Abstract
We show that the final-state interaction perfectly explains the recent experimental data of BESIII Collaboration on the near-threshold invariant-mass spectrum of in the process . The position of peak in invariant-mass spectrum is above the threshold though the interaction of and is due to an attractive potential. This potential has a simple form and depends only on two parameters. We show that the invariant-mass spectrum is consistent with the quantum numbers and of pair but contradicts to .
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