Issue |
A&A
Volume 521, October 2010
|
|
---|---|---|
Article Number | L51 | |
Number of page(s) | 5 | |
Section | Letters | |
DOI | https://doi.org/10.1051/0004-6361/201015042 | |
Published online | 01 October 2010 |
Online Material
Appendix A: A cautionary note on observations of extended sources
As part of the performance verification of HIFI in space, spectroscopic
observations of the 12C16O
576.3 GHz transition
were obtained at the position of the chemically-active bow shock B1
driven by the LDN 1157 Class 0 protostar (Bachiller et al. 2001).
Initial observations in HIFI's Band 1B were made on August 1,
2009; a second set was obtained 186 days later on February 4,
2010. The spectral shape of the source remained essentially unchanged
but initially the signal from the high-frequency edge of the line
appeared stronger in the V direction, when the H and V peaks
were matched, whereas half a year later it appeared stronger by the
same ratio in the H direction.
This ``false polarisation'' effect was due to the small misalignment of
the H and V beams described earlier, which imaged slightly
different portions of a scene onto the two receivers (Attard et al. 2008).
Unless otherwise specified, observations of a targeted source are
centred on a position halfway between the two beam centres. Because
the viewing direction of Herschel at all times is constrained by the
need to keep the plane of the sun-shield roughly perpendicular to
the radius vector to the Sun, sources close to the ecliptic plane
can only be viewed at half year intervals. Over this interval the
telescope aperture rotates 180
about its viewing direction
on the sky. Thus, portions of LDN 1157 B1 initially viewed
by the V channel were viewed, half a year later, by the H channel
and vice versa. It is clear that this effect was not due to linear
polarisation because a 180
rotation of the telescope leaves
the polarisation direction unchanged.
For VY CMa, where the entire source was relatively well centred on each beam, this effect was negligible. But for linear polarisation observations of an extended source the best strategy may be to make a small map with HIFI over the area of interest, where the spectra obtained in the H and V channels at each position of the source, can be individually and directly compared.
Appendix B: Ground-based observations at 22.235 GHz
Overlapping with the second epoch of 620.701 GHz observations, we observed the VY CMa 22.235 GHz maser with the Effelsberg 100-m telescope of the Max-Planck-Institut für Radioastronomie. Those observations were begun on April 11, 2010 at 16:40 UT and lasted until 17:20 UT and are shown in Fig. 3. Data in two linear polarisations were obtained with the two channels of the K-band or 1.3 cm receiver at the primary focus. The frequency resolution was 6.104 kHz, corresponding to a velocity resolution of 0.082 km s-1. Although these observations were realised at only one epoch and are, therefore, insufficient for a full characterisation of the linear polarisation state, a search by Vlemmings et al. (2002) found that the linear polarisation of the VY CMa 22.235 GHz masers is well below 1%.
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