Massless QCD(2) is dominated by classical configurations in the large-N-f l
imit. We use this observation to study the theory by finding solutions to e
quations of motion, which are the non-abelian generalization of the Schwing
er equation. We find that the spectrum consists of massive mesons with M-2
= e(2)N(f)/2 pi, which correspond to abelian solutions. We generalize previ
ously discovered non-abelian solutions and discuss their interpretation. We
prove a no-go theorem ruling out the existence of soliton solutions. Thus
the semi-classical approximation shows no baryons in the case of massless q
uarks, a result derived before in the strong-coupling limit only. (C) 1999
Elsevier Science B.V.