![]() | Annu. Rev. Astron. Astrophys. 2000. 38: 761-814 Copyright © 2000 by Annual Reviews. All rights reserved |
3.4.3. Hidden AGNs: The Role of Dust Obscuration in ULIRGs
The active regions of ULIRGs are veiled by thick
layers of dust. Fine structure and recombination line ratios imply
equivalent
"screen" dust extinctions in ULIRGs (and LIRGs) between AV ~ 5 and 50
(Genzel et al 1998).
ISOPHOT-S and ground-based data confirm this evidence for high dust
extinction
(Lutz et al 1998a,
Dudley & Wynn-Williams
1997,
Dudley 1999).
The most extreme case is Arp 220, where the ISO SWS data indicate
AV(screen) ~ 50 (A25µm
~ 1), or an equivalent mixed model extinction of 500 to 1000 mag in the
V-band 8
(Sturm et al 1996).
Smith et al (1989),
Soifer et al (1999)
found similar values from the depth of the silicate feature and from mid-IR
imaging. These large extinctions combined with a mixed extinction model
solve the puzzle that starburst models based on near-IR/optical data
cannot account for the far-IR luminosities (AV
10;
Armus et al 1995,
Goldader et al 1997a,
b).
If the emission line data are instead corrected for the (much larger)
ISO-derived extinctions, the derived LIR / LLyc
ratios are in reasonable agreement with starburst models
(Section 3.4.4).
Submm/mm CO and dust observations imply yet larger column densities than
the mid-IR data (
1024 cm-2, or AV
500;
Rigopoulou et al
1996b,
Solomon et al 1997,
Scoville et al 1997,
Downes and Solomon 1998).
Is it possible, therefore, that most ULIRGs contain powerful central AGNs
that are missed by the mid-IR data? Hard X-rays penetrate to column
densities
1024
cm-2. ASCA has observed a small sample of ULIRGs in the 2-10
keV band. About a dozen sources are common between ISO and ASCA
(Brandt et al 1997,
Kii et al 1997,
Nakagawa et al 2000,
Misaki et al 1999).
In Mrk 273, 05189-2524, NGC 6240, and 230605+0505, ASCA finds evidence
for a hard X-ray source with < LX / LIR >
10-3. BeppoSAX
observations show that the AGN in NGC 6240 is attenuated by a Compton
thick (NH ~ 2 × 1024 cm-2) absorber
(Vignati et al 1999).
After correction for this absorption, and depending on its filling factor,
the ratio of intrinsic AGN X-ray to IR luminosity is 2 to 6 ×
10-2. In Mrk 231, a hard X-ray source is seen but is weak
(< LX / LIR > ~ 10-3.5).
ISO finds evidence for significant AGN activity in all of these sources as
well. In sources classified by ISO as starburst dominated (Arp 220,
UGC 5101,
17208-0014, 20551-4250, 23128-5919), ASCA also finds no hard X-ray source.
The limit to the hard X-ray emission in Arp 220 corresponds to
10-4 of the
infrared luminosity. For comparison, in Seyfert 1 and Seyfert 2 galaxies
< LX / LIR > is 10-1 and
10-2, respectively
(Boller et al 1997,
Awaki et al 1991).
For radio-quiet QSOs, the sample averaged SEDs of
Sanders et al (1989),
Elvis et al (1994),
giving LX / LIR = 0.2 and LX /
Lbol ~
0.05. Although the statistics are still relatively poor at this point, the
hard X-ray data do not present evidence for powerful AGNs that are
completely missed by the mid-IR observations. Still, there are
exceptions to this reasonable
agreement between IR and X-ray data. The nearby galaxy NGC 4945 fulfills
all criteria of a pure starburst at optical to mid-IR wavelengths
(Moorwood et al 1996b;
in Figure 5a,
NGC 4945 is the starburst to the bottom right of Arp 220 and top left
of M82). There is no evidence for a narrow line region or any other AGN
indicator
at these wavelengths. The [NeIII] / [NeII] line ratio is small and indicates
that the starburst is aging (Spoon, private communication). Yet ASCA and
BeppoSAX data show that at its center lurks a powerful AGN, attenuated by
a Compton thick foreground absorber
(Iwasawa et al 1993).
As in NGC 6240, both the AGN (from the X-ray data) as well as the starburst
(from the optical to IR data) can account for the entire bolometric
luminosity
of NGC 4945. Although NGC 4945 is much less luminous than a ULIRG, the case
is puzzling and requires further study.
If mid-infrared continuum and UIB features suffer different obscurations, as in Seyfert 2 galaxies (Section 3.3.1; Clavel et al 1998), the UIB strength criterion5 loses its meaning. Instead it is necessary to directly compare the ratio of UIB luminosity to total far-IR (60 + 100 µm) luminosity, even if this ratio depends on mid-infrared extinction. The UIB/FIR ratio in ULIRGs (Figure 10) is on average half of that in starbursts (and Seyferts). Following the discussion in Section 3.3.2, this suggests that at least half of the luminosity in the average ULIRG comes from star formation if the same UIB/FIR ratio holds as in other galaxies. Correction for extinction increases this fraction. If the average mid-IR extinction is AV(screen) ~ 15 and A7.7 / AV ~ 0.04, the UIB/FIR ratio is fully consistent with that in starburst galaxies.
Hence, despite the large extinctions present in most
ULIRGs, optical/near-IR emission line diagnostics remain useful qualitative
diagnostic tools in the majority of sources. For these objects, mid-IR
emission lines/UIB features can be used as quantitative tools for
estimating the relative
contributions of AGN and star formation. The reason is that optical and IR
emission line diagnostics only rely on penetrating through dust in the disk
to the narrow line region, and not through a high column density
circumnuclear torus to the central AGN itself. The large-scale
( 100 pc) obscuring material
is likely very patchy and arranged in thin (and self-gravitating) disks
(as in Arp 220;
Scoville et al 1998).
Radiation and outflows from AGNs punch rapidly through the clumpy
obscuring screen, at least in certain directions.
8
In the screen extinction model the dust is in a homogeneous screen in
front of the source and the attenuation at
is given by
exp(-
d(
)) where
d(
) is the optical
depth of the dust screen at
. An
alternative, and probably more plausible scenario is that obscuring dust
clouds and emitting HII regions
are completely spatially mixed throughout an extended region. In that
case the attenuation at
is
d(
)
/ (1 - exp(-
d(
))) which changes much more
slowly with wavelength.
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