A&A 373, 459-472 (2001)
DOI: 10.1051/0004-6361:20010635
Global molecular gas properties of Seyfert galaxies![[*]](/icons/foot_motif.gif)
II. Analysis of the results
S. J. Curran1,2,3 - A. G. Polatidis1 - S. Aalto1 - R. S. Booth1
1 - Onsala Space Observatory,
Chalmers University of Technology,
439 92 Onsala,
Sweden
2 - European Southern Observatory,
Casilla 19001, Santiago 19,
Chile
3 - School of Physics,
University of New South Wales,
Sydney NSW 2052,
Australia
Received 3 April 2001 / Accepted 24 April 2001
Abstract
We use the data published in Paper I and Curran et al. (2000) to determine the global
molecular gas luminosities and distributions in a sample of 22 Seyfert
galaxies. From this we find definite differences in the CO to HCN
luminosity ratios between the near-by and distant galaxies of the
sample. This is perhaps due to a selection effect where we only observe the
brightest of the distant sources. With regard to distributions, we
find in the near-by (mapped) sample that the CO is usually much wider
distributed than the central telescope beam and that the HCN is
considerably more extended beyond the
1 kpc often cited in the
literature. In fact this molecule has been detected as far as
5 kpc from the centre of NGC 1365. We may also have detected
a bar in HCN in NGC 5033. Also, using the data to complement the
results of Curran (2000a), we find
i.e. no difference in the molecular gas luminosities between the two
main Seyfert classes. In fact we consider it more meaningful to
discuss the differences between the near-by and distant sample
(irrespective of Seyfert type), although both of these samples may
show evidence that much of the far infrared luminosity could arise
from an active galactic nucleus as opposed to being predominantly due
to vigorous star formation. We do believe, however, that improved
statistics would be of little value in distinguishing between these
two scenarios and that future high resolution observations are the key
to resolving this issue.
Key words: galaxies: Seyfert - galaxies: starburst - galaxies: abundances - galaxies: ISM
Activity in galaxies spans from centrally located active galactic
nuclei (AGN) to more extended but less powerful starbursts, although
in some extreme ultra-luminous infrared galaxies (ULIRGs) the
star-powered luminosity may rival that of a compact AGN. Both
phenomena appear to be associated with significant amounts of
circumnuclear gas and high resolution observations reveal that the
HCN, which is much more centralised than the CO, tends to trace gas in
the nuclear regions of Seyfert galaxies (e.g. Tacconi et al. 1996; Helfer & Blitz 1997).
Previously, we (Curran et al. 2000) found, from a survey of 20 Seyfert
galaxies
, an HCN/CO luminosity ratio of
1/6 for all 13 HCN
detections, a ratio similar to that of ULIRGs. We were, however,
surprised, to find that such a high HCN/CO luminosity ratio holds for
both the "distant'' sources (of recessional velocity
km s-1, where the beamwidth exceeds
10 kpc)
and the "near-by'' sources (
km s-1, beamwidth
10 kpc), since we expect a larger CO contribution from the
galactic disk in the distant sources, which would result in a lower
/
ratio compared to the near-by galaxies.
Since the results of Curran et al. (2000) were based on single-beam observation, at the
centre of the source, these results suggested that either:
- 1.
- For the near-by galaxies we have sampled most of the CO in our single beam observation;
- 2.
- The HCN is more extended than the beam in the near-by sources;
- 3.
- Or perhaps the most plausible explanation, simply that the mean luminosity ratio differs between the near-by and distant galaxies.
There may also exist different angular CO distributions between the
near-by and distant galaxies, since for the latter sources the high
HCN/CO luminosity ratio may suggest that the CO is highly centralised
(as is believed to be the case for the HCN; within
1 kpc, Downes et al. 1992; Nguyen et al. 1992; Tacconi et al. 1996).
Interestingly, the mean values of the far infrared luminosities
are
and
for the full distant and
near-by samples respectively
(including the galaxies where Curran et al. 2000 did not detect HCN).
In the case of ULIRGs, the higher FIR luminosity (
)
is an indicator of a high central CO
concentration (Bryant 1997), and the high values of
in
our distant sample may also imply a selection effect, in which our
distant sources comprise mainly of galaxies suffering from little CO
contamination from the galactic disk.
