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Having plotted up the data, please then report the
FF value at peak signal to Russell and ukss. CGS4The CGS4 protocol is as follows:
Data AnalysisBy HandPlot the means of each set of signal numbers vs the Fine Focus setting at which they were secured. Draw a smooth curve through the data points (smooth through ragged data points, don’t join them). Select three or four levels at which the data are reasonably well behaved (i.e. not too near the peak, where seeing has the biggest effect on signal level, not too near the background level) and determine the Fine Focus values corresponding LHS and RHS of the plotted curve; average these to find the centre. The different centre values should agree to 0.01 or 0.03 depending on how ragged the measures were. The mean is the new estimate for the CGS4 Autoguider Fine Focus setting. (One gets surprisingly similar results by just interpolating linearly between the data points to get the LHS and RHS values.)Using the Spreadsheet
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EAST and WEST ports |
TOFF X 0 |
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NORTH and SOUTH ports |
TOFF 0 Y |
As an example - the vignetted regions as of January 2001 were:
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East port |
-146.5 < X < -125.5 & 124 < X < 141.5 arcsec |
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West port |
-134.5 < X < -117 & 132.5 < X < 153.5 arcsec |
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North port |
-163 < Y < -141.5 & 108 < Y < 125 arcsec |
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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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Grating |
PA |
Instap x |
Instap y |
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40l/mm, 1st order |
0 |
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-60 |
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-90 |
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-120 |
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-150 |
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150l/mm, 2nd order |
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-120 |
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-150 |
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-60 |
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-120 |
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-150 |
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0 |
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40,1 pixel, 1.65um |
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40, 1pix, prism (use lower beam) |
0 |
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Signal Values |
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FF setting |
1 |
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4 |
5 |
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Mean |
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0.3 |
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0.5 |
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0.9 |
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1.3 |
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1.5 |
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1.7 |
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1.9 |
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Best focus setting: |
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Observers |
Offset (2pix) |
Offset (1pix) |
Saved as |
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Date |
Observers |
Aperture (band, x,y) |
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20001227 |
AJA,TW |
K, 4.05,11.64 |
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20001228 |
AJA,TW |
K, 4.18,11.67 K plus pol 4.18, 15.32 (righthand slot) |
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FF setting |
FWHM |
FWHM |
FWHM |
FWHM |
Mean FWHM for spreadsheet |
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0.2 |
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0.4 |
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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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Recorded by |
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FF setting |
FWHM |
FWHM |
FWHM |
FWHM |
Mean FWHM for spreadsheet |
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0.2 |
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0.4 |
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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 |
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Recorded by |
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| Star Location |
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| Position Angle (deg) |
X
(pixels) |
Y (pixels) |
| -90 |
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| -60 |
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| -30 |
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| 30 |
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| 60 |
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| 90 |
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Date |
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Recorded by |
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| +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 | ||||
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Contact: Tom Kerr. Updated: Tue Dec 11 21:21:49 HST 2007 Return to top ^ |