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Related papers: The Trigger System of the CMS Experiment

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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

The large ttbar production cross-section at the LHC suggests the use of top quark decays to calibrate several critical parts of the detectors, such as the trigger system, the jet energy scale and b-tagging.

High Energy Physics - Experiment · Physics 2010-11-11 B. S. Acharya , F. Cavallari , G. Corcella , R. Di Sipio , G. Petrucciani

The CMS High-Level Trigger (HLT) is responsible for ensuring that data samples with potentially interesting events are recorded with high efficiency and good quality. This paper gives an overview of the HLT and focuses on its commissioning…

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

Energy constraint long-range wireless sensor/ actuator based solutions are theoretically the perfect choice to support the next generation of city-scale cyber-physical systems. Traditional systems adopt periodic control which increases…

Systems and Control · Computer Science 2016-11-15 Sokratis Kartakis , Anqi Fu , Manuel Mazo , Julie A. McCann

The Compact Muon Solenoid (CMS) experiment prepares its Phase-2 upgrade for the high-luminosity era of the LHC operation (HL-LHC). Due to the increase of occupancy, trigger latency and rates, the full electronics of the CMS Drift Tube (DT)…

High Energy Physics - Experiment · Physics 2023-02-06 G. Abbiendi , J. Alcaraz Maestre , A. Álvarez Fernández , B. Álvarez González , N. Amapane , I. Bachiller , L. Barcellan , C. Baldanza , C. Battilana , M. Bellato , G. Bencze , M. Benettoni , N. Beni , A. Benvenuti , A. Bergnoli , L. C. Blanco Ramos , L. Borgonovi , A. Bragagnolo , V. Cafaro , A. Calderon , E. Calvo , R. Carlin , C. A. Carrillo Montoya , F. R. Cavallo , J. M. Cela Ruiz , M. Cepeda , M. Cerrada , P. Checchia , L. Ciano , N. Colino , D. Corti , G. Cotto , A. Crupano , S. Cuadrado Calzada , J. Cuevas , M. Cuffiani , G. M. Dallavalle , D. Dattola , B. De La Cruz , C. I. de Lara Rodríguez , P. De Remigis , C. Erice Cid , D. Eliseev , F. Fabbri , A. Fanfani , D. Fasanella , C. F. Bedoya , J. F. de Trocóniz , D. Fernández del Val , J. Fernández Menéndez , J. P. Fernández Ramos , S. Folgueras , M. C. Fouz , D. Francia Ferrero , J. García Romero , F. Gasparini , U. Gasparini , V. Giordano , 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 , K. Hoepfner , R. Isocrate , M. I. Josa , B. Kiani , J. León Holgado , S. Lo Meo , E. Lusiani , L. Lunerti , S. Marcellini , M. Margoni , C. Mariotti , I. Martín Martín , J. J. Martínez Morales , S. Maselli , G. Masetti , A. T. Meneguzzo , M. Merschmeyer , M. Migliorini , L. Modenese , J. Molnar , F. Montecassiano , J. Mora Martínez , D. Moran , S. Mukherjee , J. J. Navarrete , F. Navarria , A. Navarro Tobar , F. Nowotny , E. Palencia Cortezón , M. Passaseo , J. Pazzini , M. Pelliccioni , A. Perrotta , B. Philipps , J. Piedra Gomez , F. Primavera , J. Puerta Pelayo , J. C. Puras Sánchez , C. Ramón Álvarez , I. Redondo , D. D. Redondo Ferrero , H. Reithler , R. Reyes-Almanza , V. Rodríguez Bouza , P. Ronchese , A. M. Rossi , R. Rossin , F. Rotondo , T. Rovelli , S. Sánchez Cruz , S. Sánchez Navas , J. Sastre , A. Sharma , F. Simonetto , A. Soto Rodríguez , A. Staiano , Z. Szillasi , D. F. Teyssier , N. Toniolo , G. Torromeo , A. Trapote , N. Trevisani , A. Triossi , D. Trocino , B. Ujvari , G. Umoret , L. Urda Gómez , B. Uwe , S. Ventura , C. Vico Villalba , S. Wiedenbeck , M. Zanetti , F. P. Zantis , G. Zilizi , P. Zotto , A. Zucchetta

The Physics and Data Quality Monitoring (DQM) framework aims at providing a homogeneous monitoring environment across various applications related to data taking at the CMS experiment. In this contribution, the DQM system for the Silicon…

Instrumentation and Detectors · Physics 2010-11-19 Leonardo Benucci

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

A new pixel detector for the CMS experiment is being built, owing to the instantaneous luminosities anticipated for the Phase I Upgrade of the LHC. The new CMS pixel detector provides four-hit tracking while featuring a significantly…