It is thus probable that in the distant galaxies we sample the whole
CO and HCN. In the near-by sources, however, it is possible that the
full distributions are not mapped. In order to account
for the limitations of the sampling by our single beam of regions of
different linear extent, in Paper I (Curran et al. 2001b) we mapped the
distribution of CO and HCN in order to assess the contribution of
the galactic disk and to take into account the total molecular gas
content of each galaxy.
In this paper we shall use the results presented in Paper I to study
the CO to HCN
luminosity ratios and compare these with the FIR
luminosities: In ULIRGs, the relatively high HCN luminosities are
believed to be due to the presence of dense star forming cores
(Solomon et al. 1992). However, in the case of Seyferts this excess of
(denser) gas traced by the HCN (as well as the excess FIR) may also be
due to the accumulation of gas around the active nucleus, terminating
in the obscuration (Kohno et al. 1999; Curran et al. 2000), and a large fraction of the gas
traced by the CO may act as a resevoir for star formation in Seyferts
(Curran 2000a; Curran et al. 2001a). In this paper we shall also discuss the
CO
/CO
ratios for the Southern sources
in which we could observe this higher CO transition with SEST.
2.1 HCN and CO
distribution in the near-by sample
In this section we refer to the spectral maps shown in Figs. 1 to 6 of Paper I,
which we show, as well as the CO
maps, here as contour plots (Figs. 1 to 17). We also describe the gas distribution in individual sources and then
we summarise the gas distribution trends.
2.1.1 NGC 1068
Although fairly confined (
HPBW), there is still significant amounts of CO emission at map
positions adjacent to the central position, although most of the CO
emission is within one 44'' beam from the centre (

kpc). The HCN shows a similar distribution although the emission in
the adjacent positions is more marginal.
Even though it is faint (Paper I), CO is still detected out to
15 kpc
from the nucleus thus extending much farther than the
HCN (Fig. 21).
![\begin{figure}
\includegraphics[width=8.2cm,angle=-90,clip]{ms1325f1.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg38.gif) |
Figure 1:
Contour map of CO
in NGC 1068. The levels are
up to 75 K km s-1 in steps of 15 K km s-1. Here and in all the
contour maps the integrated intensities are uncorrected for beam efficiencies
and the observed grid points are shown. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f2.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg39.gif) |
Figure 2:
Contour map of CO
in NGC 1068. The levels are
up to 66 K km s-1 in steps of 13 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f3.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg40.gif) |
Figure 3:
Contour map of HCN
in NGC 1068. The levels are
up to 7 K km s-1 in steps of 1.2 K km s-1. |
Open with DEXTER |
Like NGC 1068, we find
80%-90% of the CO emission to be confined within one
34'' beam from the centre, i.e. 
kpc (Sandqvist et al. 1995),
probably in the molecular ring (Sandqvist 1999).
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f4.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg41.gif) |
Figure 4:
Contour map of CO
in NGC 1365. The levels are
up to 66 K km s-1 in steps of 11 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f5.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg42.gif) |
Figure 5:
Contour map of CO
in NGC 1365. The levels are
up to 72 K km s-1 in steps of 14 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f6.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg43.gif) |
Figure 6:
Contour map of HCN
in NGC 1365. The levels are
up to 4 K km s-1 in steps of 0.7 K km s-1. |
Open with DEXTER |
The HCN results are very interesting in that, despite the fact that
this molecule is expected to be confined to within
1 kpc
(Sect. 1), we detected it out to map position
(34'',68''), i.e. at
5 kpc, Fig. 7
, and obtain a source size of 
kpc (Table 1).
![\begin{figure}
\par\includegraphics[angle=-90,width=7.9cm]{ms1325f7.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg45.gif) |
Figure 7:
HCN
at
(34'',68'') in NGC 1365. The
velocity resolution is 80 km s-1 and the moment and baseline
boxes used to determine the main-beam integrated intensity of
K km s-1 are shown. Note that no other HCN was
detected at these distances (we mapped to
). |
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This map position is actually located very close to the major axis of
the radio and molecular rings, i.e. at
(Sandqvist et al. 1995; Sandqvist 1999). It should be noted that no detection was
made towards the corresponding position in the SW (
), and the CO and radio emission does appear to be stronger towards the NE (Sandquvist et al. 1995, Paper I)
Our result implies that there is a significant disk contribution to both the CO and the
HCN luminosity, but the CO disk is much more extended.
