Published November 30, 2011 | Version v1
Journal article

First observation of the decay B¯s0→D0K⁎0 and a measurement of the ratio of branching fractions (B(B¯s0→D0K⁎0))/(B(B¯0→D0ρ0))

  • 1. Nikhef National Institute for Subatomic Physics, Amsterdam (Netherlands)
  • 2. Universitat de Barcelona, Barcelona (Spain)
  • 3. Universidad de Santiago de Compostela, Santiago de Compostela (Spain)
  • 4. H.H. Wills Physics Laboratory, University of Bristol, Bristol (United Kingdom)
  • 5. CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille (France)
  • 6. Oliver Lodge Laboratory, University of Liverpool, Liverpool (United Kingdom)
  • 7. Clermont Université, Université Blaise Pascal, CNRS/IN2P3, LPC, Clermont-Ferrand (France)
  • 8. European Organization for Nuclear Research (CERN), Geneva (Switzerland)
  • 9. School of Physics and Astronomy, University of Glasgow, Glasgow (United Kingdom)
  • 10. Petersburg Nuclear Physics Institute (PNPI), Gatchina (Russian Federation)
  • 11. Sezione INFN di Roma La Sapienza, Roma (Italy)
  • 12. Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro (Brazil)
  • 13. Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne (Switzerland)
  • 14. Physik-Institut, Universität Zürich, Zürich (Switzerland)
  • 15. School of Physics and Astronomy, University of Manchester, Manchester (United Kingdom)
  • 16. Max-Planck-Institut für Kernphysik (MPIK), Heidelberg (Germany)
  • 17. Laboratori Nazionali dell'INFN di Frascati, Frascati (Italy)
  • 18. CC-IN2P3, CNRS/IN2P3, Lyon-Villeurbanne (France)

Description

The first observation of the decay B¯s0→D0K⁎0 using pp data collected by the LHCb detector at a centre-of-mass energy of 7 TeV, corresponding to an integrated luminosity of 36 pb−1, is reported. A signal of 34.4±6.8 events is obtained and the absence of signal is rejected with a statistical significance of more than nine standard deviations. The B¯s0→D0K⁎0 branching fraction is measured relative to that of B¯0→D0ρ0: (B(B¯s0→D0K⁎0))/(B(B¯0→D0ρ0)) =1.48±0.34±0.15±0.12, where the first uncertainty is statistical, the second systematic and the third is due to the uncertainty on the ratio of the B0 and Bs0 hadronisation fractions.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.physletb.2011.10.073

Additional details

Identifiers

DOI
10.1016/j.physletb.2011.10.073;
arXiv
arXiv:1110.3676v3;
PII
S0370-2693(11)01339-6;

Publishing Information

Journal Title
Physics Letters. Section B
Journal Volume
706
Journal Issue
1
Journal Page Range
p. 32-39
ISSN
0370-2693
CODEN
PYLBAJ

Optional Information

Copyright
Copyright (c) 2011 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.