  We calculate the magnetic moments of heavy baryons with a single heavy quark
in the bound-state approach. In this approach the heavy baryons is considered
as a heavy meson bound in the field of a light baryon. The light baryon field
is represented as a soliton excitation of the light pseudoscalar and vector
meson fields. For these calculations we adopt a model that is both chirally
invariant and consistent with the heavy quark spin symmetry. We gauge the model
action with respect to photon field in order to extract the electromagnetic
current operator and obtain the magnetic moments by computing pertinent matrix
elements of this operator between the bound state wavefunctions. We compare our
predictions for the magnetic moments with results of alternative approaches for
the description of heavy baryon properties.
