2006/12/31 by Shu-Min Zhao, Xiang Liu, Shuang-Jiu Li +1 · 3 citations
Physics and Astronomy · #High-Energy Particle Collisions Research #Meson #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #hep-ex #hep-ph
paper · pdf · doi:10.1140/epjc/s10052-007-0322-7
published as Eur.Phys.J.C51:601-606,2007 · 5 pages, 3 figure, 3 tables, add more discussions, correct typos. The final version to appear at EPJC
arxiv created 2007/05/08 · openalex publication_date 2007/06/05 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Assuming D^*sJ(2317) and DsJ(2460) to be the (0+,1+) chiral partners of regular Ds(1968) and D*s(2112), we calculate the semileptonic decays of Bs to Ds(1968), D^*s(2112), DsJ*(2317), DsJ(2460) in terms of the Constituent Quark Meson (CQM) model. The large branching ratios of the semileptonic decays of Bs to DsJ*(2317) and DsJ(2460) indicate that those two semileptonic decays should be seen in future experiments.