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Performance of electron and photon triggers in ATLAS during LHC Run 2

  • ATLAS Collaboration
  • National University of Science and Technology POLITEHNICA Bucharest
  • Dep Física and CEFITEC of Faculdade de Ciências e Tecnologia
  • NOVA University Lisbon
  • Aix-Marseille Université
  • University of Oklahoma
  • University of Massachusetts
  • National Institute for Nuclear Physics
  • University of Pavia
  • University of Göttingen
  • Royal Holloway University of London
  • University of Toronto
  • University of Copenhagen
  • University of Sussex
  • Tel Aviv University
  • Technion-Israel Institute of Technology
  • Argonne National Laboratory
  • Abdus Salam International Centre for Theoretical Physics
  • The University of Tokyo
  • Johannes Gutenberg University Mainz
  • Université Grenoble Alpes
  • AGH University of Krakow
  • Northern Illinois University
  • Ludwig Maximilian University of Munich
  • Bogazici University
  • University of Geneva
  • Rutherford Appleton Laboratory
  • University of California at Santa Cruz
  • IN2P3/CNRS
  • Université Clermont Auvergne
  • Radboud University Nijmegen
  • Alexandru Ioan Cuza University of Iaşi
  • Laboratório de Instrumentação e Física Experimental de Partículas
  • University of Granada
  • Joint Institute for Nuclear Research
  • McGill University
  • Lawrence Berkeley National Laboratory
  • University of Rome Tor Vergata
  • Kyoto University
  • Lund University
  • P.N. Lebedev Physical Institute of the Russian Academy of Sciences
  • University of Bologna
  • University of Victoria BC

Research output: Contribution to journalArticlepeer-review

293 Scopus citations

Abstract

Electron and photon triggers covering transverse energies from 5 GeV to several TeV are essential for the ATLAS experiment to record signals for a wide variety of physics: from Standard Model processes to searches for new phenomena in both proton–proton and heavy-ion collisions. To cope with a fourfold increase of peak LHC luminosity from 2015 to 2018 (Run 2), to 2.1×1034cm-2s-1, and a similar increase in the number of interactions per beam-crossing to about 60, trigger algorithms and selections were optimised to control the rates while retaining a high efficiency for physics analyses. For proton–proton collisions, the single-electron trigger efficiency relative to a single-electron offline selection is at least 75% for an offline electron of 31 GeV, and rises to 96% at 60 GeV; the trigger efficiency of a 25 GeV leg of the primary diphoton trigger relative to a tight offline photon selection is more than 96% for an offline photon of 30 GeV. For heavy-ion collisions, the primary electron and photon trigger efficiencies relative to the corresponding standard offline selections are at least 84% and 95%, respectively, at 5 GeV above the corresponding trigger threshold.

Original languageEnglish
Article number47
JournalEuropean Physical Journal C
Volume80
Issue number1
DOIs
StatePublished - Jan 1 2020

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