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The coupling constants and are calculated in the framework of three-point QCD sum rules. The correlation functions responsible for these coupling constants are evaluated considering contributions of both and mesons as off-shell states, but in the absence of radiative corrections. The results, $g_{D^{\ast}{s}D K^{\ast}(892)}=(4.31\pm1.42) GeV^{-1}g{B^{\ast}_{s}B K^{\ast}(892)}=(3.24\pm1.08) GeV^{-1}$ are obtained for the considered strong coupling constants.

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