A. Lawrence et al., X-RAY AND OPTICAL CONTINUA OF ACTIVE GALACTIC NUCLEI WITH EXTREME FE-II EMISSION, Monthly Notices of the Royal Astronomical Society, 285(4), 1997, pp. 879-890
We present the results of ROSAT PSPC observations of three active gala
ctic nuclei (AGN) with extremely strong Fe II emission (PHL 1092, IRAS
07598 + 6508 and I Zw 1) and two AGN with very weak Fe II emission (M
rk 10 and 110). The weak Fe II emitters have X-ray spectra typical of
Type 1 AGN (alpha = 1.35 and 1.41, where alpha is the spectral energy
index). Of the strong Fe II emitters, two have steep spectra (PHL 1092
has alpha = 3.5, and I Zw 1 has = 2.0) and the third, IRAS 07598 + 65
08, is barely detected and so is extremely X-ray-quiet (alpha(ox) = 2.
45). During our observations, PHL 1092 varied by a factor of 4, unusua
lly fast for such a high-luminosity object, and requiring an efficienc
y of matter-to-energy conversion of 2 per cent or more. Compiling rece
ntly published data on other strong Fe II emitters, we find that they
are always X-ray-quiet, and usually X-ray-steep. Adding these data to
the complete UVX-selected quasar sample of Laor et al., we find a stat
istical connection of Fe II/H beta with alpha(x) but not a simple rela
tionship: weak Fe II emitters always have flat spectra, but strong Fe
II emitters can be either flat or steep. A much cleaner relationship e
xists between Fe II strength and X-ray loudness, as quantified by alph
a(ix), the spectral index between 1 mu m and 2 ke V. We also confirm t
hat Fe II/H beta anticorrelates with Balmer line velocity width, which
in turn correlates well with both alpha(x) and alpha(ix) in the sense
that AGN with narrow lines are X-ray-quiet. There is also marginal ev
idence that Fe II/H beta correlates with both optical continuum slope
and the curvature of the optical-UV-X-ray continuum: strong Fe II obje
cts tend to have steeper continua and weaker 'blue bumps'. The amount
of extinction required to explain the optical steepening compared to n
ormal quasars [E(B - V) in the range 0.2 to 0.6] suggests absorbing co
lumns in the range (1-3) x 10(21) cm(-2), just about the right amount
to reduce the ROSAT-band X-ray flux by enough to explain the correlati
on with alpha(ix). However, the spectral shapes observed in the ROSAT
band are not consistent with a simple absorption model. Three objects
in our total sample of 19 stand out persistently in all correlations:
Mrk 231, IRAS 07598 + 6508 and Mrk 507. Interestingly, two out of the
three are known to have low-ionization, broad absorption lines in the
UV, and the third (Mrk 507) has no UV spectrum available. Furthermore,
low-ionization, broad absorption lines are at least an order of magni
tude more common in strong Fe II emitters than in quasars in general.
Overall, continuum shape and blueshifted absorption should be added to
the intriguing cluster of properties which all vary loosely together,
and which has been isolated as 'eigenvector 1' by Boroson & Green: Fe
II strength, velocity width, narrow-line strength and line asymmetry.
We suggest that the underlying parameter is the density of an outflow
ing wind.