Instrumentation and Detectors · Physics 2016-12-23 Simon Spannagel

Highly selective triggers are essential for the physics programme of the ATLAS experiment at HL-LHC where the instantaneous luminosity will be about an order of magnitude larger than the LHC instantaneous luminosity in Run 1. The first…

Instrumentation and Detectors · Physics 2016-10-04 H. Kroha , S. Nowak

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…

This paper presents a streamlined framework for real-time processing and analysis of condition data from the CMS experiment Resistive Plate Chambers (RPC). Leveraging data streaming, it uncovers correlations between RPC performance metrics,…

High Energy Physics - Experiment · Physics 2025-04-15 A. Dimitrov , M. Tytgat , K. Mota Amarilo , A. Samalan , K. Skovpen , G. A. Alves , E. Alves Coelho , F. Marujo da Silva , M. Barroso Ferreira Filho , E. M. Da Costa , D. De Jesus Damiao , S. Fonseca De Souza , R. Gomes De Souza , L. Mundim , H. Nogima , J. P. Pinheiro , A. Santoro , M. Thiel , A. Aleksandrov , R. Hadjiiska , P. Iaydjiev , M. Shopova , G. Sultanov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , E. Shumka , P. Cao , W. Diao , Q. Hou , H. Kou , Z. -A. Liu , J. Song , J. Zhao , S. J. Qian , C. Avila , D. A. Barbosa Trujillo , A. Cabrera , C. A. Florez , J. A. Reyes Vega , R. Aly , A. Radi , Y. Assran , I. Crotty , M. A. Mahmoud , M. Gouzevitch , G. Grenier , I. B. Laktineh , L. Mirabito , I. Bagaturia , I. Lomidze , Z. Tsamalaidze , V. Amoozegarp , B. Boghrati , M. Ebrahimi , F. Esfandi , Y. Hosseini , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , N. De Filippis , G. Iaselli , F. Loddo , G. Pugliese , D. Ramos , L. Benussi , S. Bianco , S. Meola , D. Piccolo , S. Buontempo , F. Carnevali , F. Fienga , L. Lista , P. Paolucci , A. Braghieri , P. Montagna , C. Riccardi , P. Salvini , P. Vitulo , E. Asilar , T. J. Kim , Y. Ryou , S. Choi , B. Hong , K. S. Lee , J. Goh , J. Shin , Y. Lee , I. Pedraza , C. Uribe Estrada , H. Castilla-Valdez , R. Lopez-Fernandez , A. Sanchez Hernandez , M. Ramirez Garcia , D. L. Ramirez Guadarrama , M. A. Shah , E. Vazquez , N. Zaganidis , A. Ahmad , M. I. Asghar , H. R. Hoorani , S. Muhammad , J. Eysermans

The LHC machine at CERN finished its first year of pp collisions at a center of mass energy of 7 TeV. While the commissioning to exploit its full potential is still ongoing, there are plans to upgrade its components to reach instantaneous…

Instrumentation and Detectors · Physics 2011-03-22 Hans-Christian Kästli

The CMS muon system includes in both the barrel and endcap region Resistive Plate Chambers (RPC). They mainly serve as trigger detectors and also improve the reconstruction of muon parameters. Over the years, the instantaneous luminosity of…

An FPGA-based online trigger system has been developed for the COMET Phase-I experiment. This experiment searches for muon-to-electron conversion, which has never been observed yet. A drift chamber and trigger counters detect a…

A data acquisition (DAQ) system has been developed which will read out and control calorimeters serving as prototype systems for a future detector at an electron-positron linear collider. This is a modular, flexible and scalable DAQ system…

In the first phase of LHC data-taking ATLAS will measure the charged-particle density at the initial center-of-mass energy of 10 TeV and then at 14 TeV. This will allow us improve our knowledge of soft QCD models and pin-down cross-sections…

High Energy Physics - Experiment · Physics 2008-12-04 Regina Kwee

The LHC machine is planning an upgrade program, which will smoothly bring the instantaneous luminosity to about $5-7.5\times10^{34}~\mathrm{cm}^{-2}\mathrm{s}^{-1}$ in 2028, to possibly reach an integrated luminosity of 3000-4500 fb$^{-1}$…

Instrumentation and Detectors · Physics 2019-11-07 Ernesto Migliore

We discuss how the CMS and ATLAS experiments are preparing for the analysis of first LHC data with emphasis on the search for supersymmetry. We will show the importance of the understanding of detector, trigger, reconstruction and…

High Energy Physics - Experiment · Physics 2009-02-02 Paul de Jong

Data-intensive science is increasingly reliant on real-time processing capabilities and machine learning workflows, in order to filter and analyze the extreme volumes of data being collected. This is especially true at the energy and…

Artificial Intelligence · Computer Science 2021-04-21 Chinmaya Mahesh , Kristin Dona , David W. Miller , Yuxin Chen