The interaction via a or exchange is constructed within an extended hidden gauge symmetry approach, where the strange quark is replaced by the charm quark in the flavor space. With this interaction, a bound state slightly lower than the $D \bar{D}^$ threshold is generated dynamically in the isospin zero sector by solving the Bethe-Salpeter equation in the coupled-channel approximation, which might correspond to the particle announced by many collaborations. This formulism is also used to study the interaction, and a $B \bar{B}^$ bound state with isospin zero is generated dynamically, which has no counterpart listed in the review of the Particle Data Group. Furthermore, the one-pion exchange between the meson and the is analyzed precisely, and we do not think the one-pion exchange potential need be considered when the Bethe-Salpeter equation is solved.

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