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B- and D-meson decay constants from three-flavor lattice QCD

A. Bazavov1, C. Bernard2, C. M. Bouchard3,4,5, C. DeTar6, M. Di Pierro7, A. X. El-Khadra3, R. T. Evans3, E. D. Freeland3,8, E. Gámiz4,9 et al. (Fermilab Lattice and MILC Collaborations)

E. Gámiz4,9, Steven Gottlieb10, U. M. Heller11, J. E. Hetrick12, R. Jain3, A. S. Kronfeld4, J. Laiho13, L. Levkova6, P. B. Mackenzie4, E. T. Neil4, M. B. Oktay6, J. N. Simone4, R. Sugar14, D. Toussaint15, and R. S. Van de Water1,* (Fermilab Lattice and MILC Collaborations)

  • 1Physics Department, Brookhaven National Laboratory, Upton, New York, USA
  • 2Department of Physics, Washington University, St. Louis, Missouri, USA
  • 3Physics Department, University of Illinois, Urbana, Illinois, USA
  • 4Fermi National Accelerator Laboratory, Batavia, Illinois, USA
  • 5Department of Physics, The Ohio State University, Columbus, Ohio, USA
  • 6Physics Department, University of Utah, Salt Lake City, Utah, USA
  • 7School of Computing, DePaul University, Chicago, Illinois, USA
  • 8Department of Physics, Benedictine University, Lisle, Illinois, 60532, USA
  • 9CAFPE and Departamento de Física Teórica y del Cosmos, Universidad de Granada, Granada, Spain
  • 10Department of Physics, Indiana University, Bloomington, Indiana, USA
  • 11American Physical Society, Ridge, New York, USA
  • 12Physics Department, University of the Pacific, Stockton, California, USA
  • 13SUPA, School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
  • 14Department of Physics, University of California, Santa Barbara, California, USA
  • 15Department of Physics, University of Arizona, Tucson, Arizona, USA

  • *ruthv@bnl.gov

Phys. Rev. D 85, 114506 – Published 8 June, 2012

DOI: https://doi.org/10.1103/PhysRevD.85.114506

Abstract

We calculate the leptonic decay constants of B(s) and D(s) mesons in lattice QCD using staggered light quarks and Fermilab bottom and charm quarks. We compute the heavy-light-meson correlation functions on the MILC Asqtad-improved staggered gauge configurations, which include the effects of three light dynamical sea quarks. We simulate with several values of the light valence- and sea-quark masses (down to ms/10) and at three lattice spacings (a0.15, 0.12, and 0.09 fm) and extrapolate to the physical up and down quark masses and the continuum using expressions derived in heavy-light-meson staggered chiral perturbation theory. We renormalize the heavy-light axial current using a mostly nonperturbative method such that only a small correction to unity must be computed in lattice perturbation theory, and higher-order terms are expected to be small. We use the two finer lattice spacings for our central analysis, and we use the third to help estimate discretization errors. We obtain fB+=196.9(9.1)MeV, fBs=242.0(10.0)MeV, fD+=218.9(11.3)MeV, fDs=260.1(10.8)MeV, and the SU(3) flavor-breaking ratios fBs/fB=1.229(26) and fDs/fD=1.188(25), where the numbers in parentheses are the total statistical and systematic uncertainties added in quadrature.

Article Text

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