We formulate a consistent 1/N-c(2) expansion of the QCD evolution equations
for the twist-three quark distributions g(2)(x,Q(2)), h(L)(x,Q(2)) and e(x
,Q(2)) based on the interpretation of the evolution as a three-particle qua
ntum-mechanical problem with hermitian Hamiltonian. Each distribution ampli
tude can be decomposed in contributions of partonic components with DGLAP-t
ype scale dependence. We calculate the 1/N-c(2) corrections to the evolutio
n of the dominant component with the lowest anomalous dimension - the only
one that survives in the large-N-c limit - and observe a good agreement wit
h the exact numerical results for N-c = 3. The 1/N-c(2) admixture of operat
ors with higher anomalous dimensions is shown to be concentrated at a few l
owest partonic components and in general is rather weak. (C) 2000 Elsevier
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