Two-dimensional QCD is bosonized to be an integrably deformed Wess-Zum
ino-Witten model under proper limit. Fermions are identified having in
dices of the Grassmann manifold. Conditions for integrability are anal
yzed and their physical meanings are discussed. We also address the na
ture of the exactly solvable part of the theory and find the infinitel
y many conserved quantities. (C) 1997 American Institute of Physics.