We find the CO emission to be fairly confined;
60% of the
emission lies within the central beam (
kpc), which is not
surprising as this is the most distant galaxy of the near-by sample.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f8.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg49.gif) |
Figure 8:
Contour map of CO
in NGC 2273. The levels are
up to 2.3 K km s-1 in steps of 0.4 K km s-1. |
Open with DEXTER |
Our results imply that there is some disk contribution to the CO
luminosity and so we expect the global HCN to CO line ratio to be
affected by disk contamination.
2.1.4 NGC 4945
The CO and HCN may (see Sect. 2.1.8) have similar, and
relatively small, source sizes (consistent with the results of Sandqvist Henkel et al. 1994), probably corresponding to the
pc ring of
Bergman et al. 1992 (1992; Dahlem et al. 1993
.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f9.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg52.gif) |
Figure 9:
Contour map of CO
in NGC 4945. The levels are
up to 370 K km s-1 in steps of 62 K km s-1. Because
of the added position angle to the CO
data of Dahlem
et al. (1993) it was impossible for us to plot this as a contour
plot, which can, however, be seen in their article. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=7.9cm]{ms1325f10.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg53.gif) |
Figure 10:
Contour map of HCN
in NGC 4945. The levels are
up to 18 K km s-1 in steps of 3.6 K km s-1. |
Open with DEXTER |
There is a large-scale CO disk in this galaxy (Dahlem et al. 1993) which will also
significantly affect the global CO/HCN luminosity ratio.
In the nearest galaxy of the original sample (Heckman et al. 1989; 2000), the
CO appears to be quite extended and only about 10% of the emission is
in the central beam (Paper I). The optical disk of the galaxy is very
extended
and it is possible that the structure seen in
our CO map (Fig. 11) is due to spiral arms or other
features. Approximately
of the HCN emission is confined within
the central beam and its structure is dramatically distinct from any
other galaxy in our sample; it appears that the HCN is located in a
bar (Fig. 12).
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f11.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg55.gif) |
Figure 11:
Contour map of CO
in NGC 5033. The levels are
up to 20 K km s-1 in steps of 5 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f12.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg56.gif) |
Figure 12:
Contour map of HCN
in NGC 5033. The levels are
up to 1.3 K km s-1 in steps of 0.1 K km s-1. |
Open with DEXTER |
NGC 5033 is a likely example where the disk contribution could
dramatically affect the global HCN/CO luminosity ratio.
As in the case of NGC 4945, the CO and HCN may (see Sect. 2.1.8) share similar source sizes
([
pc, corresponding to the molecular ring of Curran et al. 1998)
.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.6cm]{ms1325f13.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg57.gif) |
Figure 13:
Contour map of CO
in Circinus. The levels are
up to 80 K km s-1 in steps of 13 K km s-1. Note the
extension of the emission towards the SW in this and
Fig. 14, where this portion of the molecular ring
(Curran et al. 1998) is 1.4 times more luminous than the NE portion
(Curran 1998) corresponding to enhanced star formation
(Marconi et al. 1994; Marconi et al. Curran 2000). |
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![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f14.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg58.gif) |
Figure 14:
Contour map of CO
in Circinus. The levels are
up to 78 K km s-1 in steps of 13 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=7.9cm]{ms1325f15.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg59.gif) |
Figure 15:
Contour map of HCN
in Circinus. The levels are
up to 5.5 K km s-1 in steps of 1.1 K km s-1. Like Figs. 13
and 14 this also shows an extension of emission towards the SW. |
Open with DEXTER |
The contour maps show that there is significant disk
contribution to the CO luminosity which will cause the HCN to CO
luminosity ratio to decrease with increasing radius.
2.1.7 NGC 6814
While there are significant amounts of CO located away from the
central beam, most of the emission is confined within the
adjacent map positions. Only
30% of the HCN is located
within the central beam, and in fact there could be significant emission
at
6 kpc (to the east) from the centre. Due to the incomplete map
(Paper I) we were unable to produce a contour plot for this molecule.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f16.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg60.gif) |
Figure 16:
Contour map of CO
in NGC 6814. The levels are
up to 4.7 K km s-1 in steps of 0.9 K km s-1. |
Open with DEXTER |
![\begin{figure}
\par\includegraphics[angle=-90,width=8.2cm]{ms1325f17.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg61.gif) |
Figure 17:
Contour map of CO
in NGC 6814. The levels are
up to 2.3 K km s-1 in steps of
K km s-1. |
Open with DEXTER |
2.1.8 Source size fittings
The source sizes were measured assuming that the source distribution
on the sky is Gaussian and deconvolving the telescope response (HPBW)
from the full-width half-maximum (FWHM) diameter (see Paper I). It
should be noted that the source size concept could be misleading here:
The source sizes may seem similar because all galaxies have bright CO
emission coming from their centres, thus causing the source size fits
to look the same for HCN and CO
.
