The role of charged exotic states in $e^{+}{e}^{-}\to \psi (2S){\pi }^{+}{\pi }^{-}$

Abstract

In this work, we use the dispersion theory to provide a physical description of recent BESIII data on the reaction $e^{+}{e}^{-}\to \psi (2S){\pi }^{+}{\pi }^{-}$. Taking into account explicitly the effects of charged exotic intermediate states in the $t$- and $u$-channels as well as the two-pion final state interaction, we describe the invariant mass distribution for four different $e^{+}{e}^{-}$ center-of-mass energies. The effects of the $\pi \pi$ rescattering are accounted for within a model-independent single channel approach which is found to explain the $\pi \pi$-invariant mass distributions at all $e^{+}{e}^{-}$ center-of-mass energies. For $q=4.226$ GeV and $q=4.258$ GeV the already established charged exotic state $Z_c(3900)$ is considered as the intermediate state, whereas for $q=4.358$ GeV the rescattering of pions dominates the fits. For the highest energy, $q=4.416$ GeV, a heavier charged exotic state with mass $m_{Z_c}=4.016(4)$ GeV and width ${\Gamma }_{Z_c}=52(10)$ MeV is essential to describe the experimental data. Although the mass of this state is consistent with the established $Z_c(4020)$, its width is significantly larger.