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The decay ${\ensuremath{\eta}}_{c}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\eta}$ is searched for through the radiative transition $\ensuremath{\psi}(3686)\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\eta}}_{c}(2S)$ using 448 million $\ensuremath{\psi}(3686)$ events accumulated at the BESIII detector. The first evidence of ${\ensuremath{\eta}}_{c}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\eta}$ is found with a statistical significance of $3.5\ensuremath{\sigma}$. The product of the branching fractions of $\ensuremath{\psi}(3686)\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\eta}}_{c}(2S)$ and ${\ensuremath{\eta}}_{c}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\eta}$ is measured to be $\mathrm{Br}(\ensuremath{\psi}(3686)\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\eta}}_{c}(2S))\ifmmode\times\else\texttimes\fi{}\mathrm{Br}({\ensuremath{\eta}}_{c}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\eta})=\phantom{\rule{0ex}{0ex}}(2.97\ifmmode\pm\else\textpm\fi{}0.81\ifmmode\pm\else\textpm\fi{}0.26)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$, where …