Bibcode
Kerschbaum, F.; Groenewegen, M. A. T.; Lazaro, C.
Bibliographical reference
Astronomy and Astrophysics, Volume 460, Issue 2, December III 2006, pp.539-545
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12
2006
Journal
Citations
14
Refereed citations
12
Description
Aims.In this paper we aim to determine the longest pulsation period of
infrared carbon stars. Methods: .Forty-seven infrared carbon stars
were selected based on (1) IRAS colours and spectral classification from
the IRAS LRS atlas, and (2) known carbon stars with large CO expansion
velocities. Multi-epoch JHKL'photometry was obtained. Results:
.Reliable periods could be derived for 31 stars. The two longest periods
are 840 and 870 days, only slightly longer than the previously longest
known period for a galactic carbon star of 783 days. This is
considerably shorter than the periods of some OH/IR stars. As the
present survey targeted carbon stars that are likely to be among those
with the longest periods expected, this difference appears real. To try
to understand the longest observed period, the synthetic AGB code of
Wagenhuber & Groenewegen (1998, A&A, 340, 183) was fine-tuned to
reproduce the models of Vassiliadis & Wood (1993, ApJ, 413, 641).
For several initial masses the fundamental mode period distribution was
calculated for stars inside observed instability strip. Depending on
details of the adopted mass loss rate, it is found that the mass limit
where a carbon star has a probability of less than 1% of being in the
observed instability strip with a period longer than 900 days is between
2.6 and 3.1 M&sun;. Conclusions: .Synthetic AGB
calculations suggest that the observed upper limit in period can be
interpreted as an upper mass limit of carbon star formation, with a
value of between 2.6 and 3.1 M&sun;, depending on the adopted
AGB mass loss rate. Such a mass limit is predicted by stellar evolution
through the occurence of Hot Bottom Burning where (dredged-up) carbon is
converted into nitrogen; this is predicted to occur at higher masses (~4
M&sun;), although this depends on convection and core
overshoot.