Abstract
We find that the evolution equation for the three-particle quark-gluon -meson light-cone distribution amplitude (DA) of subleading twist is completely integrable in the large limit and can be solved exactly. The lowest anomalous dimension is separated from the remaining, continuous spectrum by a finite gap. The corresponding eigenfunction coincides with the contribution of quark-gluon states to the two-particle DA so that the evolution equation for the latter is the same as for the leading-twist DA up to a constant shift in the anomalous dimension. Thus, “genuine” three-particle states that belong to the continuous spectrum effectively decouple from to the leading-order accuracy. In turn, the scale dependence of the full three-particle DA turns out to be nontrivial so that the contribution with the lowest anomalous dimension does not become leading at any scale. The results are illustrated on a simple model that can be used in studies of corrections to heavy-meson decays in the framework of QCD factorization or light-cone sum rules.
- Received 14 July 2015
DOI:https://doi.org/10.1103/PhysRevD.92.074044
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