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Performance and Improvements of the ATLAS Jet Trigger System

At the harsh conditions of the LHC, with proton bunches colliding every 50 ns and up to 40 pp interactions per bunch crossing, the ATLAS trigger system has to be flexible to maintaining an unbiased efficiency for a wide variety of physics studies while providing a fast rejection of non-interesting e...

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Autor principal: Conde Muino, P
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:http://cds.cern.ch/record/1453877
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author Conde Muino, P
author_facet Conde Muino, P
author_sort Conde Muino, P
collection CERN
description At the harsh conditions of the LHC, with proton bunches colliding every 50 ns and up to 40 pp interactions per bunch crossing, the ATLAS trigger system has to be flexible to maintaining an unbiased efficiency for a wide variety of physics studies while providing a fast rejection of non-interesting events. Jets are the most commonly produced objects at the LHC, essential for many physics measurements that range from precise QCD studies to searches for New Physics beyond the Standard Model, or even unexpected physics signals. The ATLAS jet trigger is the primary mean for selecting events with high pT jets and its good performance is fundamental to achieve the physics goals of ATLAS. The ATLAS trigger system is divided in three levels, the first one (L1) being hardware based, with a 2 μs latency, and the two following ones (called collectively High Level Triggers or HLT) being softwared based with larger processing times. It was designed to work in a Region of Interest (RoI) based approach, where the second level trigger (L2) is limited to verify the signals provided by the L1 by looking at a region of the detector around them. The last level, EF, has potential full event access. The RoI based strategy was not well-suited for multi-jet events since it lead to pathologies and efficiency losses. A re-design of the jet trigger to overcome this difficulty has happened in between 2011, with the implementation of the full calorimeter unpacking at EF, and 2012 with the introduction of a pseudo-full scan at L2. It is now also possible to run a variety of jet algorithms, both at L2 and at EF, reducing even further possible biases for physics studies. In this presentation, we will describe the challenges of the ATLAS Jet Trigger system, its original limitations and the new developments that were implemented to overcome them. We will also show performance results obtained with 2012 data, including efficiency measuments with respect to the offline reconstructed jets, resolutions and jet energy scale studies.
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spelling cern-14538772019-09-30T06:29:59Zhttp://cds.cern.ch/record/1453877engConde Muino, PPerformance and Improvements of the ATLAS Jet Trigger SystemDetectors and Experimental TechniquesAt the harsh conditions of the LHC, with proton bunches colliding every 50 ns and up to 40 pp interactions per bunch crossing, the ATLAS trigger system has to be flexible to maintaining an unbiased efficiency for a wide variety of physics studies while providing a fast rejection of non-interesting events. Jets are the most commonly produced objects at the LHC, essential for many physics measurements that range from precise QCD studies to searches for New Physics beyond the Standard Model, or even unexpected physics signals. The ATLAS jet trigger is the primary mean for selecting events with high pT jets and its good performance is fundamental to achieve the physics goals of ATLAS. The ATLAS trigger system is divided in three levels, the first one (L1) being hardware based, with a 2 μs latency, and the two following ones (called collectively High Level Triggers or HLT) being softwared based with larger processing times. It was designed to work in a Region of Interest (RoI) based approach, where the second level trigger (L2) is limited to verify the signals provided by the L1 by looking at a region of the detector around them. The last level, EF, has potential full event access. The RoI based strategy was not well-suited for multi-jet events since it lead to pathologies and efficiency losses. A re-design of the jet trigger to overcome this difficulty has happened in between 2011, with the implementation of the full calorimeter unpacking at EF, and 2012 with the introduction of a pseudo-full scan at L2. It is now also possible to run a variety of jet algorithms, both at L2 and at EF, reducing even further possible biases for physics studies. In this presentation, we will describe the challenges of the ATLAS Jet Trigger system, its original limitations and the new developments that were implemented to overcome them. We will also show performance results obtained with 2012 data, including efficiency measuments with respect to the offline reconstructed jets, resolutions and jet energy scale studies.ATL-DAQ-SLIDE-2012-327oai:cds.cern.ch:14538772012-06-04
spellingShingle Detectors and Experimental Techniques
Conde Muino, P
Performance and Improvements of the ATLAS Jet Trigger System
title Performance and Improvements of the ATLAS Jet Trigger System
title_full Performance and Improvements of the ATLAS Jet Trigger System
title_fullStr Performance and Improvements of the ATLAS Jet Trigger System
title_full_unstemmed Performance and Improvements of the ATLAS Jet Trigger System
title_short Performance and Improvements of the ATLAS Jet Trigger System
title_sort performance and improvements of the atlas jet trigger system
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1453877
work_keys_str_mv AT condemuinop performanceandimprovementsoftheatlasjettriggersystem