Additionally, for many galaxies (like
NGCs 4945 and 5033) there is low level disk emission (which is
sub-thermally excited) which will contribute significantly to the
luminosity, but only little to the source size fit. We show the
fitted source sizes for the different transitions in Table 1.
2.1.9 Summary
In general we see that the HCN is rarely confined to 1 kpc in the FIR
weak (near-by) galaxies (Paper I and Table 1) although it
does appear to be more concentrated towards the nucleus than the CO
(Table 2), thus indicating significant CO contamination in
the galactic disk.
Table 2:
The approximate CO/HCN luminosity
ratios for the near-by sample over the telescope beam (i.e. as in Curran et al. 2000), over the HCN map and over the full CO mapped region.
Galaxy |
 |
|
Beam |
HCN Map |
CO Map |
NGC 1068 |
8 |
9 |
20 |
NGC 1365 |
11 |
11 |
19 |
NGC 2273 |
5 |
- |
- |
NGC 4945 |
13 |
20 |
35 |
NGC 5033 |
7 |
12 |
27 |
Circinus |
15 |
33 |
45 |
NGC 6814 |
9 |
12 |
12 |
Average |
9 |
16 |
26 |
Returning to Section 1, we can rule out the first option, i.e. that we
had previously sampled most of the CO in the near-by
sample
, and attribute our previous results to points 2 and 3 (addressed
in Sect. 2.2).
2.2 Luminosity ratios
In order to simultaneously analyse the two samples, in the following
we use the full map (global) values (last column Table 2) for the
near-by sample and the central beam values, which are analogous to these, for the distant galaxies.
![\begin{figure}
\includegraphics[angle=-90,width=8.6cm]{ms1325f18.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg68.gif) |
Figure 18:
versus
(units as
in Fig. 5 of Curran et al. 2000 i.e.
K
km s-1 kpc2) for all the
detections. From these we obtain
a mean fitted ratio of
and
using only sources with km s-1, we obtain
a ratio of
. |
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As in Curran et al. (2000), in Figs. 18 and 19 we plot
and
against
for all of the sample. Unlike previously, where we obtained
for all of the detections and using
only sources with
km s-1, we find a definite
difference between the distant and near-by samples, i.e.
(distant) and
(from Paper I and Table 2). In fact all of
the
km s-1 sources lie to the left, above the fitted mean ratio
line and, with the exceptions of NGCs 5135 (v=4112 km s-1) and
7130 (v=4842 km s-1), the
km s-1 sources lie to
the right, below the line, Fig. 18.
Again (Curran et al. 2000), in order to determine the far infrared/HCN
luminosity correlation, i.e. compare our results with those of
Solomon et al. (1992), we plotted
against
,
for all of the
sources, Fig. 19. Once again we see that we obtain a
fairly linear (on a log-log plot) relationship between the FIR and the HCN luminosities and
from this we determine
(cf.
previously). For the near-by and distant sources we obtain
and
,
respectively,
suggesting additional FIR flux over and above that associated
with the denser molecular gas in the distant sample.
All of the near-by sources except NGC 1068 and Circinus lie below the
line, i.e. like the distant sample, these two galaxies exhibit an excess in FIR
compared to HCN. This also holds when, in order to account for the
distances and the extents in our sample Solomon et al. (1992; Curran et al. 2000), we plot
against
,
Fig. 20.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.6cm]{ms1325f20.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg82.gif) |
Figure 20:
[
]
versus
normalised by the CO luminosity for all the detections [no units]. From this fit we also find
. |
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From this, however, we see a large change in the position of NGC
4945 relative to Circinus in the figure. As suggested by Forbes & Norris (1998), this may indicate that
not all of the FIR in NGC 4945 was sampled by
Rice et al. (1988)
, although the shift in
position for this galaxy does not appear to cause an abnormal deviation from
the fit defined by the other Seyferts.
We discuss the various luminosity relationships further in Sect. 3.2.
