Study light scalar meson property from heavy meson decays

preprint2010arXivOpen access

Abstract

In the SU(3) symmetry limit, the ratio R≡B(D+→f0l+ν)+B(D+→σl+ν)B(D+→a00l+ν)R\equiv\frac{{\cal B}(D^+\to f_0l^+ν)+ {\cal B}(D^+\to σl^+ν)}{{\cal B}(D^+\to a_0^0l^+ν)} is equal to 1 if the scalar mesons are qˉq\bar qq states, while it is 3 if these mesons are tentraquark states. This ratio provides a model-independent way to distinguish the descriptions for light scalar mesons . It also applies to the B−→Sl−νˉB^-\to Sl^-\barν and Bˉ0→J/ψ(ηc)S\bar B^0\to J/ψ(η_c) S decays. The SU(3) symmetry breaking effect is found to be under control, which will not spoil our method. The branching fractions of the D+→Sl+νD^+\to S l^+ν, B−→Sl−νˉB^-\to S l^-\barν and Bˉ0→J/ψ(ηc)S\bar B^0\to J/ψ(η_c) S decays roughly have the order 10−410^{-4}, 10−510^{-5} and 10−610^{-6}, respectively. The B factory experiments and ongoing BEPC-II experiments are able to measure these channels and accordingly to provide the detailed information of the scalar meson inner structure.

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