2005/10/31 by C. Aubin, Christopher Aubin, C. Bernard +1 · 3 citations
Physics and Astronomy · #Chiral perturbation theory #High-Energy Particle Collisions Research #Meson #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum electrodynamics #Quark #hep-lat #hep-ph
paper · pdf · doi:10.1103/physrevd.73.014515
published as Phys.Rev. D73 (2006) 014515 · 48 pages, 6 figures. v3: Some clarifying comments/caveats added; typos fixed. Corresponds to published version
arxiv created 2006/01/25 · openalex publication_date 2006/01/25 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We incorporate heavy-light mesons into staggered chiral perturbation theory (S\ensuremathχPT), working to leading order in 1/mQ, where mQ is the heavy-quark mass. At first nontrivial order in the chiral expansion, staggered taste violations affect the chiral logarithms for heavy-light quantities only through the light-meson propagators in loops. There are also new analytic contributions coming from additional terms in the Lagrangian involving heavy-light and light mesons. Using this heavy-light S\ensuremathχPT, we perform the one-loop calculation of the B (or D) meson leptonic decay constant in the partially quenched and full QCD cases. In our treatment, we assume the validity both of the ``fourth root trick'' to reduce four staggered tastes to one, and of the S\ensuremathχPT prescription to represent this trick by insertions of factors of 1/4 for each sea-quark loop.