  In the large $N_c$ limit, one can describe normal heavy baryons $Qqq$ and
heavy pentaquarks $\bar Qqqqq$ as bound states of heavy mesons to chiral
(anti)solitons. In this picture, the strong and electromagnetic decay
parameters of these hadrons can be calculated from those of the constituent
heavy mesons and light baryons, while the weak decay form factors can be
evaluated analytically.
