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Simultaneous description of the e+eJ/ψππ(KKˉ)e^+e^- \to J/ ψ\, ππ\, (K \bar{K}) processes

Published 28 Apr 2020 in hep-ph | (2004.13499v2)

Abstract: In this work, we provide a simultaneous and accurate description of the π<sup>+π<sup>\pi<sup>+\pi<sup>- and π<sup>±</sup>J/ψ\pi<sup>{\pm}</sup> J/\psi invariant mass distributions of the recent BESIII data on e<sup>+</sup>e<sup></sup>J/ψ  π<sup>+</sup>π<sup>e<sup>+</sup> e<sup>-</sup> \to J/\psi \; \pi<sup>+</sup> \pi<sup>- together with the e<sup>+</sup>e<sup></sup>J/ψ  K<sup>+K<sup>e<sup>+</sup> e<sup>-</sup> \to J/\psi \; K<sup>+K<sup>- cross sections at e<sup>+e<sup>e<sup>+e<sup>- center-of-mass energies q=4.23q=4.23 GeV and q=4.26q=4.26 GeV. The rescattering effects between pions in the S and D-waves are taken into account through the Muskhelishvili-Omn`es formalism. Since the physical region of the ππ\pi\pi invariant mass extends above 1 GeV, the important KKˉK\bar{K} intermediate state in the S-wave is implemented through coupled-channel unitarity. For the left-hand cuts, we account for the well established charged exotic state Zc(3900)Z_c(3900) in tt- and uu-channels, while the other contributions are absorbed in the subtraction constants. For the e<sup>+</sup>e<sup></sup>J/ψKKˉe<sup>+</sup> e<sup>-</sup> \to J/\psi\, K \bar{K} we provide the prediction of the two-kaon invariant mass distribution. The constructed amplitudes serve as an essential framework to interpret the present and forthcoming measurements by the BESIII and Belle II Collaborations.

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