UKIRT Newsletter : Issue 3 : Special Report : UKIRT Seeing
Measuring Seeing at UKIRT
Tim Hawarden
Head of UKIRT Development, Joint Astronomy Centre, Hilo
NUMBERS IN SHORT SUPPLY
Objective, consistent measurements of image quality at UKIRT have been
few to non-existent in the past, which is distinctly embarassing : such
data are the critical measure of progress in improving the telescope performance.
However, they are not simple to obtain, especially in the technical context
of UKIRT.
Eyeball estimates from the TV have been around for more than a decade,
but are hard to calibrate in the presence of automatic gain control. Image
cross-sections from the SCANCO autoguider were obtained, AAT-style, some
years ago, but required operation with control settings which impaired
our never-too-robust guiding performance, and the conflicting requirements
of detectivity of faint objects and resolving images in any case mean that
image scales are too small for any but the worst seeing to be properly
resolved.
WHEN WE GET GOOD DATA, PROBLEMS GETTING ENOUGH OF IT...
For the last year or so we have secured regular seeing measurements in
engineering time using the JOSE system on IRCAM. This uses the Snapshot
facility on IRCAM and yields time-dependent measures of the Fried length
r0 over a period of a few minutes, taking about 30 minutes in all. This
is hard and invaluable data about the atmosphere over Mauna Kea but given
the variability of all atmospheric properties we just can’t do such measurements
often enough to provide a statistical picture of the effects of our
attempts to improve the telescope performance.
It has long been recognised that nearly-ideal, simply-acquired, performance
measures would be values of the FWHM (say) of well-focussed images taken
with IRCAM using the x2, or preferably, the x5, magnifiers. However, these
were provided as post-hoc add-ons, mainly intended for test purposes, and
cause background level increases and consequently sensitivity losses. So
they were
rarely used until word of regular undersampling with IRCAM in standard
mode (x1 = 0.28" per pixel) began to spread; use of x5 is still a rarity,
although the x2 magnifier is now used on 25-30% of IRCAM nights. This was
encouraging, but it soon became apparent that observers are unlikely to
bother with the x2 magnifier if the seeing is poor ( > 0.7" say) so that
a uniform sampling policy would be required.
Unfortunately, installing and removing a magnifier, and taking measurements
of the image quality with it, takes about half an hour, due to slewing,
installing, focussing, observing, slewing, removing, refocussing ... etc.
So it has clearly been impractical to require observers who are not using
it already to install it several times a night to do image quality measurements
in addition to their own
programme.
This has left us in a dilemma, and we have taken some deliberate steps
to try to solve it. In particular, we feel a strong need to have a seeing
measurement system in place and working, and enough data gathered to allow
before and after estimates to be made of the effects of the mirror cooling
system, which comes into operation late this year.
A PROTOCOL IN PLACE
Our overall objective has been to obtain an objective and unbiassed sample
of the seeing (or rather, the delivered well-focussed image quality) at
UKIRT on all nights that IRCAM is in use. Initially, after a few experiments
with fitting Gaussians, etc., to a selection of x2 images, we decided on
a simple measurement technique involving the TSS’s counting pixels on print-outs
of image cross-sections.
After a little experimentation a standard procedure has been adopted.
This protocol can be found on the public UKIRT web-page (http://www.jach.hawaii.edu/UKIRT/telescope/protocol.html).
Observers are now asked to make hard-copy cross-sections of images from
standard star measurements made soon after focus checks, around the middle
of the first and second halves of the night (if this has the beneficial
effect of gently persuading observers – who do like to know the seeing
– to do more focus checks and observe more standards, which many do NOT
like doing, it’s all to the good). The TSS’s then do the pencil-and-paper
work and record the results in their nightly log, onto which I then pounce
upon next morning and extract into the database ready for analysis and
display.
In case the IRCAM observer is not observing at K at the right time,
or at all (which is in any case rare!) there are now two standardised
system EXEC’s for use with the x2 magnifier and without. These secure 3
images at K. The observations are made using a subset of the UKIRT Faint
Standards to ensure proper S/N on the one hand and a long enough exposure
on the other (to avoid freezing the seeing and inadvertantly doing speckle
imaging!). We find that together with averaging over the 3 images, this
produces a robust result.
I would not ask observers to measure all 5 images from a normal standard
observation unless they were short of entertainment, but hey! if
you’re feeling generous...
Nevertheless, all measures are welcomed as long as they are reasonably
carefully done according to the protocol. For overall statistics we use
only two (possibly averaged) values per night, to avoid bias, but (for
example) one or more series of good measures made approximatly hourly through
several nights would be invaluable to start learning about trends and changes
(I just don't have the gumption to lean that hard on observers to analyse
so many images!).
In engineering time we have secured consecutive, carefully focussed,
image sets with and without the x2 magnifier on 4 occasions. They trace
a well-defined locus outlining the effects of undersampling (which can
be dramatic: an image measured at 2.0 pixels FWHM with no magnifier is
actually 1.05 pixels wide). We can use this relation to correct no magnifier
images to equivalent x2 images – but the better x2 images are significantly
undersampled too. We have extended the correction to the x2 data by assuming
the same effects affect the better images in the same way too, something
we will check and correct with the x5 magnifier now we know how serious
undersampling effects can be.
In the meantime, the provisional correction curve allows us to confidently
correct onto a fully sampled scale the larger images taken with no magnifier.
The smaller images are done so with some reservations, and the x2 images
similarly.
The figure displays a histogram of the results which will be kept updated
on the UKIRT web site (http://www.jach.hawaii.edu/UKIRT/telescope/seeing.html).
At the time of writing the overall data set (95 measurements) has a
median FWHM of around 0.52". This is in the K band and transforms to around
0.68" at V (0.55 microns).
We want to impress on our visiting observers our need for increasing
and improving the database of seeing statistics at UKIRT. These numbers
are the final validation of the things we do to make the telescope better:
without them we are in reality firing blind. In addition, they are tools
for the further investigation and understanding of the factors affecting
the ultimate performance of the telescope and such understanding is the
key to further development of this and many other telescopes.
In the meantime, please remember – GET THAT SEEING DATA ( please?).
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