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Observation of the Bs0 → D *+ D *− decay

  • 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
  • Sorbonne Université
  • University of Michigan, Ann Arbor
  • Sezione INFN di Milano
  • University of Cincinnati
  • Fakultät Physik
  • University of Dortmund
  • European Organization for Nuclear Research
  • SUPA
  • University of Glasgow
  • University of Barcelona
  • Department of Physics and Astronomy
  • University of Manchester
  • University of Cambridge
  • Instituto de Biofisica da UFRJ
  • Université Paris-Saclay
  • Istituto Nazionale di Fisica Nucleare, Sezione di Firenze
  • Sezione INFN di Ferrara
  • Syracuse University
  • University of Chinese Academy of Sciences
  • University of Heidelberg
  • Aix-Marseille Université
  • Ip Paris
  • Institute of Physics
  • ENAC-IIC-GEL
  • Centro Brasileiro de Pesquisas Fisicas
  • University of Florence

Research output: Contribution to journal › Article › peer-review

3 Citations (Scopus)

Abstract

The first observation of the Bs0 → D ∗+ D ∗− decay and the measurement of its branching ratio relative to the B 0 → D ∗+ D ∗− decay are presented. The data sample used corresponds to an integrated luminosity of 9 fb −1 of proton-proton collisions recorded by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV between 2011 and 2018. The decay is observed with more than 10 standard deviations and the time-integrated ratio of branching fractions is determined to be B(Bs0→D∗+D∗−)B(B0→D∗+D∗−)=0.269±0.032±0.011±0.008, where the first uncertainty is statistical, the second systematic and the third due to the uncertainty of the fragmentation fraction ratio fs /fd. The Bs0 → D *+ D *− branching fraction is calculated to be B(Bs0→D∗+D∗−)=(2.15±0.26±0.09±0.06±0.16)×10−4, where the fourth uncertainty is due to the B 0 → D *+ D *− branching fraction. These results are calculated using the average Bs0 meson lifetime in simulation. Correction factors are reported for scenarios where either a purely heavy or a purely light Bs0 eigenstate is considered. [Figure not available: see fulltext.].

Original languageEnglish
Article number119
JournalJournal of High Energy Physics
Volume2023
Issue number7
DOIs
Publication statusPublished - 1 Jul 2023

Keywords

  • Branching fraction
  • Hadron-Hadron Scattering

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