Astron. Astrophys. 324, 97-108 (1997)
6. Conclusions
A detailed spectroscopic study of
( K, ,
) has shown that it is a low-metallicity star
([Fe/H] ) with overabundances in the s-process
elements. It is a twin of AG Dra studied in Paper I, another
yellow symbiotic exhibiting the `barium syndrome'. The s-process
abundance distribution is best fitted by a single neutron exposure of
mb-1, and a neutron density
, as derived from the observed Rb/Zr ratio.
These results confirm that the s-process synthesis is more efficient
(larger and ) at lower
metallicities, a result already inferred from the study of barium and
CH stars. That trend had been predicted by Clayton (1988) in the case
that is the neutron source responsible for the
operation of the s-process.
The barium syndrome seems to be shared by many yellow symbiotics
( , AG Dra, UKS-Ce1 and S32; see Schmid 1994),
which also appear to be halo objects. This correlation may be a
consequence of the fact that the barium syndrome is more easily
produced at low metallicities. It is moreover argued that
low-metallicity giants reach higher luminosities at a given
than giants of lower metallicities, and thus
suffer from a more severe mass loss making them appear as symbiotic
stars.
The orbital parameters of have been derived
from CORAVEL measurements, and are similar to those of barium stars.
Like the other two yellow symbiotics with known periods (AG Dra and LT
Del), the orbital period (282 d) of falls in the
short-period tail of the distribution of barium stars. Periods for
more yellow symbiotic stars are however required before one can
conclude that this is a systematic effect.
The fact that exhibits ellipsoidal light
variations has been used to narrow down the range of admissible
parameters. However, no solution matching the Geneva evolutionary
tracks could be found. This discrepancy has been interpreted as an
indication that the usual Roche geometry is not applicable to systems
where a strong mass loss from one component is driven by a force
substantially reducing its effective gravity. This effect is also
present in X-ray binaries, and makes the restricted three-body
equipotentials around the (more massive) mass-losing component shrink.
A solution matching the orbital parameters, the ellipsoidal lightcurve
and the evolutionary constraints may be obtained when this effect is
taken into account.
© European Southern Observatory (ESO) 1997
Online publication: May 26, 1998
helpdesk.link@springer.de  |