40 MHz can be reduced to a data rate that…

Instrumentation and Detectors · Physics 2015-06-17 P. Lujan , V. Halyo , A. Hunt , P. Jindal , P. LeGresley
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