The cross section for ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\psi}(2S)$ between threshold and $\sqrt{s}=5.5\text{ }\text{ }\mathrm{GeV}$ is measured using $673\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ of data on and off the $\ensuremath{\Upsilon}(4S)$ resonance collected with the Belle detector at KEKB. Two resonant structures are observed in the ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\psi}(2S)$ invariant-mass distribution, one at $4361\ifmmode\pm\else\textpm\fi{}9\ifmmode\pm\else\textpm\fi{}9\text{ }\text{ }\mathrm{MeV}/{c}^{2}$ with a width of $74\ifmmode\pm\else\textpm\fi{}15\ifmmode\pm\else\textpm\fi{}10\text{ }\text{ }\mathrm{MeV}/{c}^{2}$, and another at $4664\ifmmode\pm\else\textpm\fi{}11\ifmmode\pm\else\textpm\fi{}5\text{ }\text{ }\mathrm{MeV}/{c}^{2}$ with a width of $48\ifmmode\pm\else\textpm\fi{}15\ifmmode\pm\else\textpm\fi{}3\text{ }\text{ }\mathrm{MeV}/{c}^{2}$, if the mass spectrum is parametrized with the coherent sum of two Breit-Wigner functions. These values do not match those of any of the known charmonium states.
Observation of Two Resonant Structures ine+e−→π+π−ψ(2S)via Initial-State Radiation at Belle | Litlas
