  We present a relativistic constituent-quark model that covers all known
baryons from the nucleon up to $\Omega_{bbb}$. The corresponding invariant mass
operator includes a linear confinement and a hyperfine interaction based on
effective degrees of freedom. The model provides for a unified description of
practically all baryon spectra in good agreement with present phenomenology and
it can tentatively be employed for the relativistic treatment of all kinds of
baryon reactions. Predictions of states still missing in the phenomenological
data base, especially in the lesser explored heavy-flavor sectors of charm and
bottom baryons, should be important especially for future experiments in these
areas.
