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Performance of the ATLAS Trigger System

The ATLAS Trigger System reduces the event rate from the bunch-crossing rate of $40 \rm \ MHz$ to an average recording rate of $200 \rm \ Hz$ by selecting high-$p_{T}$ physics events. The ATLAS Trigger is composed of three levels. The first level (L1) is implemented in custom-built electronics, the...

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Detalles Bibliográficos
Autor principal: Gabaldon, C
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1748-0221/7/01/C01092
http://cds.cern.ch/record/1401234
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author Gabaldon, C
author_facet Gabaldon, C
author_sort Gabaldon, C
collection CERN
description The ATLAS Trigger System reduces the event rate from the bunch-crossing rate of $40 \rm \ MHz$ to an average recording rate of $200 \rm \ Hz$ by selecting high-$p_{T}$ physics events. The ATLAS Trigger is composed of three levels. The first level (L1) is implemented in custom-built electronics, the two-stage High Level Trigger (HLT) is implemented in software executed on large computing farms. The L1 consists of calorimeter, muon and forward triggers to identify electron, photon, jet and muon candidates, as well as event features such as missing transverse energy. These inputs are used by the L1 Central Trigger to generate an L1 Accept (L1A) decision. L1A and timing information is sent to all sub-detectors and summary information is sent to the subsequent levels of the Trigger System. In this paper the performance of the ATLAS Trigger System in 2010 and 2011 is presented.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
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spelling cern-14012342019-09-30T06:29:59Zdoi:10.1088/1748-0221/7/01/C01092http://cds.cern.ch/record/1401234engGabaldon, CPerformance of the ATLAS Trigger SystemDetectors and Experimental TechniquesThe ATLAS Trigger System reduces the event rate from the bunch-crossing rate of $40 \rm \ MHz$ to an average recording rate of $200 \rm \ Hz$ by selecting high-$p_{T}$ physics events. The ATLAS Trigger is composed of three levels. The first level (L1) is implemented in custom-built electronics, the two-stage High Level Trigger (HLT) is implemented in software executed on large computing farms. The L1 consists of calorimeter, muon and forward triggers to identify electron, photon, jet and muon candidates, as well as event features such as missing transverse energy. These inputs are used by the L1 Central Trigger to generate an L1 Accept (L1A) decision. L1A and timing information is sent to all sub-detectors and summary information is sent to the subsequent levels of the Trigger System. In this paper the performance of the ATLAS Trigger System in 2010 and 2011 is presented.ATL-DAQ-PROC-2011-042oai:cds.cern.ch:14012342011-11-23
spellingShingle Detectors and Experimental Techniques
Gabaldon, C
Performance of the ATLAS Trigger System
title Performance of the ATLAS Trigger System
title_full Performance of the ATLAS Trigger System
title_fullStr Performance of the ATLAS Trigger System
title_full_unstemmed Performance of the ATLAS Trigger System
title_short Performance of the ATLAS Trigger System
title_sort performance of the atlas trigger system
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1088/1748-0221/7/01/C01092
http://cds.cern.ch/record/1401234
work_keys_str_mv AT gabaldonc performanceoftheatlastriggersystem