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The High-Luminosity LHC (HL-LHC) will provide the unique opportunity to explore the nature of physics beyond the Standard Model of strong and electroweak interactions. Highly selective first-level triggers are essential for the physics…

Instrumentation and Detectors · Physics 2017-02-01 S. Abovyan , V. Danielyan , M. Fras , P. Gadow , O. Kortner , S. Kortner , H. Kroha , F. Mueller , S. Nowak , R. Richter , K. Schmidt-Sommerfeld

The performance of the three-level ATLAS muon trigger as evaluated by using LHC data is presented. Events have been selected by using only the hardware-based Level-1 trigger in order to commission and to subsequently enable the…

Instrumentation and Detectors · Physics 2010-10-04 Elisa Musto

The CERN LHC provided proton and heavy ion collisions during its Run 2 operation period from 2015 to 2018. Proton-proton collisions reached a peak instantaneous luminosity of 2.1 $\times$ 10$^{34}$ cm$^{-2}$s$^{-1}$, twice the initial…

Instrumentation and Detectors · Physics 2024-11-26 CMS Collaboration

Among the many challenges presented by the future ATLAS detector at the LHC are the high data taking rate and volume and the derivation of a rapid trigger decision with limited resources. To address this challenge within the ATLAS second…

Computational Physics · Physics 2014-11-18 V. Boisvert , S. Armstrong , J. Baines , S. Brandt , M. Elsing , S. George , W. Li , A. G. Mello

The ATLAS High Level Trigger (HLT) consists of two selection steps: the second level trigger and the event filter. Both will be implemented in software, running on mostly commodity hardware. Both levels have a coherent approach to event…

Computational Physics · Physics 2014-11-18 Monika Grothe

The performance of the ATLAS muon trigger system is evaluated with proton-proton ($pp$) and heavy-ion (HI) collision data collected in Run 2 during 2015-2018 at the Large Hadron Collider. It is primarily evaluated using events containing a…

Instrumentation and Detectors · Physics 2021-01-12 ATLAS Collaboration

During the upcoming Run 3 and Run 4 at the LHC the upgraded ALICE (A Large Ion Collider Experiment) will operate at a significantly higher luminosity and will collect two orders of magnitude more events than in Run 1 and Run 2. A part of…

Instrumentation and Detectors · Physics 2020-12-07 Alla Maevskaya

The High-Luminosity LHC will provide the unique opportunity to explore the nature of physics beyond the Standard Model of strong and electroweak interactions. Highly selective first level triggers are essential for the physics programme of…

The online event selection is crucial to reject most of the events containing uninteresting background collisions while preserving as much as possible the interesting physical signals. The b-jet selection is part of the trigger strategy of…

High Energy Physics - Experiment · Physics 2011-11-18 Per Hansson

In this paper a conceptual overview is given of the software foreseen to configure the ATLAS trigger system. Two functional software prototypes have been developed to configure the ATLAS Level-1 emulation and the High-Level Trigger…

Instrumentation and Detectors · Physics 2007-05-23 M. Elsing , T. Schoerner-Sadenius

During the 2015-2018 data-taking period, the Large Hadron Collider delivered proton-proton bunch crossings at a centre-of-mass energy of 13 TeV to the ATLAS experiment at a rate of roughly 30 MHz, where each bunch crossing contained an…

High Energy Physics - Experiment · Physics 2024-12-24 ATLAS Collaboration

The ATLAS detector at CERN's Large Hadron Collider will be exposed to proton-proton collisions from beams crossing at 40 MHz that have to be reduced to the few 100 Hz allowed by the storage systems. A three-level trigger system has been…

Instrumentation and Detectors · Physics 2008-11-26 A. dos Anjos , N. Ellis , J. Haller , A. Hoecker , T. Kohno , M. Landon , H. von der Schmitt , R. Spiwoks , T. Wengler , W. Wiedenmann , H. Zobernig

The CMS experiment has been designed with a 2-level trigger system: the Level 1 Trigger, implemented on custom-designed electronics, and the High Level Trigger (HLT), a streamlined version of the CMS offline reconstruction software running…

Instrumentation and Detectors · Physics 2015-06-19 Valentina Gori

Clusters of topologically connected calorimeter cells around cells with large absolute signal-to-noise ratio (topo-clusters) are the basis for calorimeter signal reconstruction in the ATLAS experiment. Topological cell clustering has proven…

Instrumentation and Detectors · Physics 2024-05-08 ATLAS Collaboration

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

A sophisticated trigger system, capable of real-time track reconstruction, is used in the ATLAS experiment to select interesting events in the proton-proton collisions at the Large Hadron Collider at CERN. A set of $b$-jet triggers was…

