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Most of these have a target component set to RA, Dec 0,0. You will need to disable observability to get them to come up. Skip the slew and the TSS will go to an appropriate star. The following notes describe the principles of the measurement.
SETUP THE DOME
TELESCOPE STARTUP INSTRUMENT tilt: 0 0 0 0 0 0 0 0 0 0 0 0 0 The routine is: take an exposure with dichroic at 0,0; move dichroic, when dichroic is settled, take another exposure. There is some hysteresis so move the dichroic from positive to negative values, or always go through (0,0) (no need to actually take repeat data at 0,0, just set the dichroic there). The command is e.g. for moving port, "poffset 0 -50". Set to minimum signal value e.g (0,-190), then cycle through tilt, e.g.: tilt: 0 -20 +20 0 +40 0 +100 -80 +70 -60 +100set to minimum signal value e.g (+15,-190), take another frame to check for low signal. KAUWA, ANALYSING THE DATA You can either analyse the data in the raw or reduced data
directory, via this sort of kappa command: for UFTI data: "stats clip=3 f20001216_00014.i1" for /raw oror use a Gaia ARD region and look at the mean. Plot the mean value against port or tilt offset and get a minimum by linear extrapolation from the outer points to center, or by fitting a parabola. The data will look something like: counts When you have got a final value for
port and tilt, record them in : http://wiki.jach.hawaii.edu/staff_wiki-bin/wiki/UKIRT_QA_night_Logs
Focus offset measurementsPlease log the results of focus measurements in http://wiki.jach.hawaii.edu/staff_wiki-bin/wiki/UKIRT_QA_night_Logs.
Send a note to Tom and Russell at the end of the night pointing to this
location. See http://www.jach.hawaii.edu/UKIRT/telescope/QAnight/FF.html
for the current and past focus values. MSB Names and LocationsThe MSBs you will need for these measurements are in U/EC/1. Titles are:
Most of these have a target component set to RA, Dec 0,0. You will
need to disable observability to get them to come up. Skip the slew and
the TSS will go to an appropriate star. The following sections describe
the details for each instrument/mode. UFTI
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1 |
Choose and point to an A or F-type star, near the zenith around 8th magnitude. This allows you to use an exposure time of around 20 seconds. |
| 2 |
Set up an observation that uses an E-W slit and the HK grism with 20 sec exposures. Probably best to use the 4-pix slit, since this is wide enough (hopefully) to minimise the effects of any minor seeing changes. The sequence in the programme doesn't matter since you will only be running movie. (Could just use the standard star observation as it is in the template library.) |
| 3 |
Load and run the observation, slewing to the standard star (or a near-cmc). Run the sequence to the imaging acquisition pause and start Movie. |
| 4 |
Set the Fast Guider mode to autofocus. The TSS now uses XOFFSET to move the guide telescope and put the four images produced by the Autofocus lens array in roughly the right place on the CCD for autofocus. The shift is roughly (9, -3) arcsec (is this still necessary??). |
| 5 |
Start Autofocus (this also does fast guiding). Centre/acquire the star for spectroscopy on the correct pixel in the usual way (with uist_pick?). Once the star is acquired, continue the sequence to the next break (just before you'd normally start observing). However, now run movie again so that the Movie-Gaia displays the star's continuum. |
| 6 |
On the Bottom End Controller screen set Fine Focus to -1.5. Allow autofocus to converge again after the change (this may take a little while after a big shift). [Note - the location is this: Bottom Eng Engineering screen -> other displays -> bottom end (1st column in this window).] |
| 7 |
When happy with the autofocus convergence, record the "signal" from the stellar continuum. To do this we suggest using "X-Y profiles" in the Movie-Gaia window. Drag out the box across the entire spectrum and watch the signal over several cycles of the display; write down the MAXIMUM VALUE you see. |
| 8 |
Change "Fine Focus" to +2.5 (yes - the opposite end of ff travel) and repeat steps 6 and 7. Note that re-acquisition of the star shouldn't be necessary after each FF change (since the star should still be down the slit). |
| 9 |
Take measurements at alternate +ve and -ve offsets about the nominal (which is around 0.8mm) to build up the coverage (alternate in this way to avoid any possibility of hysteresis). At each ff value, record the peak signal strength and enter this and the ff value into the excel spread sheet on the UKIRT PC. Measurements about 0.25mm apart should be ok - NOTE: ITS THE ff SETTINGS FARTHEST FROM FOCUS THAT LEAD TO THE BEST MEASUREMENT, NOT THOSE NEAR THE FOCUS WHERE CHANGES IN THE ff VALUE HAVE LITTLE EFFECT ON THE SIGNAL. |
Having plotted up the data, please then report the
FF value at peak signal into the wiki and email notification to Russell
and ukss.
IFU mode
Essentially repeat the steps for a normal spectroscopy focus run.
