Issue |
A&A
Volume 378, Number 3, November II 2001
|
|
---|---|---|
Page(s) | 861 - 882 | |
Section | Interstellar and circumstellar matter | |
DOI | https://doi.org/10.1051/0004-6361:20011202 | |
Published online | 15 November 2001 |
High and intermediate-resolution spectroscopy of Be stars *,**
An atlas of Hγ, He I 4471 and Mg II 4481 lines
1
DASGAL, UMR 8633 du CNRS, Observatoire de Paris-Meudon, 92195 Meudon, France
2
Institut d'Astrophysique de Paris, CNRS, 98bis Bld. Arago, 75014 Paris, France
3
Facultad de Ciencias Astronómicas y Geofísicas, Universidad de La Plata, Paseo del Bosque S/N, 1900 La Plata, Argentina
Corresponding author: J. Zorec, zorec@iap.fr
Received:
19
June
2001
Accepted:
16
August
2001
We present an atlas of Hγ, He i
λ 4471 and Mg ii
λ 4481 line profiles obtained in a 10 year observation period of 116 Be
stars, which enabled many of them to be observed at quite different emission
epochs. From the best fit of the observed He i
λ 4471 line
profiles with non-LTE, uniform () and full limb-darkened
model line profiles, we determined the
of the program stars. To
account, to some degree, for the line formation peculiarities related to the
rapid rotation-induced non-uniform distributions of temperature and gravity on
the stellar surface, the fit was achieved by considering (
)
as free parameters. This method produced
estimations that correlate
with the rotational velocities determined by Slettebak (1982) within a
dispersion
30 km s-1 and without any systematic deviation.
They can be considered as given in the new Slettebak's et al. (1975) system.
Only 13 program stars have discrepant
values. In some objects, this
discrepancy could be attributed to binary effects. Using the newly determined
parameters, we found that the ratio of true rotational velocities
of the program Be stars has a very low dispersion around the
mean value. Assuming then that all the stars are rigid rotators with the same
ratio
, we looked for the value of
that better represents the distribution of
for
randomly oriented rotational axes. We obtained
.
This value enabled us to determine the probable inclination angle of the
stellar rotation axis of the program stars. In the observed line profiles of
Hγ, He i
λ 4471, Mg ii
λ 4481 and
Fe ii
λ 4351 we measured several parameters related to the
absorption and/or emission components, such as: equivalent width, residual
emission and/or absorption intensity, FWHM, emission peak separations, etc.
The parameters related to the Hγ line emission profiles were used to
investigate the structure of the nearby environment of the central star. From
the characteristics of the correlations between these quantities and the
inferred inclination angle, we concluded that in most of cases the Hγ
line emission forming regions may not be strongly flattened. Using a simple
representation of the radiation flux emitted by the star+envelope system, we
derived first order estimates of physical parameters characterizing the
Hγ line emission formation region. Thus, we obtained that the total
extent of the Hγ region is
and that
the density distribution in these layers can be mimicked with a power law
, where
. The same
approach enabled us to estimate the optical depth of the Hγ line
emission formation region. From its dependence with the aspect angle, we
concluded that these regions are caracterized by a modest flattening and that
the
density contrast of the circumstellar
envelope near the star should be two orders of magnitude lower than predicted
by models based on a priori disc-shaped circumstellar envelopes. We found that
the separation between the emission peaks,
, and the full
width at half maximum,
, of the Hγ line emission are not
only sensitive to kinematic effects, but to line optical depth as well. This
finding agrees with previous theoretical predictions and confirms that Huang's
(1972) relation overestimates the extent of the Hγ line emission
formation region.
Key words: stars: emission-line, Be / stars: fundamental parameters / techniques: spectroscopic / line: profiles
© ESO, 2001
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