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Measurement of the tt¯Z and tt¯W cross sections in proton-proton collisions at s=13 TeV with the ATLAS detector

  • (ATLAS Collaboration)
  • Mohamed I University
  • Aix-Marseille Université
  • University of Oklahoma
  • University of Massachusetts
  • Azerbaijan National Academy of Sciences
  • Université Paris-Saclay
  • Royal Holloway University of London
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  • University of Copenhagen
  • University of Sussex
  • Tel Aviv University
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  • Argonne National Laboratory
  • National Institute for Nuclear Physics
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  • AGH University of Science and Technology
  • Northern Illinois University
  • Ludwig Maximilian University of Munich
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  • Rutherford Appleton Laboratory
  • University of California at Santa Cruz
  • Alexandru Ioan Cuza University of Iaşi
  • Laboratório de Instrumentação e Física Experimental de Partículas
  • University of Granada
  • NOVA University Lisbon
  • Joint Institute for Nuclear Research
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  • Kyoto University
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  • University of Geneva
  • RAS - P.N. Lebedev Physics Institute
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  • Tokyo Institute of Technology
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  • Tomsk State University
  • University of Belgrade
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  • The University of Hong Kong
  • Universidad Antonio Nariño
  • KTH Royal Institute of Technology
  • A. Alikhanian Yerevan Institute of Physics
  • Hiroshima Institute of Technology
  • Okayama University
  • Jagiellonian University in Kraków
  • National Institute for Research and Development of Isotopic and Molecular Technologies
  • University Politehnica of Bucharest
  • IN2P3 - Institut National de Physique Nucléaire et de Physique Des Particules
  • TOBB University of Economics and Technology
  • Kyoto University of Education
  • Transilvania University of Brasov

Research output: Contribution to journalArticlepeer-review

108 Citations (Scopus)

Abstract

A measurement of the associated production of a top-quark pair (tt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb-1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The ttZ and ttW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σttZ=0.95±0.08stat±0.10syst pb and σttW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the ttZ cross section is used to set constraints on effective field theory operators which modify the ttZ vertex.

Original languageEnglish
Article number072009
JournalPhysical Review D
Volume99
Issue number7
DOIs
Publication statusPublished - 29 Apr 2019

ASJC Scopus subject areas

  • Nuclear and High Energy Physics

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