Analysis of three-body decays B → D ( V → ) P P under the factorization-assisted topological-amplitude approach

• Published in: Physical review. D 2024-09, Vol.110 (5), Article 056001
• Main Authors: Zhou, Si-Hong, Li, Run-Hui, Lü, Xiao-Yao
• Format: Article
• Language: English
• ISSN: 2470-0010; 2470-0029
• DOI: 10.1103/PhysRevD.110.056001

Motivated by the accumulated experimental results on three-body charmed B decays with resonance contributions in , LHCb, and Belle (II), we systematically analyze B ( s ) → D ( s ) ( V → ) P 1 P 2 decays with V representing a vector resonance ( ρ , K * , ω , or ϕ ) and P 1 , 2 as a light pseudoscalar meson (pion or kaon). The intermediate subprocesses B ( s ) → D ( s ) V are calculated with the factorization-assisted topological-amplitude (FAT) approach and the intermediate resonant states V described by the relativistic Breit-Wigner distribution successively decay to P 1 P 2 via strong interaction. Taking all lowest resonance states ( ρ , K * , ω , ϕ ) into account, we calculate the branching fractions of these decay modes as well as the Breit-Wigner-tail effects for B ( s ) → D ( s ) ( ρ , ω → ) K K . Our results agree with the data by , LHCb, and Belle (II). Among the predictions that are still not observed, there are some branching ratios of order 10 − 6 – 10 − 4 which are hopeful to be measured by LHCb and Belle II. Our approach and the perturbative QCD approach (PQCD) adopt the compatible theme to deal with the resonance contributions. What is more, our data for the intermediate two-body charmed B -meson decays in FAT approach are more precise. As a result, our results for branching fractions have smaller uncertainties, especially for color-suppressed emission diagram dominated modes.