The selection of several suitable spectral lines and the evaluation of
their reliability as a function of broadening and effective
temperature allows the computation of
over the whole spectral range of
A-type stars and a robust estimate of the associated relative error.
Up to 150
,
a statistical analysis indicates that the standard
deviation is about 6% of the
.
It can be seen, in both Figs. 17 and 18,
that the dispersion increases beyond 180
approximately, when
comparing rotational velocities to previous determination by Abt &
Morrell and SCBWP. SCBWP estimate a larger uncertainty for rotational velocities higher than
200
;
nevertheless our precision estimation for a 200
is extrapolated from Fig. 8. Errors
may thus be larger, due to the sampling in Fourier space, which is proportional to
.
In addition, determination of continuum level induces a
systematic underestimation of
that reaches about 5 to 10%
depending on the lines and broadening.
Gravity darkening (von Zeipel effect, von Zeipel 1925) is not taken into account in
this work. Hardorp & Strittmatter (1968) quantify this effect, showing that
could be 15 to 40% too small if gravity darkening is neglected for
stars near break-up velocity. Nevertheless, in a recent work (Shan 2000), this
effect is revised downwards and found to remain very small as long as
angular velocity is not close to critical velocity (
): it induces an
underestimation
lower than 1% of the FWHM.
In our observed sample, 15 stars (with spectral type from B8V to
A1V) have
.
According to their radii and masses, derived from empirical
calibrations (Habets & Heintze 1981), their critical velocities
are higher
than 405
(Zorec, private communication).
Only seven stars have a high
,
so that
.
The fraction of stars rotating near their break-up velocity remains
very small, probably lower than 2% of the sample size.
A systematic shift is found between the values from the
catalogue of AM (1995). This difference arises from the use of the
calibration relation from SCBWP, for which a similar shift is
found. The discrepancy observed with standard
values given by
SCBWP has already been mentioned in the literature.
Ramella et al. (1989) point out a similar shift with respect to the
from SCBWP. They suppose that the discrepancy could come from the models SCBWP used to compute theoretical FWHM of the Mg II line.
Brown & Verschueren (1997) derived
for early-type stars. For low
(up to
60
), their values are systematically higher than those of SCBWP. They attribute this effect to the use of the models from Collins & Sonneborn (1977) by SCBWP; they assert that using the modern models of Collins et al. (1991) to derive
from FWHM eliminates the discrepancy.
Fekel (private communication) also finds this systematic effect between values from AM (1995), which are directly derived from the SCBWP's calibration, and the
he measured using his own calibration (Fekel 1997).
In addition, some stars used as
standards turn out to be multiple
systems or to have spectral features such that their status as a
standard is no longer valid. The presence of these "faulty'' objects in the standard star sample may introduce biases in the
scale. There is no doubt that the list of standards established by SCBWP has to be revised.
The above comparisons and remarks lead us to call into question the
values of the standard stars from SCBWP.
This paper is a first step, and a second part will complete these data with a northern sample of A-type stars.
Acknowledgements
We are very grateful to Dr M. Ramella for providing us the computer program used to derive the. We also thank the referee, Prof. J. R. de Medeiros, for his several helpful suggestions. Precious advice on statistical analysis was kindly given by Dr F. Arenou and was of great utility. We want to acknowledge Dr F. C. Fekel for his help in comparing
with data from the literature. Finally, we are thankful to B. Tilton for her careful reading of the manuscript. This work made use of the SIMBAD database, operated at CDS, Strasbourg, France.
Copyright ESO 2001