![]() | ![]() |
Astron. Astrophys. 363, 289-294 (2000) 2. 2-D models and spectral observationsThe 2-D models used here and the limitations of a 2-D approach were
described by Gadun et al. (1999) in detail. The models have a
computational box with sizes
3360 km 2-D models normally produce larger model oscillations than 3-D
simulations. Therefore in these simulations special boundary
conditions at the top and at the bottom of the computational domain
were chosen such that the oscillations were kept as weak as possible.
These conditions were described by Gadun et al. (1999). The total
evolution time of the simulated granulation which was taken into
consideration in our analysis is about
The spectral observations were described in detail by
Kucera et al. (1995) and
Hanslmeier et al. (2000). They were carried out with the Vacuum
Tower Telescope (Observatorio del Teide, Tenerife) using its echelle
spectrograph. Five Fe I spectral lines have been
observed strictly simultaneously with exposure time of 0.3 s:
5434.543 Å, 6494.994 Å, 5576.508 Å,
6301.508 Å, and 6302.499 Å. Their main
characteristics are given in
Kucera et al. (1995). The slit
width was 0.28" and the subsequent spectral profiles are separated by
to 0.17" in the spatial direction. The dispersions of the spectra were
between 3.3 and 4.0 mÅ/px. Only the most quiet region covering
30arcsec on the Sun was used for the computation of the continuum
intensity and the spectral line characteristics (the residual line
core intensity and the Doppler shifts). This region was without
supergranular network activity and was situated close to the disk
center (
© European Southern Observatory (ESO) 2000 Online publication: December 5, 2000 ![]() |