CO radio line emission and far-infrared dust emission are both good probes
of the stellar mass-loss on the AGB. The gas and the dust are also
connected to each other in the "dust-driven wind''-scenario
(Sedlmayr & Dominik 1995). Therefore, an observational test of the
correlation of the two emissions can be useful. In Olofsson et al.
(1993) integrated CO line intensities, as we present in
this paper, were plotted against the IRAS 60m flux densities.
The latter is known to provide a reasonable measure of the dust mass
loss rate (Jura 1987).
Since we have data from different telescopes and up to four
transitions we selected only data from the most frequent
observatory/transition combinations for a similar comparison.
As argued in Olofsson et al.
(1993), as a first approximation, intensities measured at
different telescopes should scale in proportion to the beam-areas. In
such a way CO (1-0) data from SEST where scaled to the OSO
scale by multiplying them with 1.8 (the observational results of
Olofsson et al. 1993, suggest a value of 1.5 for visually
bright C-stars). For the other transitions only data from a single telescope
were used (2-1 from SEST, and 3-2 from JCMT). Plots of
versus
for the three lines show positive
correlations, but with some substantial scatter. The slopes of linear
fits are very similar for the three transitions,
, but
considerably lower than the results for the C-stars where the CO line
flux varies essentially linearly with the far-infrared flux
(slope
1.0, Olofsson et al. 1993). In order to
study this in more detail we have made a first order correction for
the distance using K-magnitudes from the literature (mainly SR_IIa,
SR_IIb, Lb_I). The resulting diagrams are shown in
Fig. 8.
There is very likely a positive correlation in the expected way (e.g., the
open circles in the CO(3-2) plot are approximately fitted with a line
of slope 1), but the scatter is large in all diagrams. Parts of the
scatter in I can be attributed to calibration uncertainties, but
these are expected to be significantly less than 50% for the large
majority of the stars. Parts of the scatter in S60 could be a stellar
contribution to the 60m flux density. We have estimated this by
fitting combinations of two blackbodies to the spectral energy
distributions (see SR_III). It turns out that the stellar
contribution is typically only 10% with a relatively small scatter
around this value, and consequently this can only lead to minor shifts
in the figures (preferentially shifting the low
objects
to the right). The crude distance correction will also lead to a
scatter, but it will affect
and
in the same way.
However, none of these effects can explain the fact that the
scatter is substantially larger in
than in
. A more detailed analysis of both the CO and the
dust emission is required to understand this scatter in detail, but we
suggest here that it points to a difference in the mass
loss properties of these stars.
We note first that in a given -interval the bluer
objects (in
) lie significantly lower in
. We
find also that objects with very low
-values also
have low gas expansion velocities (
km s-1). The extreme
case is that of L2 Pup with an expansion velocity of about
2.5 km s-1, one of the smallest ever measured for an AGB-star.
Some indication of an IR-colour dependence of the gas and dust
mass-loss relation is found in Nyman et al. (1992). They
found a difference in slope (of linear fits) in
versus
-diagrammes between objects in regions II and IIIa of the IRAS
two-colour diagram (although there are relatively few objects in
region II, and both groups may contain C-stars).
We tentatively conclude from this that it is the intergrated CO intensity that
is anomalously low for the blue, low objects (as judged from
the IRAS two-colour diagramme the 60
m flux densities are normal). This
could be due to a higher, in a relative sense, dust content in these objects
suggesting that dust plays less of a rôle
for the gas mass-loss of optically bright, O-rich IRVs and SRVs than
it does for higher mass-loss rate O-rich objects and C-stars. Possibly,
shock waves or radiation pressure on molecules dominate here (e.g.,
Höfner et al. 1998). Alternatively, these envelopes are so thin
that photodissociation of CO makes CO radio line emission a less reliable mass loss
estimator. We cannot exclude that also temporal mass loss rate variations have an
effect on this ratio since the CO line and the dust continuum emission do not
probe the same regions (epochs).
Recently, Josselin et al. (1996, 1998), argued
that the ratio can be used to discriminate
between AGB-stars and supergiants. For the former the ratio falls in
the range 20-220, while the latter only show ratios
(using the IRAM intensity scale for the CO data). In
Fig. 9 we present the distribution of this ratio for our
sample (OSO scale for the CO data; OSO and SEST data were combined in
the way desribed above).
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