  The covariant Faddeev approach which describes baryons as relativistic
three-quark bound states and is based on the Dyson-Schwinger and Bethe-Salpeter
equations of QCD is briefly reviewed. All elements, including especially the
baryons' three-body-wave-functions, the quark propagators and the dressed
quark-photon vertex, are calculated from a well-established approximation for
the quark-gluon interaction. Selected previous results of this approach for the
spectrum and elastic electromagnetic form factors of ground-state baryons and
resonances are reported. The main focus of this talk is a presentation and
discussion of results from a recent investigation of the electromagnetic
transition form factors between ground-state octet and decuplet baryons as well
as the octet-only $\Sigma^0$ to $\Lambda$ transition.
