  We study Quantum Chromodynamics in the chiral large $N_c$ limit which
contains a left-handed Weyl fermion in the fundamental representation, a
left-handed Weyl fermion in the two index antisymmetric representation and
$(N_c-3)$ left-handed Weyl fermions in the antifundamental representation of
the $SU(N_c)$ gauge group. We construct gauge singlet composite operators and
study their masses and correlation functions at large $N_c$.
  It is shown that all hadron masses scale as $\sim N_c^0 n_q$ where $n_q$ is
the number of constituent quarks in the hadron. In addition by simple gluon
exchange considerations it is seen that scattering amplitudes between hadrons
have the same $N_c$ scaling as the mass of the lightest hadron involved. This
is the case provided the hadrons in the scattering amplitude share a
sufficiently large number of constituent quarks.
  The chiral large $N_c$ extension also allows for other non-trivial processes.
For instance we consider two different baryonium states that are unique to this
extension and that decay via emissions of two- and three-quark hadrons. Also
other non-trivial scattering processes are considered. Finally, we study
composites made of a mix of left- and right-handed fields. We categorize
multiple groups of hadrons within the full spectrum according to their flavor
structure. Within these groups all $n$-point functions scale the same.
