UIST Spectroscopy
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IFU: Preparing a Programme
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Preparing an Observing Programme: the UKIRT-OT
FIRST TIME USERS: Please read the General
Introduction to the OMP before reading the notes below (which are
specific only to the IFU). If after doing this these notes are still
as clear as mud, try the long-slit
spectroscopy page on programme preparation.
Your complete observing programme can be prepared either in Hilo or
before you arrive in Hawaii from your home institute (provided you
have access to the ukirt-ot). From any Unix or Linux box
in Hilo (or at the summit) type ukirtot to run-up the observing
tool (the OT).
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Alternatively, on KAUWA at UKIRT just click on this
icon on the tool-bar at the bottom of the screen. |
A small window will appear (containing a photo of UKIRT) in addition
to the copyright notice window; you may use the former to open
existing programmes, create new programmes or access the database. If
you're new to ORAC, close the copyright box and read on...
The UIST Template Library
The expectation is that most users will work from "Template
observations" (available
Template observations are described on a separate page - a table
of DR recipes is also available). The "Template Library" contains
observations that can be modified to suit your specific needs (see
Fig.1). It is probably unwise to try and write an observation
completely from scratch. Thus, with this in mind, open the Template
Library by selecting this option from the menu under "File" (top-left
corner of the small "UKIRT" window). At the same time, create a new
programme by selecting this option from the same (File) menu. After a
few moments, two Programme windows - like the one shown in Fig.1 -
will appear.
In the template library, click on the button to the left of the
"folder" icon labelled IFU templates. There you'll find the
available observations or "sequences" for IFU spectroscopy. Examine
those that may be of use to you by clicking on the button to the left
of the blue/pink icon; the component observations
should be displayed as a flow chart, as in the example below.
Like ordinary spectroscopy, an IFU observation should comprise a
flat, an arc and a sequence of "object" and "sky" exposures of a
standard star, followed by a similar sequence of object/sky frames on
the target itself. The example below contains all of these components.
Point sources should be "nodded" in and out of the IFU
field of view, unless the seeing is very good, in which case it
may be possible to nod the star between the top and the bottom
half of the elongated IFU field. Subtraction of the sky frames from
the object frames will remove OH line and thermal background
emissions, giving a series of spectra in adjacent slices in the
scrunched spectral image. An arc spectrum will be used by the DR to
accurately wavelength-calibrate the data, and a similarly-reduced
standard star spectrum can be used to divide out atmospheric
absorption bands and flux-calibrate the source spectra. The DR will then
"chop up" the scrunched spectral image and create a data cube (see the
ORAC-DR pages for full details).
For an extended source, nodding to blank sky is likewise
necessary. A larger nod (than the default in the template
observation) may be necessary.
Flexible Scheduling and Minimum Schedulable Blocks:
From semester 03A onwards all UKIRT observing will be
flexibly-scheduled. Consequently, observations must be grouped within
"Minimum schedulable blocks", or MSBs. An MSB represents the minimum
amount of data that needs to be obtained for an observation to be
useful. In the OT, an MSB is represented by a blue and pink cube.
You or indeed any other observer will then be equipped to
properly observe one or more of your targets, simply by executing
everything in the MSB. For IFU spectroscopy, an MSB usually includes
flat, arc, standard star and target observations.
Flats, arcs, standards...
In Fig.1 the "IFU, Nod to blank sky" MSB has been opened; it
contains a Calibration (flat and arc) observation , a Bright
(standard) star observation and a Science target
observation. UIST must be set up in exactly the same way for the flat
and arc as for the standard and target observations (i.e. same
position angle, grism, etc.). This is achieved by placing the UIST
component (the broken blue square labelled UIST in Fig.1) above
the three observations. The observations then "inherit" the UIST
component parameters; the slit width, position angle, grism, etc.
Only the exposure time is changed in each observation, as described
below. The flat and arc have default exposure times, set by clicking
"Use defaults" in the flat and arc observations.
