Two dimensional massless quantum chromodynamics presents many features
which resemble those of the true theory. In particular the spectrum c
onsists of mesons and baryons arranged in flavour multiplets without p
arity doubling. We analyze the implications of chiral symmetry, which
is not spontaneously broken in two dimensions, in the spectrum and in
the quark condensate. We study how parity doubling, an awaited consequ
ence of Coleman's theorem, is avoided due to the dimensionality of spa
ce-time and confinement. We prove that a chiral phase transition is no
t possible in the theory.