However, when faced with the multiple spectra in Movie, drag out the
XY-profiles box over all the bright/central spectra. Although moving
away from focus spreads light into adjacent spectra, it also spreads
light along the slit axis, so ALL the spectra in the IFU movie will
drop
in strength.
Finally, note that current ff values for all UIST modes are listed on
the UIST
engineering web pages.
The CGS4 protocol is as follows:
|
1 |
Choose and point to a star with K around 10, near the zenith. Use one of the brighter faint standards, for example. This allows you to use 10-20 second exposure times. |
|
2 |
In the CGS4 sms screen (TSS side), set CGS4 to 2.1 um, 1st order, 2x1 sampling (say; it's irrelevant), NDSTARE. Note that at 2.1 microns you won't include the thermal end of the K window, which can mask signal changes due to focus. The slit width can be 1 or 2 depending on seeing: Tom Kerr recommends 2 pixels since it doesn't make much apparent difference. |
|
3 |
Set the Fast Guider mode to autofocus. |
|
4 |
Start Autofocus (this also does fast guiding).
Peak up on a suitable CGS4 row using "Peakup" and 10-20 second
exposures. Record the mean of a series of peak counts. |
|
5 |
On the Bottom End Controller screen set Fine Focus to 1.0 below the nominal. Allow autofocus to converge again after the change. This may take a little while after the big shift. Note - the location is this: Bottom Eng Engineering screen -> other displays -> bottom end (1st column in this window). |
|
6 |
When happy with the autofocus convergence, again record the mean of a few readings on the movie display. |
|
7 |
Change "Fine Focus" to 1 greater than the
original value (yes - the opposite end; build the coverage up in
alternating fashion to avoid any possibility of hysteresis) and measure
the peak mean again. |
|
8 |
Continue filling in the steps until all have been covered. |
This whole process takes 15 or 20 minutes.
Run the FINE FOCUS CALCULATOR Spreadsheet by double-clicking it on the desktop of the summit PC (this is a shortcut to the actual sheet, which is stored in C:\UKIRT\Utilities).
Enter the mean values determined above against the fine focus setting. Unless you know what you're doing with EXCEL, don't try to expand the tables to allow for more focus positions; let me (AJA) know if this needs to be done.
The spreadsheet does a fit to the values you enter. If any value is missing, leave the corresponding entry empty in the table, and it will be ignored.
Copy the coefficients of x(squared) and x as
reported in the chart window into the box to its right (you can drag
the equation around if you need to). The sheet
calculates the best-fit focus position and reports it in the green box.
Please document this value in the "history" sheet, which you can get to
by clicking on its tab at the bottom of the excel window.
This should be measured at the end of every
night indicated on the ukirt schedule as "em". It is performed with the
echelle,
so
as to achieve the required resolution. Instructions are available on
the staff
wiki. Please be careful to move the dichroic to the CGS4 (north)
port before taking sky and dome data.
A few times a year we should observe the same
source with the HK grism, just to keep an eye on its transmission,
etc. So, if you have a spare ten minutes please run the "HK Grism
sensitivity check" MSB in the EC1 QA nite programme. Its set for just
the one target, g-129 (RA 03hrs, Dec +18) so it should only come up in
the QT if the target's available. The target is faint (10th-11th), so
imaging
acquisition on the target itself (rather than a nearcmc) should be
fine. Its set for just one quad, with 60sec exposures.
Protocol is as follows: TSS runs a two-row peakup for one and two pixel slits: Peakup is run twice, on two rows well spaced on the array - 140 and 200 for example.
If significantly nonzero angles are found (note - image rotator can set to accuracy of about 0.1 degree, and with the 2-pixel slit successive determinations can vary by 0.05 degree in good conditions):
TSS saves the slit position angle -
SAVE_PA <SLITNAME>where SLITNAME is something informative such as 1pixdec00. Inform Tom Kerr by email that the offset has changed; he will adjust the settings in the cgs4 config file.
Until the config has been changed, using the affected slit will require the offset to be recalled from the saved version, until the new values are made the default:
ADJUST_PA <SLITNAME>| Instrument |
MSB name in
U/EC/1 |
| CGS4 | CGS4 aperture/PA measurements |
| UFTI | UFTI (full and sub) apertures |
| UIST | ALL UIST aperture measurements (2 cameras) |
Most of these have a target component set to RA, Dec 0,0. You will need to disable observability to get them to come up. Skip the slew and the TSS will go to an appropriate star. The following sections describe the details for each instrument/mode.
Note: for the Imaging 0.12" and 0.06" apertures, use the full array and the same reference pixel (see the table in the above eng. web page).