2.3 CO
/CO
In Table 3 we present the CO
luminosity ratio for the Southern sources in which we could
simultaneously observe the CO
and
lines. For the distant sources (NGCs 0034, 4593, 5135, 5548, 7130 and
7469) we could not map the CO
emission, and therefore
have no direct information on the CO source sizes. To estimate the
line ratios we have therefore used the suggested correlation between
the (low frequency) radio continuum and molecular gas distribution
(e.g. Allen 1992; Bajaja et al. 1995). We found radio continuum images for 7 of
the sample galaxies and used these to make estimates of the CO source
sizes
(see Appendix A of Curran et al. 2000b for details).
On the whole, our results seem consistent with those of Papadopoulos & Seaquist (1998),
except in the cases of NGCs 0034 and 1365.
In the former galaxy, when we look at the main beam brightness
temperatures of Papadopoulos & Seaquist (1998), we see that they obtain
10 mK
for CO
in a 55'' beam and
7 mK in a 9 point
grid map which convolves the 32''
beam to the
beam size. At the distance of NGC 0034 these beam sizes
correspond to diameters of 21 kpc and 12 kpc for the
and
transitions, respectively. At these linear scales we would be
surprised if the molecular gas filled the central beam
in this, one of our distant
(v=5931 km s-1) sample galaxies. For a point source the
intensity ratio should be divided by a factor of
and where the beam is filled no
correction is required. So we feel that the Papadopoulos & Seaquist (1998) ratio would
be better quoted as 0.2-0.7 (i.e. somewhere between these two cases). The
upper value is still consistent with their stated result and it should
be remembered that our ratio is merely an estimate from the radio
continuum, although it does lie in the range we obtain for the
Papadopoulos & Seaquist (1998) result and in the two cases where we do have both CO and
radio continuum maps (NGCs 1365 and 6814, Table 3), we find
fair agreement in the values. In the case of NGC 1365, we believe that
the opposite effect may be the cause of the discrepancy between our
ratio and that of Papadopoulos & Seaquist (1998), i.e. that their 
beam
is insufficient to map all of the CO, which is seen out to
(Fig. 2 of Paper I), in this near-by galaxy. Referring to
Table 3 of Paper I, we note a CO
/
luminosity ratio of
over the central beam. This is more
consistent with
Papadopoulos & Seaquist (1998) and (unlike NGC 4945) the increasing CO
/
ratio with galactocentric radius perhaps suggests
more vigorous star formation at larger radii (next paragraph).
Note that our two closest examples (which also share similar intrinsic properties, see Curran et al. 2001a), NGC 4945 and Circinus, have the
most extreme values (one at either end of the range, Table 3) of global CO
.
The
ratio is also
significantly higher in Circinus. Comparing the results with those of
Curran et al. (2001a) who suggest that star formation may be more dominant in this galaxy,
implies that the CO may be excited by large-scale star-burst activity for which
the HCN does not necessarily provide a good tracer
(Curran et al. 2001a and Sect. 3.2).
For all of our galaxies the HCN/CO luminosity ratio increases
towards the nucleus (Table 2), and when we combine our results
with those of previous interferometric observations for the much studied NGC 1068,
Figs. 21 and 22,
![\begin{figure}
\par\includegraphics[angle=-90,width=8.6cm]{ms1325f21.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg98.gif) |
Figure 21:
The CO to HCN intensity/luminosity ratio variation with distance
from the nucleus of NGC 1068. HB95 refers to data taken from Helfer & Blitz (1995),
CAB00 from Curran et al. (2000) and HB93 from Helfer & Blitz (1993). The star-burst
activity in this galaxy is associated with the CO ring of radius 0.9-2.4 kpc
(Myers & Scoville 1987; Planeas et al. 1991). Around these radii
it is seen that the ratio appears to follow an increasing trend (a detail is
shown in Fig. 22) and although there is relatively little CO out in
the galactic disk ( 15 kpc, see Paper I), the ratio is very high due to near total
lack of HCN. |
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![\begin{figure}
\par\includegraphics[angle=-90,width=8.6cm]{ms1325f22.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg99.gif) |
Figure 22:
Detail of Fig. 21 showing the CO to HCN intensity/luminosity within the galactic bulge of NGC 1068 (a second order polynomial fit is shown). It is seen here that the relative HCN abundance
continues to increase within the inner radius ( 1 kpc) of the star forming ring,
perhaps supporting the results of Curran et al. (2001a) who suggest that HCN abundances may
not be the best tracer of star-burst activity. |
Open with DEXTER |
we find that, while the HCN/CO ratio is high within the star-forming
