One of the greatest mysteries in the field of AGN research is the physical mechanism underlying the radio-quiet/radio-loud dichotomy. Why do some black hole systems choose to launch, accelerate and collimate powerful relativistic jets, whereas other systems do not? The natural environment in which to form an energetic relativistic jet is the relativistic region close to an accreting black hole. A first step in addressing this problem from an observational standpoint is to compare and contrast the central engine structures of radio-quiet and radio-loud AGN. Since they are direct probes of the inner accretion disk, broad iron lines provide a powerful way of facilitating such a comparison.
Radio-loud AGN are rarer, and hence typically fainter, than their
radio-quiet counterparts. Furthermore, many of the best candidates
for study are found in clusters of galaxies and it can be difficult to
observationally distinguish AGN emission from thermal X-rays emitted
by
gas trapped in the cluster's gravitational potential
well. For these reasons, the quality of the observational constraints
are rather poorer than for Seyfert-1 galaxies. There does,
however, appear to be a difference between the iron line properties of
radio-loud nuclei and radio-quiet nuclei. Broad iron lines, and the
associated Compton reflection continua, are generally weak or absent
in the radio-loud counterparts
[257,258,259,260,261,262,263].
This effect might be due to the swamping of a normal `Seyfert-like'
X-ray spectrum by a beamed jet component (similar to the swamping of
optical emission lines in a blazar spectrum). Alternatively, the
inner disk might be in the form of a very hot and optically-thin
radiatively-inefficient accretion flow. Finally, the inner disk might
be radiatively-efficient and optically-thick, but not produce
prominent X-ray reflection features due to a very high ionization
[264]. Again, future observations with XMM-Newton should be able to distinguish these possibilities by
searching for very weak broad components to the iron line and iron
edges with high signal-to-noise.