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The ATLAS tau trigger

The ATLAS tau trigger consists of three level trigger systems: the first one (L1) is hardware based and uses FPGAs, while the second (L2) and third levels (EF -Event Filter-) are software based and use commodity computers (2 x Intel Harpertown quad-core 2.5 GHz), running scientific linux 5. In this...

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Detalles Bibliográficos
Autor principal: Tsuno, S
Lenguaje:eng
Publicado: 2009
Materias:
Acceso en línea:http://cds.cern.ch/record/1224643
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author Tsuno, S
author_facet Tsuno, S
author_sort Tsuno, S
collection CERN
description The ATLAS tau trigger consists of three level trigger systems: the first one (L1) is hardware based and uses FPGAs, while the second (L2) and third levels (EF -Event Filter-) are software based and use commodity computers (2 x Intel Harpertown quad-core 2.5 GHz), running scientific linux 5. In this contribution, we discuss both the physics characteristics of tau leptons and the technical solutions to quick data access and fast algorithms. We show that L1 selects narrow jets in the calorimeter with an overall rejection against QCD jets of 300, whilst L2 and EF (referred together as High Level Trigger -HLT-) use all the detectors with full granularity and apply a typical rejection of 15 within the stringent timing requirements of the LHC. In the HLT there are two complementary approaches: specialized, fast algorithms are used at L2, while more refined and sophisticated algorithms, imported from the offline, are utilized in the EF.
id cern-1224643
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2009
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spelling cern-12246432019-09-30T06:29:59Zhttp://cds.cern.ch/record/1224643engTsuno, SThe ATLAS tau triggerDetectors and Experimental TechniquesThe ATLAS tau trigger consists of three level trigger systems: the first one (L1) is hardware based and uses FPGAs, while the second (L2) and third levels (EF -Event Filter-) are software based and use commodity computers (2 x Intel Harpertown quad-core 2.5 GHz), running scientific linux 5. In this contribution, we discuss both the physics characteristics of tau leptons and the technical solutions to quick data access and fast algorithms. We show that L1 selects narrow jets in the calorimeter with an overall rejection against QCD jets of 300, whilst L2 and EF (referred together as High Level Trigger -HLT-) use all the detectors with full granularity and apply a typical rejection of 15 within the stringent timing requirements of the LHC. In the HLT there are two complementary approaches: specialized, fast algorithms are used at L2, while more refined and sophisticated algorithms, imported from the offline, are utilized in the EF.ATL-DAQ-PROC-2009-040oai:cds.cern.ch:12246432009-11-25
spellingShingle Detectors and Experimental Techniques
Tsuno, S
The ATLAS tau trigger
title The ATLAS tau trigger
title_full The ATLAS tau trigger
title_fullStr The ATLAS tau trigger
title_full_unstemmed The ATLAS tau trigger
title_short The ATLAS tau trigger
title_sort atlas tau trigger
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1224643
work_keys_str_mv AT tsunos theatlastautrigger
AT tsunos atlastautrigger