region
, the ratio keeps increasing within this radius:
In AGN the growth of the central super-massive black hole is regulated
by the ongoing star-burst with which it competes for the in-flowing
material. While the presence of a star-burst will restrict feeding to
the black hole, there is expected to be an inner limit to the
proximity of this star formation, since tidal effects will exert shear
on the parent gas clouds, tearing them apart
(e.g. the inner limit for a molecular cloud of density 104
approaching a
black hole is 55
pc, Lang 1980; Maiolino & Rieke 1995). As well as this, ionising radiation from the
black hole will hinder star formation in molecular clouds
(Silk & Rees 1998). For example, in NGC 7214 the star formation rate is
found to increase with distance from the nucleus (Radovich et al. 1998) and in
Circinus the star-burst is seen to occur at
200 pc from the
nucleus (e.g. Marconi et al. 1994)
,
while in the star-burst galaxy NGC 253, the nucleus is apparently
dominated by stars (Ulvestad & Antonucci 1997; Vogler & Pietsch 1999). In this, and all galaxies,
a super-massive black hole may also exist, although the presence
of stars close to this may still be permitted due to the low activity of the black hole (no
mega-masers are observed, see Curran 2000b)
,
which could be the consequence of a low feeding rate (Bryant & Hunstead 1999).
For example, although such a black hole is believed to be present in the
Galactic centre (e.g. Kormendy & Richstone 1995), young stars are observed
very close to this (e.g. Okuda et al. 1990; Nagata et al. 1990; Nagata et al. 1995).
Finally, from Table 2 and
Fig. 21, we see again that contamination by CO in the disk is
indeed an issue, although from the average value of
over the HCN map (Table 2) we can see that any such contamination which
may exist in the distant sample is still not sufficient to bring a similar
average luminosity ratio between the two samples.
Previously, we suggested this difference in the luminosities could be due to a selection
effect, i.e. we only detect the FIR bright galaxies at these distances
(corresponding to
km s-1) and so the distant sample
may be intrinsically different, not only in its FIR and molecular gas
luminosities, but in gas distributions to the near-by sample. Now that we
have complete CO luminosity values for the near-by sample, we can say
that this certainly seems to be a possibility. That is, that in order
to produce the high HCN/CO ratios in the distant sample we could have
relatively little disk contamination, at least in relation to the HCN
which seems to be considerably more extended than previously
thought
(Sect. 1).
Returning to the ratios, we see a decrease of relative CO luminosity
with FIR luminosity (Fig. 23) which implies, not only
that the distant sources are more FIR bright (Sect. 1), but that this is
in excess relative to CO. This could arise either from
young stars and/or the AGN, both of which we would expect to also be
traced by the HCN (Curran et al. 2001a).
In the former situation we would expect the
ratio to be fairly independent of the FIR luminosity of the galaxy and
in the latter we might expect this ratio to increase
(see Curran et al. 2000), i.e. a further FIR contribution than that of the
star formation. Plotting the
ratio versus
(Fig. 24) we see that the HCN/FIR ratio may well
decrease with the FIR luminosity, perhaps indicating that the latter
scenario may be the case. Although, as well as the elevated FIR
emission due to the accumulation of HCN towards the nucleus (as
opposed to star forming regions), the HCN luminosity may also increase
accordingly (Curran et al. 2001a and references therein), although
Fig. 21 suggests that while the HCN/CO ratio is as high as
that of ULIRGs over the region of enhanced star formation, there
exists excess HCN at smaller radii, indicating correspondingly higher
FIR luminosities at these radii. So rather than a matter of relative
luminosities, the question becomes a matter of distribution: How much
dense gas/FIR emission arises from the nucleus with
respect to the 100 pc-scale star forming ring
(Curran 2000b and references therein)?
From Figs. 19 and 20 there appears to be no FIR to HCN excess in
comparison with normal spirals and ULIRGs (Solomon et al. 1992)
.
![\begin{figure}
\par\includegraphics[angle=-90,width=8.6cm]{ms1325f24.ps}\end{figure}](/articles/aa/full/2001/26/aa1325/Timg110.gif) |
Figure 24:
[
]
versus
[
]. As in Curran et al. (2000) the least squares linear fit is shown. |
Open with DEXTER |
This may be caused by the possibility that both the FIR
and HCN emission could come from stars and material surrounding the
central engine
. In an attempt to distinguish between these two sources
of radiation, we note:
- 1.
