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    Determinations of form factors for semileptonic D→KD\rightarrow K decays and leptoquark constraints

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    By analyzing all existing measurements for Dβ†’Kβ„“+Ξ½β„“ D\rightarrow K \ell^+ \nu_{\ell} ( β„“=e,Β ΞΌ\ell=e,\ \mu ) decays, we find that the determinations of both the vector form factor f+K(q2)f_+^K(q^2) and scalar form factor f0K(q2)f_0^K(q^2) for semileptonic Dβ†’KD\rightarrow K decays from these measurements are feasible. By taking the parameterization of the one order series expansion of the f+K(q2)f_+^K(q^2) and f0K(q2)f_0^K(q^2), f+K(0)∣Vcs∣f_+^K(0)|V_{cs}| is determined to be 0.7182Β±0.00290.7182\pm0.0029, and the shape parameters of f+K(q2)f_+^K(q^2) and f0K(q2)f_0^K(q^2) are r+1=βˆ’2.16Β±0.007r_{+1}=-2.16\pm0.007 and r01=0.89Β±3.27r_{01}=0.89\pm3.27, respectively. Combining with the average f+K(0)f_+^K(0) of Nf=2+1N_f=2+1 and Nf=2+1+1N_f=2+1+1 lattice calculaltion, the ∣Vcs∣|V_{cs}| is extracted to be 0.964Β±0.004Β±0.0190.964\pm0.004\pm0.019 where the first error is experimental and the second theoretical. Alternatively, the f+K(0)f_+^K(0) is extracted to be 0.7377Β±0.003Β±0.0000.7377\pm0.003\pm0.000 by taking the ∣Vcs∣|V_{cs}| as the value from the global fit with the unitarity constraint of the CKM matrix. Moreover, using the obtained form factors by Nf=2+1+1N_f=2+1+1 lattice QCD, we re-analyze these measurements in the context of new physics. Constraints on scalar leptoquarks are obtained for different final states of semileptonic Dβ†’KD \rightarrow K decays
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