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The form factors of transition process $\mathcal{B}_{Q_{1}Q_{2}}(\frac{1}{2}^{+})\rightarrow\mathcal{B}_{Q_{1}}^{*}(\frac{3}{2}^{+})$ and their applications to semileptonic decays
In the framework of QCD sum rules, we obtain the form factors of the weak transition process $\mathcal{B}_{Q_{1}Q_{2}}(\frac{1}{2}^{+})\rightarrow\mathcal{B}_{Q_{1}}^{*}(\frac{3}{2}^{+})$. In this analysis, we eliminate the interferences of the low spin states and negative parity states to final res
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