- From above,
,
giving a FIR excess in the distant sample;
- 2.
- From Fig. 23 we note an excess of FIR in comparison to CO
emission in the distant sample. In order to approximately quantify this:
- a.
- From Fig. 18 and Paper I we find
i.e. also an excess of HCN emission in the distant sample.
- b.
- Multiplying this with the previous equation gives

.
This is a very rough calculation which assumes an average distant
source compared to an average near-by source and the value is probably
considerably greater than 4 (i.e.
10, Tables 3 and 5 of Paper
I). It does show, however, that both HCN and FIR are in excess in the
distant sample but that the FIR increases more rapidly than the HCN
luminosity with the FIR output of the galaxy. Why should this be if
the HCN and FIR are signatures of both star and nuclear activity? One
possible answer
could be that while both the line and
thermal emission arise from cloud cores and nuclear gas, the
beam-filling in the latter would be considerably less than in the more
widely distributed HCN associated with star formation
(Helfer & Blitz 1993; Sternberg et al. 1994; Helfer & Blitz 1995; Tacconi et al. 1998). Since the FIR radiation actually
originates from re-radiation by the dust grains
(e.g. Rees et al. 1969; Rieke 1978; Lebofsky & Rieke 1980), we expect this to be a lot more
isotropic and therefore not so seriously affected by the
beam-filling
.
- 3.
- Applying this argument to the results of Curran et al. (2001a):
- a.
- Both NGC 4945 and Circinus are well known for their vigorous star-burst activity (e.g. Harnett et al. 1990; Dahlem et al. 1993; Moorwood et al. 1996; Siebenmorgen et al. 1997; Oliva et al. 1999; Viegas et al. 1999),
and lie close to the other
weaker (near-by) galaxies in Figs. 23 and 24, perhaps
suggesting that such Seyfert/star-burst activity may be fairly typical for the near-by sources.
However, while in the literature we can find a reference to star-burst activity
in each near-by source
, we can also find such references for the distant sample
;
- b.
- Note that in Fig. 18 Circinus exhibits a definite
HCN deficiency (compared to the rest of the sample) and that from
Curran et al. (2001a),
.
This apparently contradicts point 2 (above) since Curran et al. (2001a) believe that NGC 4945 has
greater Seyfert activity and therefore should have more FIR in comparison to HCN emission.
The discrepancy is perhaps due to the possibility that not all of the FIR radiation
has been sampled in NGC 4945 (Forbes & Norris 1998) but also, with regard to point 2, that both
the galaxies are considerably closer (
times) than the distant sample. That is,
the central HCN does provide ample beam-filling, although this would be confused
with HCN in the star forming rings (Bergman et al. 1992; Dahlem et al. 1993; Marconi et al. 1994; Curran et al. 1998).
Note that for Figs. 23 and 24, the errors (Paper
I) as well as variance in the sample could produce an apparent
correlation since we are plotting x/y versus x. This emphasises
the uncertainties in these results making the above points highly
speculative. The real solution to the question of relative
star-burst/AGN contribution is discussed in Sect. 4.
Previously (Curran 2000a), we found for the distant sample that
both the main Seyfert classes had on average similar abundances of molecular
gas, i.e.
 |
(1) |
10
,
for all of the sample. However,
this result was not so certain with the possibility that
 |
(2) |
which supports the results of Heckman et al. (1989), who find a significant
difference in molecular gas abundances between the two main Seyfert
classes. However, note that Eq. (1) supports the results of
Maiolino et al. (1997) and their sample corresponds to our distant galaxies
(i.e. none with v<4000 km s-1). When we
re-examine our results by adding the global
values for the near-by sample, we find that
 |
(3) |
,
i.e. there is no significant
difference in molecular gas abundances between the two main Seyfert
classes.
