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We use the QCD sum rules to analize the hadronic decay $D_{sJ}^{+}(2317)\to D_s^+\pi^0D_{sJ}^{+}(2317)$ can be identified as a four-quark state. We use a diquak-antidiquark current and work to the order of in full QCD, without relying on expansion. We find that the partial decay width of the hadronic isospin violating mode is proportional to the isovector quark condensate, . The estimated partial decay width is of the order of 6 keV.

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