We examine the statistical mechanics of a one-dimensional gas of both
adjoint and fundamental representation quarks which interact with each
other through (1 + 1)-dimensional U(N) gauge fields. Using large-N ex
pansion we show that, when the density of fundamental quarks is small,
there is a first-order phase transition al a critical temperature and
adjoint quark density which can be interpreted as deconfinement. When
the fundamental quark density is comparable to the adjoint quark dens
ity, the phase transition becomes a third order one. We formulate a wa
y to distinguish the phases by considering the expectation values of h
igh winding number Polyakov loop operators. (C) 1997 Academic Press.