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Study of the B 0 → ρ(770)°K * (892) 0 decay with an amplitude analysis of B 0 → (π + π − )(K + π − ) decays

  • The LHCb collaboration
  • Science Park 105
  • Physik-Institut
  • University of Zurich
  • Universidade de Santiago de Compostela
  • University of Bristol
  • University of Michigan, Ann Arbor
  • Clermont-Auvergne University
  • University of Cincinnati
  • LNF-INFN
  • Fakultät Physik
  • University of Dortmund
  • European Organization for Nuclear Research
  • SUPA
  • University of Glasgow
  • University of Barcelona
  • Petersburg Nuclear Physics Institute (PNPI)
  • Imperial College London
  • Instituto de Biofisica da UFRJ
  • INFN
  • Laboratoire de l'Accélérateur Linéaire
  • Istituto Nazionale di Fisica Nucleare, Sezione di Firenze
  • Institute of Physics
  • ENAC-IIC-GEL
  • Sezione INFN di Ferrara
  • University of Maryland, College Park
  • University of Heidelberg
  • Aix Marseille Université
  • Kurchatov Institute
  • Syracuse University
  • Yandex School of Data Analysis
  • Sezione INFN di Cagliari
  • Department of Physics
  • University of Warwick
  • School of Physics and Astronomy
  • University of Manchester
  • Sezione di Genova
  • National University of Science and Technology “MISIS”
  • National Centre for Nuclear Research (NCBJ)

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Résumé

An amplitude analysis of B 0 → (π + π − )(K + π − ) decays is performed in the two-body invariant mass regions 300 < m(π + π − ) < 1100 MeV/c 2 , accounting for the ρ 0 , ω, f 0 (500), f 0 (980) and f 0 (1370) resonances, and 750 < m(K + π − ) < 1200 MeV/c 2 , which is dominated by the K * (892) 0 meson. The analysis uses 3 fb −1 of proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. The CP averages and asymmetries are measured for the magnitudes and phase differences of the con- tributing amplitudes. The CP-averaged longitudinal polarisation fractions of the vector-vector modes are found to be f˜ρK*0 = 0.164 ± 0.015 ± 0.022 and f˜ωK*0 = 0.68 ± 0.17 ± 0.16, and their CP asymmetries, AρK*0 = −0.62 ± 0.09 ± 0.09 and AωK*0 = −0.13 ± 0.27 ± 0.13, where the first uncertainty is statistical and the second systematic.[Figure not available: see fulltext.].

langue originaleAnglais
Numéro d'article26
journalJournal of High Energy Physics
Volume2019
Numéro de publication5
Les DOIs
étatPublié - 1 mai 2019

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