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Observation of the decay Bs 0 → ηc φ and evidence for Bs 0 → ηc π + π −

  • The LHCb collaboration
  • European Organization for Nuclear Research
  • University Santiago de Compostela
  • University of Bristol
  • Clermont-Auvergne University
  • University of Cincinnati
  • Fakultät Physik
  • University of Dortmund
  • SUPA
  • University of Glasgow
  • Science Park 105
  • Petersburg Nuclear Physics Institute (PNPI)
  • Imperial College London
  • Instituto de Biofisica da UFRJ
  • INFN
  • Laboratoire de l'Accélérateur Linéaire
  • Center for High Energy Physics
  • Tsinghua University
  • Istituto Nazionale di Fisica Nucleare, Sezione di Firenze
  • Institute of Physics
  • ENAC-IIC-GEL
  • Sezione INFN di Ferrara
  • University of Ferrara
  • University of Maryland, College Park
  • School of Physics and Astronomy
  • University of Manchester
  • University of Heidelberg
  • Aix-Marseille Université
  • Kurchatov Institute
  • Syracuse University
  • Sezione di Roma
  • University of Warwick
  • ICCUB
  • University of Barcelona
  • Pontifícia Universidade Católica do Rio de Janeiro
  • P.N. Lebedev Physical Institute of the Russian Academy of Sciences
  • Institute for Theoretical and Experimental Physics
  • Institute for Nuclear Physics
  • National Centre for Nuclear Research (NCBJ)
  • Université Savoie Mont Blanc

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

8 Citations (Scopus)

Abstract

A study of Bs 0 → ηcϕ and Bs 0 → ηcπ+π− decays is performed using pp collision data corresponding to an integrated luminosity of 3.0 fb−1, collected with the LHCb detector in Run 1 of the LHC. The observation of the decay Bs 0 → ηcϕ is reported, where the ηc meson is reconstructed in the pp¯ , K+K−π+π−, π+π−π+π− and K+K−K+K− decay modes and the ϕ(1020) in the K+K− decay mode. The decay Bs 0 → J/ψϕ is used as a normalisation channel. Evidence is also reported for the decay Bs 0 → ηcπ+π−, where the ηc meson is reconstructed in the pp¯ decay mode, using the decay Bs 0 → J/ψπ+π− as a normalisation channel. The measured branching fractions are(Formula Presented.)where in each case the first uncertainty is statistical, the second systematic and the third uncertainty is due to the limited knowledge of the external branching fractions.[Figure not available: see fulltext.].

Original languageEnglish
Article number21
JournalJournal of High Energy Physics
Volume2017
Issue number7
DOIs
Publication statusPublished - 1 Jul 2017

Keywords

  • B physics
  • Branching fraction
  • Flavor physics
  • Hadron-Hadron scattering (experiments)

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