  We consider a ``one current'' state, which is obtained by the application of
a color current on the ``adjoint'' vacuum. This is done in $QCD_2$, with the
underlying quarks in the fundamental representation. The quarks are taken to be
massless, in which case the theory on the light-front can be ``currentized'',
namely, formulated in terms of currents only. The adjoint vacuum is shown to be
the application of a current derivative, at zero momentum, on the singlet
vacuum. We apply the operator $M^2=2P^+P^-$ on these states and find that in
general they are not eigenstates of $M^2$ apart from the large $N_f$ limit.
Problems with infra-red regularizations are pointed out. We discuss the
fermionic structure of these states.
