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It is argued that the ratio of the yield of pairs of charged and neutral mesons in the processes $\Upsilon(5S) \to \pi^0 + (B \bar B^* + c.c.)\Upsilon(5S) \to \pi^0 + B^* \bar B^*$ is very sensitive near the corresponding heavy meson threshold to the strong interaction between the mesons in the channel due to significant isospin breaking by the Coulomb force. This channel, not readily accessible by other means, may contain near-threshold molecular meson-antimeson resonances — isoscalar analogs of the isovector states and .

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