ROVER
FIRST LIGHT WITH ROVER
J.S. Greaves - ROE/ATC
Inside the ROVER module. The large blue circle is the
waveplate (blue because it's made of sapphire!). The dark and light
segments are the encoder, which triggers the TTL pulse that is used
for logging the waveplate cycles.
The ROVER spectral-line polarimeter has just seen first light,
although not yet at JCMT. It 'roved' to the IRAM 30m telescope in
Spain in May 2003, under the care of Jane Greaves and Sye Murray -
whom those of long memories may recall from the commissioning of the
UKT14 and SCUBA polarimeters. We observed at 3mm wavelength, in a
variety of conditions ranging from fog to snow to glorious sunshine
(it was daytime!). Some of the first results are shown below.
The main aim of this observing run was to prove, once and for all,
that millimetre spectra-line polarimetry gives real science results
and is not contaminated by instrumental polarization effects. This
has been a long-standing criticism since the early 1980's when the
first attempts were made to measure weakly polarized lines from
molecular clouds. JCMT results published over the last few years have
been very impressive, but there are a number of subtle effects like
sidelobe polarization that are hard to quantify. So, we took
advantage of a unique opportunity to compare the polarization
measured with a waveplate device (ROVER) with the same polarized
source seen with a 'correlation polarimeter'. IRAM have been
developing observations in this mode, using a pair of receivers
accepting the two orthogonal planes of light and extracting the
correlated (polarized) component. Our idea was that if the two
polarimeters produce the same signal, by completely different
methods, then it must be 'real'. There is probably no other telescope
where this could be tried, and we pushed the system to the limits,
including sampling the spectra at an impressive rate of 32 Hz!
Figures 1 and 2 show the results we obtained for the SiO Maser in the
envelope of the star R Leo. Can you tell which is taken with which
instrument?? (They are so close, at first we thought we'd analysed
the same data twice by mistake!). The sharp-of-eye may notice that
there is a flat line in the ROVER data - this is circular
polarization which we can't measure with a half-wave plate. Also, the
percentage of linear polarization is slightly less than with the IRAM
'Xpol' results, because the data are not yet corrected for the
polarizing efficiency of the plate. Apart from that, the shape of the
percentage and angle of polarization curves is exactly the same -
just the proof that has been sought for so long.

Figures 1 & 2 - ROVER and Xpol spectra of R Leo in the SiO v1,J=1-0
line. From top to bottom: total intensity, percentage of linear
polarization, percentage of circular polarization, direction of
linear polarization.
We obtained a few other science results - most importantly, detecting
polarized CO from Mira giant stars, which has never been done before
- and also did some work on optimising observing modes. It turned out
the simplest mode was the best: we simply took data as fast as the
correlator could sample, while simultaneously spinning the waveplate.
Each sample then corresponds to a small range of plate angles, and
can be analysed as though it is all one fixed angle (which is what we
get with SCUBA polarimeter data, for example). To analyse the data,
all you have to do is compare the time stamps of the spectra and the
polarimeter cycles - all done by logging and with a single TTL pulse.
This continuous spinning observing mode (another 'first') was
very efficient and is the way we plan to observe also at JCMT.
The instrument performed beautifully and the only real problem we had
was fitting it in the receiver cabin! I would very much like to thank
the ATC team who built the polarimeter (especially Ian Laidlaw and
Brenda Graham), all the IRAM staff who helped us, and the Directors
who allowed us to take the risk of removing one of the delicate
beam-splitters so we could slide the polarimeter module in instead.
Our IRAM colleagues Clemens Thum and Helmut Wiesemeyer also did
heroic work with getting everything set up and having reduction
software all ready so that we saw the polarization results
immediately they came in. We are all now very pleased with the data
(and also all very fit after running up to the cabin to check the
polarimeter rotation - it's a long way to go, halfway up a 30m!).
The final stages of the ROVER project are to design and test the JCMT
waveplate - hopefully this will be achromatic covering both the A and
B bands, so there will be no need to swap plates. ROVER should be
coming out in spring 2004 to be included in the late stages of ACSIS
commissioning, and will be available to the community as soon as
possible thereafter. And when HARP-B comes online, ROVER will also
provide the world's only imaging spectral polarimeter for the
submillimetre regime. The scientific advances we can then make should
be as dramatic as those made with the SCUBA polarimeter.
back to:> September 2003 Newsletter Index
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Gerald Moriarty Schieven
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