The UIST instrument component and Target component are described
further below.
Fig.1 An IFU
Observation in the template library (click for a full-sized
image).
The components of an IFU observation
Each observation (the blue squares) needs three components (the
"broken" blue squares), which specify the Target information
(target and guide star coordinates), the UIST instrument
configuration and the Data Reduction Recipe (DRRecipe). These
can be contained "within" each observation, or they can be
"inherited". In Fig.1, for example, all three observations inherit
the UIST configuration from the component above them. The flat/arc
and standard star observations also inherit the standard star
coordinates (so that the flat and arc are observed at the location of
the standard). The science target observation contains its own
coordinate information, which overrides the inherited standard star
information (see Fig.2 below, where the target is called HH2). The
data reduction recipes, to be used to reduce the calibration, standard
and science target data, are then specified individually inside each
observation (see e.g. Fig.2).
- The Target information component is used to enter the
standard star or science target coordinates. It may also be used to
display a Digitised Sky Survey image of the target field, the
instrument aperture size, and various guide-star catalogues (see this
ORAC-OMP
Guide for a comprehensive description of this tool).
The UIST instrument component is used to select grism,
exposure time, position angle, etc. Here the IFU mode is also
selected. In Fig.2 the UIST component is highlighted, so that the UIST
configuration is displayed on the right half of the window: in this
case, UIST has been set for HK IFU spectroscopy with the IFU's major
(6-arcsecond long) axis orientated east-west. One 7sec exposure -
appropriate for the standard star - will be taken with the default
NDSTARE 1024x1024 readout area.
The DRRecipe component allows you to select the recipe
appropriate to the mode of observation, so that the DR can reduce your
data on-line. An observation copied from the template library should
already have the DR recipe set correctly, so these shouldn't need
changing. All object files obtained as part of this observation will
be flagged with this recipe.
Fig.2 An IFU
MSB showing the components of the science target observation.
Below the DRRecipe component in Fig.2 there is a "running man" icon or
"iterator" labelled Sequence. Embedded "within" this Sequence
iterator is the Imaging Acquisition observation, five optional short
darks (used to flush the array after acquisition), then a
UIST IFU/Spec iterator, a Repeat iterator and the actual
Offset iterators (more running-man symbols) which nod the
telescope between the object and sky positions. The "eye" symbols are
the actual exposures at each position. IMPORTANT: the observes (the
eye symbols) must be labelled as "Observe" and "Sky" (as they are in
the above example, and in the template library) for the IFU DR to work
properly.
After source acquisition and array "flushing" (both discussed below),
the UIST Spec/IFU iterator changes the exposure time.
This iterator is needed because the UIST component, inherited by the
observation of HH2, is set up for 7sec exposures on the standard.
Longer exposures will probably be needed on the science target. (By
selecting a source magnitude, a sensible exposure time will be set.)
The iterators below "UIST IFU/Spec" are then stacked much like
"embedded do-loops" in a computer programme. With the setup in Figs.2
an object-sky-sky-object "quad", defined by the offset
iterators, will be repeated five times (specified by the repeat
iterator) to build up signal-to-noise on HH2. The offsets are set in
the offset iterators by "p" and "q" parameters, q being along the long
(6") axis of the IFU, with p being perpendicular to it, regardless of
the IFU position angle.
The standard star observation will be essentially the same as that
shown above, except that the "UIST IFU/Spec" iterator is not needed,
because the exposure time has already been defined in the UIST
component (broken square) higher up. Also, fewer repeats may be
required.
Finally, to view the whole sequence of observations (telescope moves
and filter changes) written as a simple text list click on the
Sequence "running-man" icon and hit "show".
IMPORTANT: If you change the wavelength
(or anything for that matter) in the UIST component, you must click on
"Use default" in the FLAT, ARC and the flush-array DARK. This
ensures that these observations pick up the changes made in the UIST
component. Remember, though, to set the flush-array dark exposure time
back to 1 or a few seconds (and 1 co-add) - you don't want to be taking
lengthy darks to flush the array.
