As shown in Table 1 the value
differs somewhat between the three variability groups (59% for the
Lbs, 47% for SRas, and 64% for SRbs). This does not necessarily
have a physical reason, but may be due to a selection effect. The
relatively low value for the SRa variables (the smallest group) is
probably due to the fact that we tried to observe all objects down to
the S60-limit, whereas in the cases of the SRbs and the Lbs we
avoided observations of "blue''-objects (see below), and objects with
very short periods. Consequently, any statistics derived from these
observations has to be very preliminary until we arrive at more
complete samples, but at this stage we find no differences between the
"reddened'' IRVs and SRVs in terms of CO detectability. The total
detection rates are high, 71% for the 10Jy-limit, 63% for the
5Jy-limit and decreasing only marginally to 61% for all observations.
In Fig. 1 we present the detection rate as a function of
the period for the SRVs. The statistics is poor in some period
ranges, but it appears that the detection rate decreases for the
shorter periods (75
), that it is hard to detect stars in the
intermediate period range (
; although the fraction of
stars with interstellar CO confusion is high here), while for the
longer periods (
) the detection rate approaches 100%. For
the Miras observed by Young (1995, Y95) the detection rate
drops drastically when going to periods shorter than 325
(from about 70% to 30%), i.e., a very similar behaviour. Since
we do not expect large luminosity differences among our stars (i.e.,
the sampled volume does not depend on the period), our detection
statistics should be mainly caused by differences in mass-loss rate.
![]() |
Figure 1: Period distribution of the observed SRVs. The different shadings denote the success of detection |
In Fig. 2 we have plotted all our observed stars in
the classical IRAS two-colour diagram (van der Veen & Habing
1988; including the regions introduced by them). There is
no apparent trend in the detection rate with far-infrared colour,
except that the six "bluest'' SRVs, located in region I, were not
detected. For Lbs no objects bluer than 0.36 in
were observed. Our sample objects
populate, as expected, mainly regions II and IIIa. We note that the
fraction of stars where the spectra are confused by interstellar CO
emission increases with redder
and
colours, suggesting that the IRAS fluxes
are not entirely free from an interstellar contribution.
![]() |
Figure 2: IRAS two-colour diagram for the observed stars. The different symbols denote the success of detection |
The IRAS LRS-class is an independent quantity measuring dust mass-loss
in a qualitative sense. Figure 3 gives the detection
statistics for the IRAS LRS-classes. No clear trend is visible. We
detect objects with a silicate emission feature (2n class) as
well as without a clear feature (the latter sources showing only a
"flat'' continuum, LRS-classes 14-17). However, from recent ISO
results (e.g., Kerschbaum et al. 1997) we have indication
that many 1n-class objects show another dust feature at
13 m, normally attributed to corundum (crystalline Al2O3,
e.g. Begemann et al. 1997). Generally, one finds a
stronger 13
m feature for the warmer objects, whereas the colder
ones are dominated by broad silicate emission at 10 and 18
m.
Figure 4 gives the detection statistics for the M-subclasses. There is a trend of increasing detection rate with increasing sub-class (hence decreasing temperature), although we have very few objects with early and late subclasses. This again is comparable to the results on Miras by Y95.
Consequently, the detectability appears not to be very affected by the composition of the circumstellar dust or the stellar atmospheric temperature. However, we are still dealing with a small sample of objects, where we have concentrated on those expected to have circumstellar envelopes.
![]() |
Figure 3: IRAS LRS-class distribution of the observed stars. The different shadings denote the success of detection |
![]() |
Figure 4: Spectral M-subclass distribution of the observed stars. The different shadings denote the success of detection |
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