Pm. Rodriguezpascual et al., STEPS TOWARD DETERMINATION OF THE SIZE AND STRUCTURE OF THE BROAD-LINE REGION IN ACTIVE GALACTIC NUCLEI .9. ULTRAVIOLET OBSERVATIONS OF FAIRALL-9, The Astrophysical journal. Supplement series, 110(1), 1997, pp. 9-20
An 8 month monitoring campaign on the Seyfert 1 galaxy Fairall 9 has b
een conducted with the International Ultraviolet Explorer in an attemp
t to obtain reliable estimates of continuum-continuum and continuum-em
ission-line delays for a high-luminosity active galactic nucleus (AGN)
. While the results of this campaign are more ambiguous than those of
previous monitoring campaigns on lower luminosity sources, we find gen
eral agreement with the earlier results: (1) there is no measurable la
g between ultraviolet continuum bands, and (2) the measured emission-l
ine time lags are very short. It is especially notable that the Ly alp
ha + Nv emission-line lag is about 1 order of magnitude smaller than d
etermined from a previous campaign by Clavel, Wamsteker, & Glass (1989
) when Fairall 9 was in a more luminous state. In other well-monitored
sources, specially NGC 5548 and NGC 3783, the highest ionization line
s are found to respond to continuum variations more rapidly than the l
ower ionization lines, which suggests a radially ionization-stratified
broad-line region. In this case, the results are less certain, since
none of the emission-line lags are very well determined. The best-dete
rmined emission line lag is Ly alpha + N v, for which;we find that the
centroid of the continuum-emission-line crosscorrelation function is
tau(cent)approximate to 14-20 days. We measure a lag tau(cent)less tha
n or similar to 4 days for He II lambda 1640; this result is consisten
t with the ionization-stratification pattern seen in lower luminosity
sources, but the relatively large uncertainties in the emission-line l
ags measured here cannot rule out similar lags for Ly alpha + N v and
He II lambda 1640 at a high level of significance. We are unable to de
termine a reliable lag for C IV lambda 1550, but we note that the prof
iles of the variable parts of Ly alpha and C N lambda 1550 are not the
same, which does not support the hypothesis that the strongest variat
ions in these two lines arise in the same region.