Imaging acquisition
For both the bright standard and faint science target the source
will be "acquired", or centred in the 3.3"x6.0" IFU field-of-view, in
imaging acquisition mode. The TSS will do this for you. However, the
standard and science target observations must include the "Spec/IFU
Target Acquisition" eyeball (Fig.2) for this to be possible.
Exposure times for acquisition: By clicking on the
acquisition "eyeball" in the OT, you can enter either 9-10th mag for
the standard star or a higher magnitude for a fainter science target.
An appropriate exposure time and number of coadds will then be
automatically set. For the bright standard the shortest possible
exposure time must be used (9-10th gives the minimum 1sec full-array
readout). For a faint science target a total of 10 or 20secs may be
needed. Source acquisition is discussed further in the
long-slit spectroscopy pages. Beware of latency, however (see
below) - on faint targets use short exposure times and a few coadds
(e.g. 4 x 5sec for the HK grism) rather than one long exposure (1 x
20sec).
Image Latency
UIST suffers from image latency, i.e. residual signal (like dark
current) at the less than 1% level. Because imaging acquisition
involves taking images, often with longish exposures through a very
broad spectral blocking filter, this can leave some residual sky
signal on subsequent frames. Likewise, if a bright star is observed
in acquisition, there may be a residual (weak) image of the star in
the next frame or two. This latent signal gets weaker with time, and
it should "subtract off" when skies are subtracted from object frames.
The problem can (to some extent) be avoided by using short
exposures and a few coadds for imaging acquisition, rather than
one long exposure. The penalty is readout overheads, specifically 1-2
seconds per coadd. We recommend using three or four 5sec exposures
for faint targets (one 1sec exposure for a bright target). However,
even with these short exposures, residual signal from imaging
acquisition could still introduce additional noise to the first few
frames taken directly after imaging acquisition. Consequently, it may
be a good idea to "flush" the array, by taking a few short darks after
imaging acquisition, and before taking a first long (perhaps two or
three-hundred second) spectrum of the science target. The optional
flush darks are avaiulable for this purpose; they are potentially
useful for very faint targets and/or long spectroscopy exposure times
and/or short wavelengths, although their usefulness is limited - the
residual signal fades with time, not the number of read-outs.
Exposure times
Generally, the "longest possible" exposure time will give the best
performance. Background-limited performance with most of the UIST
grisms requires long exposure times. With the HK grism this is a few
minutes in the K-band and 5-10 minutes in the H-band; with the
short-K grism 5-10 minutes is also required (depending on wavelength
and whether an emission line coincides with a sky line or not).
Note, however, that OH sky-line intensities will vary on these time
scales, so the importance of perfect sky subtraction may limit the
exposure time you can use (as well as saturation on the source, of
course). For recommendations on exposure times please have a look at
the section on
preparing observations for UIST spectroscopy.
Saving and Storing your handy-work...
When preparing MSBs, keep saving the file to disk: click on
"File - Save As" at the top-left corner of the programme
window. Once the programme is complete, save it to disk one last
time. You may then store it to the telescope site (Database - store
to telescope site), using your project ID (e.g. u/03a/99) and password
(received through email). The programme can later be retrieved from
the database at the summit and your observation executed.
HOT TIP: Set up one MSB - for just one
flat/arc, standard and science target, say - then send this to your
Support Scientist. He or she will check it over. In most cases, you
can then simply copy this MSB "n" times and just change the coordinates of
the standards and science targets.
The above discussion and example is of course meant only as a brief
guide. A more comprehensive guide to the OMP, the OT and flexible
scheduling in general is avaliable here. A
UKIRT Support Scientist is assigned to each project (Visitor or
Queue-scheduled) to assist with the preparation of OT observations.
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