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Ds0∗±(2317)D_{s0}^{\ast\pm}(2317) and KDKD scattering from Bs0B^0_s decay

Published 14 Jan 2015 in hep-ph and nucl-th | (1501.03455v2)

Abstract: We study the Bˉ<em>s<sup>0→</sup>Ds<sup>−(DK)<sup>+\bar{B}<em>s<sup>0\to</sup> D_s<sup>-(DK)<sup>+ weak decay, and look at the DKDK invariant mass distribution with the aim of obtaining relevant information on the nature of the D</em>s0<sup>∗+(2317)D</em>{s0}<sup>{\ast+}(2317) resonance. We make a simulation of the experiment using the actual mass of the Ds0<sup>∗+(2317)D_{s0}<sup>{\ast+}(2317) resonance and recent lattice QCD relevant parameters of the KDKD scattering amplitude. We then solve the inverse problem of obtaining the KDKD amplitude from these synthetic data, to which we have added a 5\% or 10\% error. We prove that one can obtain from these "data" the existence of a bound KDKD state, the KDKD scattering length and effective range, and most importantly, the KDKD probability in the wave function of the bound state obtained, which was found to be largely dominant from the lattice QCD results. This means that one can obtain information on the nature of the Ds0<sup>∗+(2317)D_{s0}<sup>{\ast+}(2317) resonance from the implementation of this experiment, in the line of finding the structure of resonances, which is one of the main aims in hadron spectroscopy.

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