We consider a ``one current'' state, which is obtained by the application of
a color current on the ``adjoint'' vacuum. This is done in QCD2, 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 M2=2P+P− on these states and find that in
general they are not eigenstates of M2 apart from the large Nf limit.
Problems with infra-red regularizations are pointed out. We discuss the
fermionic structure of these states.Comment: 18 pages, no figures. v2: minor corrections. v3: added some
clarifications and remarks, mainly on the contribution of zero modes. Typos
corrected, references added. To appear in Nuclear Physics