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Precise measurement of the tt¯ production cross-section and lepton differential distributions in eμ dilepton events from s=13TeVpp collisions with the ATLAS detector

  • ATLAS Collaboration
  • Department of Physics
  • Stellenbosch University
  • School of Agriculture and Science
  • University of KwaZulu-Natal
  • Department of Physics
  • University of South Africa
  • Department of Mechanical and Aeronautical Engineering
  • University of Pretoria
  • University of Zululand
  • Cadi Ayyad University
  • Departamento de Física Teórica y del Cosmos
  • University of Granada
  • CERN
  • Demokritos National Centre for Scientific Research
  • University of Sheffield
  • Harvard University
  • University of Bologna
  • National Institute for Nuclear Physics
  • University of Belgrade
  • University of Siegen
  • Heidelberg University 
  • Indiana University Bloomington
  • CAS - Institute of High Energy Physics
  • University of Science and Technology of China
  • Shanghai Jiao Tong University
  • University of Michigan, Ann Arbor
  • University of Arizona
  • Nanjing University
  • Tsinghua University
  • University of Illinois at Urbana-Champaign
  • SLAC National Accelerator Laboratory
  • Carleton University
  • Shandong University
  • University of Washington
  • Université Paris-Saclay
  • Lawrence Berkeley National Laboratory
  • University College London
  • The University of Tokyo
  • Université Toulouse III - Paul Sabatier
  • University of Chinese Academy of Sciences
  • Argonne National Laboratory

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

The inclusive top quark pair (tt¯) cross-section σtt¯ has been measured in proton–proton collisions at s=13TeV, using 140fb-1 of data collected by the ATLAS experiment at the Large Hadron Collider. Using events with an opposite-charge eμ pair and b-tagged jets, the cross-section is measured to be: (Formula presented.) where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the proton beam energy, giving a total uncertainty of 1.3%. The result is used to determine the top quark pole mass via the dependence of the predicted cross-section on mtpole, giving mtpole=172.8-1.7+1.5 GeV. The same event sample is used to measure absolute and normalised differential cross-sections for the tt¯→eμνν¯bb¯ process as a function of single-lepton and dilepton kinematic variables. Complementary measurements of eμbb¯ production, treating both tt¯ and Wt events as signal, are also provided. Both sets of differential cross-sections are compared to the predictions of various Monte Carlo event generators, demonstrating that the state-of-the-art generators Powheg MiNNLO and Powhegbb4l describe the data better than Powheghvq.

Original languageEnglish
Article number470
JournalEuropean Physical Journal C
Volume86
Issue number5
DOIs
StatePublished - May 2026

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