There is a "UIST apertures" sequence in U/EC/1; load it, skip the
slew and go to a 9-10th mag A-
or F-type star. The sequence does 3-second exposures, which will be
enough for good centroiding on the star image. Stop at break and run
Movie. Then follow the steps outlined
below (under Camera Aperture Determinations) to centre the star on the
appropriate pixel on the array.
Apertures should be measured for the following (all but the latter
are done in the first Observation in the MSB)
Use the U/EC/1 MSB for CGS4 instrument aperture
measurement. If there is time to do more than J and K (which are the
important ones), then edit the wavelength and resubmit/query/fetch.
Also
if there is time to do several slit PAs, edit them as appropriate; a
range of 0, -15, -30, -60, -90, -120, -150 is useful to cover. Using
autopeak, each setting will take a few minutes.
The full list of required aperture measurements is given in the form
in a later section.
In the TCS command window:
1. Use the PORT command to position the dichroic for the instrument
2. Use the APER command to select the
correct instrument aperture (need to change this for each UIST mode)
3. Send the telescope to a CMC target (if necessary)
4. Use the COLLIM command to adjust the telescope pointing model
5. Turn on autoguiding
6. Click on the appropriate TCS Tab to
display Instrument Apertures
7. Use the AOFFSET and AZERO commands to
adjust the
instrument aperture values until the target is in the correct spot on
the array. For UIST see the UIST
engineering web pages for the most up-to-date values. For UFTI, see
above. Directions: for UIST,
AOFF 20,10 takes the star down 20 and right 10 on the gaia display. For
UFTI, AOFF 20,10 takes the star right 20 and down 10. There is a
spreadsheet which can help you to quickly get onto the pixel -
/home/observer/adamson/procs/APERTURECALC.ods (runs in open office).
8. The TCS status display will show the
instrument aperture values
(X and Y). Enter the numbers in the wiki: (http://wiki.jach.hawaii.edu/staff_wiki-bin/wiki/UKIRT_QA_night_Logs)
and email ukirt_ss and Russell so that the OT
configuration files and TSS values can be updated.
UFTI : the current measured APERTURE offsets between imaging and imaging pol is: +5.7,-32.5
If you do need to check the imaging to imaging-pol offset, then in EC1 there is an MSB containing two obs, one for the normal, full-array instrument aperture, and a second for the UFTI pol aperture. UFTI pol targets should ALWAYS be placed in the top-half of the array, so the difference between the two apertures should be about 30" (i.e. toff of 0,-30" should move a target from the imaging aperture to the pol aperture, so that the two images of the star [the e- and o-beams] will be well-positioned in the centre of the two upper pol windows).
NOTE: THIS SHOULD BE POSSIBLE WITHOUT INSTALLING THE WAVEPLATE OR
THE
POL MASK IN FRONT OF UFTI. JUST THE PRISM INSIDE UFTI WILL BE
USED. HOWEVER, THE MOVIE IMAGES MAY LOOK A BIT WIERD, I.E. YOU WON'T
SEE THE USUAL E- AND O-BEAM SEGMENTS.
Only do this if the dichroic has recently been changed and the vignetted region is therefore unknown.
The principle is to move the star image until it starts to 'split', then back off until you have a minimal or non-existent 'partner' image. Note: this is difficult for the E/W ports, as the acquisition mode on the guider creates a 'streak' off to the right, so some of the 'split' images will be buried somewhat in this. Also, when the star image goes into the guide box (but no companion split image) you are off the dichroic (because there is no longer any refraction due to the dichroic); move back towards the dichroic to find the area where the 'split' starts to occur.
Apply offsets as follows:
|
EAST and WEST ports |
TOFF X 0 |
|
NORTH and SOUTH ports |
TOFF 0 Y |
As an example - the vignetted regions as of January 2001 were:
|
East port |
-146.5 < X < -125.5 & 124 < X < 141.5 arcsec |
|
West port |
-134.5 < X < -117 & 132.5 < X < 153.5 arcsec |
|
North port |
-163 < Y < -141.5 & 108 < Y < 125 arcsec |
|
South port |
-150.5 < Y < -133.5 & 116 < Y < 137.5 arcsec |
The Fast Guider has two basic modes of
operation: Normal and Autofocus.
The two basic modes use different lenses,
located at a pupil plane inside the Fast Guider, to form an image on
the guider CCD. One is a single lens, forming a single star image on
the CCD for normal (fast) guiding. The second is a 2x2 lenselet array
which forms 4 star images on the CCD. (Normal Guiding has subsidiary
modes, "focus" and "acquisition" which are currently rarely used. These
differ from Fast Guiding mainly in the binning of the pixels from the
CCD and in the field of view which is read out.)
The optimum arrangement derived and employed for
Fast Guiding is to bin the native pixels of the CCD into 3x3
"superpixels" around 0."93 arcsec square: we then read out a 4x4 array
of the superpixels and use the signal on the central four and that on
the outer twelve to determine the location of the centroid of the
image.
