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Evidence for the decays B0→D ̄(*)0φ and updated measurements of the branching fractions of the Bs0→D ̄(*)0φ decays

  • The LHCb collaboration
  • University of Modena and Reggio Emilia
  • Science Park 105
  • University of Warwick
  • Physik-Institut der Universität Zürich
  • University of Liverpool
  • Universidade de Santiago de Compostela
  • University of Bristol
  • Department of Physics and Astronomy
  • Uppsala University
  • Clermont-Auvergne University
  • European Organization for Nuclear Research
  • University of Michigan, Ann Arbor
  • University of Cincinnati
  • LNF-INFN
  • Fakultät Physik
  • University of Dortmund
  • SUPA
  • University of Glasgow
  • University of Barcelona
  • Department of Physics and Astronomy
  • University of Manchester
  • University of Cambridge
  • Sorbonne Université
  • Instituto de Biofisica da UFRJ
  • Université Paris-Saclay
  • State Key Laboratory of Nuclear Physics and Technology
  • Istituto Nazionale di Fisica Nucleare, Sezione di Firenze
  • Sezione INFN di Ferrara
  • Syracuse University
  • University of Chinese Academy of Sciences
  • INFN Roma Tor Vergata
  • University of Rome “Tor Vergata”
  • Aix-Marseille Université
  • Ip Paris
  • Laboratoire de Physique des Particules
  • University of Heidelberg
  • Institute of Physics
  • ENAC-IIC-GEL
  • Centro Brasileiro de Pesquisas Fisicas

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2 Citations (Scopus)

Résumé

Evidence for the decays B0→D¯0ϕ and B0→D¯*0ϕ is reported with a significance of 3.6 σ and 4.3 σ, respectively. The analysis employs pp collision data at centre-of-mass energies s = 7, 8 and 13 TeV collected by the LHCb detector and corresponding to an integrated luminosity of 9 fb−1. The branching fractions are measured to be (Formula presented.) In these results, the first uncertainty is statistical, the second systematic, and the third is related to the branching fraction of the B0→D¯0K+K− decay, used for normalisation. By combining the branching fractions of the decays B0 → D¯∗0ϕ and B0 → D¯∗0ω, the ω-ϕ mixing angle δ is constrained to be tan2δ = (3.6 ± 0.7 ± 0.4) × 10−3, where the first uncertainty is statistical and the second systematic. An updated measurement of the branching fractions of the Bs0 → D¯∗0ϕ decays, which can be used to determine the CKM angle γ, leads to (Formula presented.) (Figure presented.).

langue originaleAnglais
Numéro d'article123
journalJournal of High Energy Physics
Volume2023
Numéro de publication10
Les DOIs
étatPublié - 1 oct. 2023

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