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Employing the light-cone sum rule approach in QCD, we relate the -meson distribution amplitude to the form factor at zero momentum transfer. In leading order, the sum rule is converted into a simple expression for the inverse moment of the distribution amplitude . Using as an input the form factor calculated from the light-cone sum rule in terms of pion distribution amplitudes, we obtain an estimate: $\lambda_B =460 \pm 160 B$-meson three-particle distribution amplitudes.

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