In fast guiding the the secondary mirror
feedback loop tries to hold the centroid at the point defined by the
inner corners of the four central pixels, by tipping and tilting the
secondary mirror with its piexo actuators. In auto-focussing we use the
fact that the radial separation of the four images is a measure of the
telescope focus position, so by measuring this separation over a period
of time and comparing it with a nominal value a focus correction can be
derived which is then applied to the telescope secondary mirror Z
position. In principle this could be done as fast as the CCD is read
out; in practice the piezos do not have enough throw to correct for the
focus excursions actually seen, so the focus corrections are applied
via the hexapod, which is a lot slower (~Hz) than the tip-tilt system
(~10s of Hz).
We normally average the 60-Hz focus correction
measures for periods of 2, 4 8, 16 or 32 seconds. (In this process we
also determine the Root-Mean-Square (RMS) variation in the numerous
computed focus corrections which were combined to get the average; this
quantity ("Zrms") is a measure of the seeing.) The nominal value for
the
radial spacing of the images is actually just set by the CCD array
pixel
spacing: in autofocus mode we read out an 8x8 array of the same 3x3
superpixels used in fast guiding. This comprises four 4x4 "fast-guide"
type sub-arrays, one for each subimage. The reference spacing is then
just that of the four centrepoints of the central quartets of pixels,
and for each readout of the array we compute the displacement of the
centroids of the sub-images from the reference positions; its radial
component measures the current defocus (and the mean X-Y component
measures tip-tilt, just as in fast guiding, so that this process is
still available).
In autofocus mode the larger readout area slows the process somewhat: whereas in fast guiding we can read out at 100 Hz (or in fact a good deal faster), in autofocus mode the standard readout rate is 60 Hz. When in autofocus mode the guider systems determine focus corrections averaged over the chosen time and send these corrections to the hexapod, which moves the secondary in the Z direction in such a way as to bring the centres of the four subimages onto the four centrepoints of the four subarrays of superpixels.
Guider Fine Focus
The single and quadruple lenses are both carried in the same lens wheel, which can be moved towards and away from the CCD. This adjustment is called "Fine Focus" on the Botttom-End Control screens and is a measure of the lens wheel position (in mm) relative to an arbitrary zero. Each scientific instrument has a slightly different optimum telescope focus setting. But as we have seen the guider in autofocus mode can only correct the telescope focus to bring the images into coincidence with the reference points on the CCD.
However the radial spacing of the images on the CCD is a function of the overall focus of the telscope and guider system, including the lenslet array. Thus moving the lenslet array towards and away from the CCD also changes the spacing of the images. This enables us to use differnt telescope focus settings for the various instruments: we just select for each an optimum distance of the lenslet array from the CCD, i.e. an optimum setting for the guider "Fine Focus". These values are referred to as the Autoguider Fine Focus Offsets.
Note that the Fine Focus setting is different when in autoguider and Normal Guide mode as the lenses used have different focal lengths.
FOCUS QUALITY CRITERION
Selecting a variable to be measured to determine focus quality is non-trivial, but image central intensity in one form or another works well. Strehl ratio on UFTI/TUFTI images should be fine and at least nominally independent of transparency. In the case of CGS4 we use the signal in the selected row as displayed on the Movie screen. (This is not independent of transparency; a normalised signal (the ratio of the central row to the two adjacent rows, perhaps?) is possible but not currently available.)
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Date: |
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Recorded by: |
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Grating |
PA |
Instap x |
Instap y |
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40l/mm, 1st order |
0 |
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Mean FWHM for spreadsheet |
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0.6 |
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0.8 |
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1.0 |
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1.2 |
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1.4 |
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1.6 |
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1.8 |
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2.0 |
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2.2 |
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Best focus setting: |
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Date |
|
|
Recorded by |
|
| Star Location |
||
|---|---|---|
| Position Angle (deg) |
X
(pixels) |
Y (pixels) |
| -90 |
||
| -60 |
||
| -30 |
||
| 0 |
||
| 30 |
||
| 60 |
||
| 90 |
||
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Date |
|
|
Recorded by |
|
| +RA
offset (arcsec) |
-RA offset (arcsec) | +Dec offset (arcsec) | -Dec offset (arcsec) | |||||
|---|---|---|---|---|---|---|---|---|
| Port |
Inner edge |
Outer edge | Inner edge | Outer edge | Inner edge | Outer edge | Inner edge | Outer edge |
| North |
N/A |
N/A | N/A | N/A | ||||
| East |
N/A | N/A | N/A | N/A | ||||
| South |
N/A | N/A | N/A | N/A | ||||
| West |
N/A | N/A | N/A | N/A | ||||
|
Contact: Tom Kerr. Updated: Wed Aug 19 11:09:32 HST 2009 Return to top ^ |