High Energy Physics - Experiment · Physics 2015-06-03 Andrea Coccaro

The ATLAS detector at CERN's Large Hadron Collider will be exposed to proton-proton collisions from beams crossing at 40 MHz. A three-level trigger system was designed to select potentially interesting events and reduce the incoming rate to…

Instrumentation and Detectors · Physics 2008-11-26 Thilo Pauly

The Phase-I trigger readout electronics upgrade of the ATLAS Liquid Argon calorimeters enhances the physics reach of the experiment during the upcoming operation at increasing Large Hadron Collider luminosities. The new system, installed…

Instrumentation and Detectors · Physics 2022-05-17 G. Aad , A. V. Akimov , K. Al Khoury , M. Aleksa , T. Andeen , C. Anelli , N. Aranzabal , C. Armijo , A. Bagulia , J. Ban , T. Barillari , F. Bellachia , M. Benoit , F. Bernon , A. Berthold , H. Bervas , D. Besin , A. Betti , Y. Bianga , M. Biaut , D. Boline , J. Boudreau , T. Bouedo , N. Braam , M. Cano Bret , G. Brooijmans , H. Cai , C. Camincher , A. Camplani , S. Cap , A. Carbone , J. W. S. Carter , S. V. Chekulaev , H. Chen , K. Chen , N. Chevillot , M. Citterio , B. Cleland , M. Constable , S. de Jong , A. M. Deiana , M. Delmastro , B. Deng , H. Deschamps , C. Diaconu , A. Dik , B. Dinkespiler , N. Dumont Dayot , A. Emerman , Y. Enari , P. J. Falke , J. Farrell , W. Fielitz , E. Fortin , J. Fragnaud , S. Franchino , L. Gantel , K. Gigliotti , D. Gong , A. Grabas , P. Grohs , N. Guettouche , T. Guillemin , D. Guo , J. Guo , L. Hasley , C. Hayes , R. Hentges , L. Hervas , M. Hils , J. Hobbs , A. Hoffman , D. Hoffmann , P. Horn , T. Hryn'ova , L. Iconomidou-Fayard , R. Iguchi , T. James , K. Johns , T. Junkermann , C. Kahra , E. F. Kay , R. Keeler , S. Ketabchi Haghighat , P. Kinget , E. Knoops , A. Kolbasin , P. Krieger , J. Kuppambatti , L. L. Kurchaninov , E. Ladygin , S. Lafrasse , M. P. J. Landon , F. Lanni , S. Latorre , D. Laugier , M. Lazzaroni , X. Le , P. Le Bourlout , C. A. Lee , M. Lefebvre , M. A. L. Leite , C. Leroy , X. Li , Z. Li , F. Liang , H. Liu , C. Liu , T. Liu , H. Ma , L. L. Ma , D. J. Mahon , U. Mallik , B. Mansoulie , A. L. Maslennikov , N. Matsuzawa , R. A. McPherson , S. Menke , A. Milic , Y. Minami , E. Molina , E. Monnier , N. Morange , L. Morvaj , J. Mueller , C. Mwewa , R. Narayan , N. Nikiforou , I. Ochoa , R. Oishi , D. Oliveira Damazio , R. E. Owen , C. Pancake , D. K. Panchal , G. Perrot , M. -A. Pleier , P. Poffenberger , R. Porter , S. Quan , J. Rabel , A. Roy , J. P. Rutherfoord , F. Sabatini , F. Salomon , E. Sauvan , A. C. Schaffer , R. D. Schamberger , Ph. Schwemling , C. Secord , L. Selem , K. Sexton , E. Shafto , M. V. Silva Oliveira , S. Simion , S. Singh , W. Sippach , A. A. Snesarev , S. Snyder , M. Spalla , S. Stärz , A. Straessner , P. Strizenec , R. Stroynowski , V. V. Sulin , J. Tanaka , S. Tang , S. Tapprogge , G. F. Tartarelli , G. Tateno , K. Terashi , S. Tisserant , D. Tompkins , G. Unal , M. Unal , K. Uno , A. Vallier , S. Vieira de Souza , R. Walker , Q. Wang , C. Wang , R. Wang , M. Wessels , I. Wingerter-Seez , K. Wolniewicz , W. Wu , Z. Xiandong , R. Xu , H. Xu , S. Yamamoto , Y. Yang , J. Ye , H. Zaghia , J. Zang , T. Zhang , H. L. Zhu , V. Zhulanov , E. Zonca , G. Zuk

The outer shell of the ATLAS experiment at the LHC consists of a system of toroidal air-core magnets in order to allow for the precise measurement of the transverse momentum p$_T$ of muons, which in many physics channels are a signature of…

Instrumentation and Detectors · Physics 2011-01-27 Jörg Dubbert , Sandra Horvat , Oliver Kortner , Hubert Kroha , Robert Richter

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