In order to ascertain the implications of this result, i.e. if the fluxes
could be of different origins between the two classes, we looked at the
HCN/FIR (as well as the CO/HCN) luminosity ratios between the classes. From this it became clear, however, that we would have to
consider the distinction between the distant and near-by samples, e.g. obtaining an
average of
for one of the Seyfert classes,
irrespective of distance, would give a standard deviation which was nearly
as large as the average value. Hence further statistics became meaningless,
i.e. we have only 3 detections of HCN in Sy1s (Curran et al. 2000), one of which is
in the near-by sample (NGC 6814). This analysis emphasised that although Eq. (3)
is valid in that it still holds
, there is
little point in assigning an average value between the distant and near-by samples,
which are evidently quite different. So all we are justified in stating is that
 |
(4) |
for v>4000 km s-1, and that it is clear that
statistics will have to be very much improved in order to
determine if the relative HCN luminosities vary between the two main
Seyfert classes. Note that, from the distribution of the number
of sources binned according to the flux, Thean et al. (2001) find, on the
whole, that Sy2s are marginally more likely to have stronger 60
m
infrared emission than Sy1s, perhaps suggesting a more dominant
starburst contribution in the former.
Only for four of the galaxies (NGC 1365, NGC 5548, Circinus and NGC 7172) does the
CO
ratio appear to be
(Table 3). So for
most of the sample the CO emission seems to be sub-thermally excited,
indicating densities below
cm-3.
This belies the bright
HCN emission emerging from several of these objects, e.g. NGC 0034, which suggests gas densities
cm-3. This
discrepancy could be resolved if the CO
source size is
larger than that
of the CO

, so
that regions of sub-thermally excited emission lie outside (at larger
radii) those of bright HCN emission, leaving the CO
source size closer to that of the HCN
,
although we see
from Table 1 that this doesn't appear to be the case. This
would also mean that a pointing error would be more serious in the
transition due to the smaller beam and (perhaps)
source size. Another possibility is that there is perhaps a mixture of
low and high density gas in the inner region, causing a large filling
factor of diffuse, unbound low density gas embedding clumps of higher
density gas. Models on the production of such a medium have been
discussed by Jog & Das (1992). In order to check this, high resolution,
multi-transitional observations of CO combined with further studies of
the emission from high density tracer molecules are necessary,
although cases of sub-thermally excited CO emission from luminous
mergers have been discussed before (e.g. 1992; Aalto et al. 1995). For
ULIRGs the situation is even less clear: Many seem to have very
sub-thermal global CO
/
line ratios
although we believe that the CO emission is very concentrated (i.e. no
extended disk distribution). For these the idea of a diffuse, low
density inter-cloud medium will work very well, thus being both under
high pressure and hot, the CO
/
line
ratio will still be low due to low densities and large velocity
gradients.
4 Conclusions
From complete mapping of the molecular gas in the near-by sample of Curran et al. (2000) and comparing
the results with those for the distant sample, it appears that:
- 1.
- We had not previously mapped most of the CO in
the near-by galaxies.
- 2.
- This is also true for the HCN which is much less confined that
previously thought.
- 3.
- There does exist a distinct difference between the near-by and distant sample.
Elaborating on this last point, it seems that there is a selection effect in which
we only detect the very FIR luminous galaxies (
)
at recessional velocities in excess of
4000 km s-1. These galaxies
have either incredibly high HCN/CO luminosity ratios
(
1 as in Mrk 273, Curran et al. 2000) within their star forming regions or, unlike the near-by galaxies, the CO is extremely confined resulting
in little contamination by this molecule in the galactic disk.
As well as this we find:
- 1.
- Low global CO
ratios for two thirds of the sample, possibly suggesting sub-thermally excited CO;
- 2.
- No significant differences in the CO luminosities between the type 1
and type 2 Seyferts of the sample;
- 3.
- That the HCN/CO ratio in the near-by sample increases with proximity to the nucleus, possibly further increasing in beyond the region of powerful star formation.
Although this latter point and our other analysis may hint at an
increased AGN (cf. stellar) contribution to the FIR emission in the
near-by and distant galaxies (respectively), we feel that the key to
this puzzle is not improved statistics but actual mapping of the
molecular gas distributions in these sources. Such projects would
require interferometric observations
which
should prove to be worthwhile projects, particularly for the more
distant galaxies, when very high resolution interferometers (such as
ALMA
) become available.
Acknowledgements
We wish to thank the referee R. Antonucci for his prompt and helpful
comments as well as Kate Brooks at the La Silla 3.6 m telescope for her
advice. This research has made use of the NASA/IPAC Extragalactic
Database (NED) which is operated by the Jet Propulsion Laboratory,
California Institute of Technology, under contract with the National
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