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The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3

  • The ATLAS collaboration
  • Aix-Marseille Université
  • University of Oklahoma
  • University of Massachusetts
  • University of Texas at Arlington
  • University of Göttingen
  • United States Department of Energy
  • Mohammed V University in Rabat
  • Max Planck Institute for Physics (Werner Heisenberg Institute)
  • Tel Aviv University
  • Technion-Israel Institute of Technology
  • New York University
  • Pontificia Universidad Católica de Chile
  • National Institute for Nuclear Physics
  • King's College London
  • Abdus Salam International Centre for Theoretical Physics
  • Université Savoie Mont Blanc
  • AGH University of Krakow
  • University of Toronto
  • Brandeis University
  • Northern Illinois University
  • Ludwig Maximilian University of Munich
  • Istanbul University
  • University of Geneva
  • Rutherford Appleton Laboratory
  • University of California at Santa Cruz
  • CERN
  • Institute for High Energy Physics
  • University of Pavia
  • Johannes Gutenberg University Mainz
  • Alexandru Ioan Cuza University of Iaşi
  • University of Granada
  • Azerbaijan National Academy of Sciences
  • McGill University
  • Royal Holloway University of London
  • German Electron Synchrotron
  • University of Rome Tor Vergata
  • University of Hassan II Casablanca
  • Weizmann Institute of Science
  • Lund University
  • A. Alikhanian Yerevan Institute of Physics
  • Columbia University

Research output: Contribution to journalArticlepeer-review

59 Scopus citations

Abstract

The ATLAS detector is installed in its experimental cavern at Point 1 of the CERN Large Hadron Collider. During Run 2 of the LHC, a luminosity of ℒ = 2 × 1034 cm-2 s-1 was routinely achieved at the start of fills, twice the design luminosity. For Run 3, accelerator improvements, notably luminosity levelling, allow sustained running at an instantaneous luminosity of ℒ = 2 × 1034 cm-2 s-1, with an average of up to 60 interactions per bunch crossing. The ATLAS detector has been upgraded to recover Run 1 single-lepton trigger thresholds while operating comfortably under Run 3 sustained pileup conditions. A fourth pixel layer 3.3 cm from the beam axis was added before Run 2 to improve vertex reconstruction and b-tagging performance. New Liquid Argon Calorimeter digital trigger electronics, with corresponding upgrades to the Trigger and Data Acquisition system, take advantage of a factor of 10 finer granularity to improve triggering on electrons, photons, taus, and hadronic signatures through increased pileup rejection. The inner muon endcap wheels were replaced by New Small Wheels with Micromegas and small-strip Thin Gap Chamber detectors, providing both precision tracking and Level-1 Muon trigger functionality. Trigger coverage of the inner barrel muon layer near one endcap region was augmented with modules integrating new thin-gap resistive plate chambers and smaller-diameter drift-tube chambers. Tile Calorimeter scintillation counters were added to improve electron energy resolution and background rejection. Upgrades to Minimum Bias Trigger Scintillators and Forward Detectors improve luminosity monitoring and enable total proton-proton cross section, diffractive physics, and heavy ion measurements. These upgrades are all compatible with operation in the much harsher environment anticipated after the High-Luminosity upgrade of the LHC and are the first steps towards preparing ATLAS for the High-Luminosity upgrade of the LHC. This paper describes the Run 3 configuration of the ATLAS detector.

Original languageEnglish
Article numberP05063
JournalJournal of Instrumentation
Volume19
Issue number5
DOIs
StatePublished - May 1 2024

Keywords

  • Calorimeter methods
  • Large detector systems for particle and astroparticle physics
  • Muon spectrometers
  • Particle tracking detectors

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