  Two-dimensional large-$N$ quantum chromodynamics with scalar quarks is
considered with particular emphasis on its strong coupling regime which has not
been studied so far. Techniques necessary to deal with the infinitely
oscillatory bound state wave functions in the strong coupling regime are
developed. I derive an estimate for the ground state mass and show that (1) the
lightest hadron in the theory is massless and (2) the ground state mass is
continuous across the transition between the weak and the strong coupling.
