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In this letter we suggest that the obvious discrepancy between theoreticalprediction on the $\mathrm{non}-D\bar D$ decays of $\psi(3770)$ and data is tobe alleviated by taking final state interaction (FSI) into account. By assumingthat $\psi(3770)$ overwhelmingly dissociates into $D\bar D$, then the finalstate interaction induces a secondary process, we calculate the branchingratios of $\psi(3770)\to D\bar D\to J/\psi\eta, \rho\pi, \omega\eta, K^*K$. Ourresults show that the branching ratio of $\psi(3770)\to \mathrm{non}-D\bar{D}$can reach up to $\mathcal{B}_{\mathrm{non}-D\bar{D}}^{FSI}=(0.2\sim1.1)%$ whiletypical parameters $I=0.4$ GeV$^{-2}$ and $\alpha=0.8\sim 1.3$ are adopted.This indicates that the FSI is obviously non-negligible.

The puzzle of excessive non-$D\bar D$ component of the inclusive $\psi(3770)$ decay and the long-distant contribution