Abstract

In our previous study, we calculated the transition from factors of J/ψD(s)()J/\psi\to D^{(*)}_{(s)} using the QCD sum rules. Based on the factorization approximation, the obtained form factors can be applied to evaluate the weak non-leptonic decay rates of J/ψD(s)()+MJ/\psi\to D^{(*)}_{(s)}+M, where MM stands for a light pseudoscalar or vector meson. We predict that the branching ratio for inclusive non-leptonic two-body weak decays of J/ψJ/\psi which are realized via the spectator mechanism, can be as large as 1.3×1081.3 \times 10^{-8}, in particular, the branching ratio of J/ψDs±+ρJ/\psi\to D^{*\pm}_s+\rho^\mp can reach 5.3×1095.3 \times 10^{-9}. Such values will be marginally accessed by the ability of BESIII which will begin running very soon.Comment: 16 pages, revTex4, 1 figur

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    Last time updated on 11/12/2019