Astron. Astrophys. 322, 256-265 (1997)
5. DO white dwarfs
Hot helium-rich white dwarfs that show He II lines
are classified DO. They are divided according to the presence or
absence of He I lines into a cool DO and a hot DO
region (Wesemael et al. 1985). The cool boundary of the DO sequence is
defined by the so-called DB gap (28000 K K)
in which no helium-rich white dwarfs are known. For the cooler DO
stars with detectable He I lines the ionization
equilibrium of He I /He II provides a
valuable temperature indicator. However, the He I lines
are invisible in the hottest DO white dwarfs and
and g must be derived from a fit of the He II
lines alone, similar to the case of the DA white dwarfs.
An exploratory calculation by Napiwotzki (1995b) resulted in strong
NLTE deviations for a model of a cool DO white dwarf (55000 K). Werner
(1996b) presented a LTE/NLTE comparison of two DO models with
K and K focussed on
effects on the He II lines coinciding to Balmer lines.
Here we calculated a representative grid of model atmospheres covering
the range from K up to 120000 K
( and ), which is
representative for the whole DO class. The result is displayed in
Fig. 7. Line profiles of representative models are shown in
Fig. 8 (see also Dreizler & Werner 1996). At first glance the
temperature dependence of the NLTE deviations is astonishing: strong
effects are present around K. They become
smaller for higher temperatures. The reason for this is the high
sensitivity of the ionization equilibrium of helium at
K. While at higher temperatures the ionization
stage He III is highly dominant the equilibrium is just
flipping from He III to He II in this
cooler region. In addition the flux maximum for a 60000 K DO star is
close to the He II 228 Å ionization edge causing
an overionization of helium.
![[FIGURE]](img70.gif) |
Fig. 7. NLTE effects on important He I and He II lines in the atmospheres of DO white dwarfs. The deviation of equivalent width in percent is plotted
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![[FIGURE]](img72.gif) |
Fig. 8. Line profiles computed for DO model atmospheres at different temperatures ( , ). NLTE is drawn with solid lines, LTE with dashed lines. The profiles are convolved with a Gaussian of 2 Å FWHM
|
From Fig. 7 it can be seen that moderate to strong NLTE
deviations are present for important lines of DO white dwarfs for
virtually the complete temperature range covered by this class.
Especially if one wants to use the full potential of the
He I /He II equilibrium for the
determination it is mandatory to use NLTE model
atmospheres.
© European Southern Observatory (ESO) 1997
Online publication: June 30, 1998
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