Up: New CORAVEL spectroscopic-binary orbits II
The same presentation strategy as in Paper I is adopted. The orbital
elements and the phase-folded radial-velocity curves are provided for
the binaries with stable orbital solutions. Badly constrained
parameters are readily identifiable by their large uncertainties. In
case the period has to be fixed to obtain a satisfactory orbit, it is
fixed to a minimized value determined by the minimum residue
around the obtained solution. In such a case, no uncertainty is given
for the fixed period. When the star is clearly binary but the period
is not sufficiently covered to derive a preliminary orbit, only a
minimum period is given. The radial velocities in function of Julian
dates are then displayed.
Figure 1 and Table 1 provide the results for the
strong barium sample (8 orbits) whereas Fig. 2 and
Table 2 give the information for the mild barium binaries (10
orbits + 2 minimum-period binaries).
![\begin{figure*}
\centering
\includegraphics[width=15cm]{o2fig1.ps}\end{figure*}](/articles/aas/full/1998/13/ds1500/Timg5.gif) |
Figure 1:
Phase-folded radial-velocity curves for the strong barium
stars. Open circles are for DAO measurements |
![\begin{figure*}
\centering
\includegraphics[width=15cm]{o2fig2.ps}
\vspace{1cm}\end{figure*}](/articles/aas/full/1998/13/ds1500/Timg6.gif) |
Figure 2:
Phase-folded radial-velocity curves for the mild barium
stars. Open circles are for DAO measurements. Due to the non-complete
coverage of the orbit a minimized period has been fixed for
HD 53199. Long-period stars without orbital solution have their radial
velocities displayed as a function of Julian dates |
![\begin{figure*}
\centering
\includegraphics[width=14.5cm]{o2fig2b.ps}\end{figure*}](/articles/aas/full/1998/13/ds1500/Timg9.gif) |
Figure 2:
continued |
Table 1:
Orbital elements for the strong barium stars. N is the number of
measurements used to derive the orbital solution and O-C the residue
around this solution.
is the span of the observations
|
For the uncompletely-covered star HD 53199, the period has been fixed
to a minimized value. In a few cases
(see Jorissen et al. 1998), even though the Lucy-Sweeney test was compatible with a
circular orbital solution (Lucy & Sweeney 1971), the
free-eccentricity solution has been given because their is no
physical argument to prefer circular orbits in the case of barium
stars. Two stars ( HD 46407 and HD 223617) have an orbital solution
derived from a combined set of CORAVEL measurements and radial
velocities obtained at the Dominion Astrophysical Observatory (DAO) by
McClure & Woodsworth (1990). The fair number of new CORAVEL measurements allows us to slightly improve the previously published
orbits.
Finally, the star HD 101079 deserves a comment. Only 7 CORAVEL radial-velocity measurements are available to date. They permit to
derive two equally-probable orbital solutions with periods of 1588d
and 3120d. In the coming months, new measurements will allow us to
decide between the two solutions but for the moment only a minimum
period P>1550 d is given in Table 2.
Table 2:
Orbital elements for the mild barium stars. No uncertainties are
given for fixed parameters
|
Acknowledgements
This research has been supported partly by the
Fonds National de la Recherche Scientifique (Switzerland, Belgium)
and the University of Geneva (Geneva Observatory).
Up: New CORAVEL spectroscopic-binary orbits II
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