A gluonic mechanism for B --> D eta'
arXiv:hep-ph/0109201 · doi:10.1103/PhysRevD.65.054030
Abstract
We present a calculation of the process B --> D eta' within a heavy-light chiral quark model. We assume that the eta' has a large gluonic component, and its coupling is described via the glue-glue-eta' effective vertex. The main contribution comes from the non-factorizable part of the effective weak Lagrangian at quark level. We find, within our model-dependent assumptions, a branching ratio Br(B --> D eta') = (1.7 -- 3.3) 10^(-4), somewhat below the experimental upper bound 9.4 10^(-4).
17 pages, 4 figures, RevTeX
References in corpus (4)
Cited by in corpus (12)
- Study of color suppressed modes
- A Heavy-Light Chiral Quark Model
- Color suppressed contributions to the decay modes B_{d,s} -> D_{s,d} D_{s,d}, B_{d,s} -> D_{s,d} D^*_{s,d}, and B_{d,s} -> D^*_{s,d} D^*_{s,d}
- Branching Fraction Measurements of the Color-Suppressed Decays B0bar to D(*)0 pi0, D(*)0 eta, D(*)0 omega, and D(*)0 eta_prime and Measurement of the Polarization in the Decay B0bar to D*0 omega
- On the Colour Suppressed Decay Modes B^0 --> D_s^+ D_s^- and B_s^0 --> D^+ D^-
- Power corrections to the space-like transition form factor F_{η^{\prime}g^{*}g^{*}}(Q^2,ω)
- The Isgur-Wise Function within a Modified Heavy-Light Chiral Quark Model
- Non-factorizable contribtion to
- A note on the baryonic B-->Lambdabar p eta' decay
- On the Decay Modes
- On the color suppressed contribution to $\bar{B_{d}^0} \rightarrow \, π^0 π^{0}
- Soft end-point and mass corrections to the eta' g*g* vertex function