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Measurement of the H→ γγ and H→ ZZ→ 4 ℓ cross-sections in pp collisions at √s=13.6 TeV with the ATLAS detector

  • ATLAS Collaboration
  • Faculty of Physics
  • University of Bucharest
  • iThemba Labs
  • Department of Physics
  • University of South Africa
  • University of Zululand
  • Cadi Ayyad University
  • New York University Abu Dhabi
  • Departamento de Física Teórica y del Cosmos
  • University of Granada
  • CERN
  • Aix-Marseille Université
  • University of Oklahoma
  • University of Göttingen
  • TU Dortmund University
  • United States Department of Energy
  • Mohammed V University in Rabat
  • Tel Aviv University
  • Technion-Israel Institute of Technology
  • New York University
  • National Institute for Nuclear Physics
  • Abdus Salam International Centre for Theoretical Physics
  • King's College London
  • Université Savoie Mont Blanc
  • AGH University of Krakow
  • University of Toronto
  • Brandeis University
  • University of Manchester
  • Northern Illinois University
  • Istanbul University
  • Rutherford Appleton Laboratory
  • University of California at Santa Cruz
  • Institute for High Energy Physics
  • University of Pavia
  • Johannes Gutenberg University Mainz
  • Alexandru Ioan Cuza University of Iaşi
  • Azerbaijan National Academy of Sciences
  • McGill University
  • Royal Holloway University of London
  • University of Science and Technology of China
  • University of Rome Tor Vergata
  • University of Valencia
  • University of Hassan II Casablanca
  • Weizmann Institute of Science
  • Lund University
  • Waseda University
  • University of Bonn
  • Columbia University
  • University of Victoria BC

Research output: Contribution to journalArticlepeer-review

11 Scopus citations

Abstract

The inclusive Higgs boson production cross-section is measured in the di-photon and the ZZ→ 4 ℓ decay channels using 31.4 and 29.0 fb - 1 of pp collision data respectively, collected with the ATLAS detector at a centre-of-mass energy of s=13.6 TeV . To reduce the model dependence, the measurement in each channel is restricted to a particle-level phase space that closely matches the channel’s detector-level kinematic selection, and it is corrected for detector effects. These measured fiducial cross-sections are σfid , γ γ= 76-13+14 fb, and σfid , 4 = 2.80±0.74 fb, in agreement with the corresponding Standard Model predictions of 67.6 ± 3.7 fb and 3.67 ± 0.19 fb. Assuming Standard Model acceptances and branching fractions for the two channels, the fiducial measurements are extrapolated to the full phase space yielding total cross-sections of σ(pp→H)=67-11+12 pb and 46 ± 12 pb at 13.6 TeV from the di-photon and ZZ→ 4 ℓ measurements respectively. The two measurements are combined into a total cross-section measurement of σ(pp→ H) = 58.2 ± 8.7 pb, to be compared with the Standard Model prediction of σ(pp→ H) SM= 59.9 ± 2.6 pb.

Original languageEnglish
Article number78
JournalEuropean Physical Journal C
Volume84
Issue number1
DOIs
StatePublished - Jan 2024

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