Issue |
A&A
Volume 509, January 2010
|
|
---|---|---|
Article Number | L7 | |
Number of page(s) | 5 | |
Section | Letters | |
DOI | https://doi.org/10.1051/0004-6361/200913704 | |
Published online | 19 January 2010 |
Online Material
Table 1: Journal of spectroscopic observations.
Table 2: Journal of NACO observations.
![]() |
Figure 6:
Magnetic field measurements using the data obtained in November 2004.
The longitudinal magnetic field is derived following the equation
|
Open with DEXTER |
Appendix A: Observations and data reduction
The observational material discussed in this section includes FORS 1
spectropolarimetric data (Appenzeller et al. 1998) obtained
in the framework of our programs carried out in May 2008 and in December 2008.
Additionally, we used ESO archive data from 2004 obtained in circular
spectropolarimetric mode.These data were used by Wade et al.
(2007) to search for the presence of longitudinal magnetic fields
in a larger number of Herbig AeBe stars. These older observations (see
Table 1) were carried out with a slit width of 0
8
and grism 600B (
). The flux spectra in the ordinary and
extraordinary ray of the Wollaston prism were extracted for all position
angle settings of the retarder waveplate. Since there were no available flux
calibrators observed for this setup in the respective night, we used flux
calibrators taken in normal spectroscopic mode without the Wollaston prism.
The new spectropolarimetric data from 2008 were obtained with the same
instrument, but now equipped with a higher UV response detector system with a
smaller pixel size.
During the December run we have used the higher dispersion
grism 1200B in addition to the data with the 600B grism. In all our
observations the slit width was set to 0
4 to optimize the resolution
for the polarimetric measurements (
and
,
respectively).
The spectrophotometric calibrators retrieved from the archive were observed
without polarization optics on different nights. One source of uncertainty
in the flux calibration is therefore the unclear spectral response of the
wave retarder plates, for which we presume a high throughput over the full
spectral range. However, significant slit losses are expected with this
setup due to the narrow slit widths and the difficult acquisition of the
target on the slit considering the extreme brightness of the target for
8 m-class telescopes. To remedy this difficulty related to the absolute
calibration, we re-scaled the flux at 5500 Å to the monthly average of the
AAVSO visual observations of 9
4 in November 2004 and 8.4 in
December 2008.
In Fig. 2 we present spectrophotometric
fluxes for the Z CMa system in 2004 and 2008, respectively.
Further we corrected the result with the chromatic zero angle of the
super-achromatic half wave retarder plate
.
for the proper interpretation of the measured polarization angle.
To perform linear polarization measurements, a Wollaston prism and a half-wave
retarder plate rotated in 22.5
steps between 0 and 67.5
were
used. For circular polarization measurements the quarter-wave retarder plate
was used at the positions +45
and -45
.
Our FORS 1 data were supplemented by three high-resolution
FEROS spectra (R=48 000) obtained in February and March 2009 to study the
behavior of hydrogen lines. The journal of spectroscopic observations is
presented in Table 1.
To better understand the parameters of the resolved binary system we retrieved all available NACO adaptive optics near-infrared data (Lenzen et al. 2003) from the ESO archive. As for the FORS 1 data sets, the target is rather bright for imaging-mode observations with 8 m-class telescopes, and accordingly the various data sets were taken with a mixed choice of neutral density and narrow band filters. As a consequence we cannot provide absolute photometry for NACO data with the required level of confidence, but only the flux ratio of the two components (see Table 2) and the astrometric parameters of the binary. In case of normal jittered observation sequences we have used the Eclipse data reduction package provided by ESO to NACO users. In other cases we had only two acquisition exposures or a few jitter positions.
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