Notes for the support astronomer
  
Before an OSCA night
 
-  With OSCA in the beam, and a well sized mask (say the 1.0"),
     take a dome flat
 -  Identify the mask center and calculate the offset from the standard
     aquisition position (pinhole) 
 
 -  Start the simplex tool on INGRID and locate the quadrant with the mask
 -  It should not be necessary to run a dedicated simplex for OSCA;
     it is definitely not recommended to simplex with the Lyot stop in
     the beam, since this will mask of large parts of the pupil.
 -  Check from pinhole images with/without OSCA that 
     abberations are small (eg, compare strehl values and faint structures in 
     these images); be aware that OSCA mirrors the images. You need to use
     the naomi-clr pupil stop to mask of unwanted light. OSCA images
     of the pinhole with no pupil stop will appear elongated
 -  Check the pupil image to determine the OSCA Lyot stop offset angle:
-  With the telescope primary mirror covers open, looking at the
     illuminated dome, and with the INGRID pupil imager into the beam;
     check the alignment of the OSCA Lyot stop relative to the M2 vanes.
     If the vanes are not completely
     covered, adjust the Lyot stop Offset angle until you have redetermined
     the optimum offset angle. Note that this requires the TCS to be active,
     in order to get updates of the rotation angle, and that the Lyot Stop
     Enabled button and the TCS-Lyot Update button are pressed
 -  Check also that the central obscuration of the Lyot stop is centered
     over the central four segments of the DM. To judge what segments
     are the central ones, use TopGui to tweak the tilt of one segment
     next to the central four until its edges becomes obvious
 -  The images may appear double, with one image offset slightly to the
     left on the RTD display. This is due to light bypassing the small
     OSCA mirrors, so that you actually see part of the direct pupil
     on top of the OSCA pupil. Placing a piece of paper between the two
     OSCA flat mirrors will remove the ghost image
 -  An even sharper pupil image can be obtained by going on a very bright
     (V=2-3) star in pupil imaging mode
  
 -  Check also that the INGRID pupil-stops match up with the Lyot stop
     and primary mirror. 
  
Nighttime observing
 
-  Aquire the star on the WFS as normal with OSCA out of the beam
 -  Move OSCA into the beam and select a mask
 -  Start the simplex tool, using continous display
 -  The distance between the acquisition and mask position is usually 
     only a few arcsec, therefore select a window size in the simplex 
     gui which covers both positions (using the above offsets)
 -  The TO can then move the star close or even onto the mask
 -  Move the WFS pickoff probe via TopGui accordingly until the 
     star appears again on the WFS (or just use the previously computed offsets 
     and center the star on the WFS via telescope movements)
 -  Close the AO loop
 -  To center the star precisely behind the mask, move the WFS pickoff probe
     in small steps (about 0.1 arcsec) until the star appears to be centered.
 -  If the seeing is less than perfect, or if your target is relatively
     faint, it can be difficult to judge when the star is well centered
     behind the mask.  To check the final alignment, it can be useful to
     take a longer exposure either on the simplex tool or with the observing
     system. Check that the halo around the mask is
     symmetrical around the mask and that (if visible) the core of the star
     light is in the center of the mask
 -  Remember to take the Simplex tool of Continuos Display before taking
     frames on the observing system
  
Changing the sky PA (rotational dithers)
 
-  Keep the AO loop closed while the TO changes the PA. Since this is
     a slow process (several minutes), the AO and AutoGuider should
     keep the star centered on the WFS if the WFS integration time is
     at its minimum. This will work well for small dithers, but if the
     dithers are in steps of more than 20-30 degrees it can fail
     If it fails, open the loop, let the TO move the star back, usually
     only about 2-3" and close again
 -  Due to the difference in atmospheric dispersion between the optical
     light on the WFS and the IR light on INGRID, the star will now
     have moved off the OSCA mask center. (Unless you are observing at very
     low airmass.) Use the pick-off probe (see above) to center it under
     the mask again
 -  For the moment only this manual centering of the star behind the mask is
     possible.  An automated centering might be implemented in the future.
     Some requirements for such an automated procedure can be found
     here
  
Which pupil to use
 
- For observations in K band the NAOMI-Obs pupil stop inside INGRID is the
    preferred one
 - The central obscuration of OSCA-Obs does not fully cover the central four
    segments
 - For short wavelengths use OSCA-Clr when the Lyot stop is being used.
 - For faint targets, the throughput can be doubled by removing the Lyot
    stop. In this case, use the NAOMI-Clr pupil stop, not the OSCA-Clr
 - Note that the OSCA-Clr/Obs pupils are heavely undersizing the primary
    (corresponding to useing a ~3.5m telescope).
    From simulations this should improve the suppression.
    It depends on the particular science case which is the preferred pupil
    choice, but usually the NAOMI-Obs/Clr pupils can be used for all standard
    observations
  
Calibration frames
 
-  As with any INGRID run, make sure you have darks for all exposure
     times used.
 -  Flat-field images should preferably be obtained for all OSCA masks
     and filter combinations used. If you only obtain OSCA flats with
     the clear mask, you will account for flat-field errors (dust
     etc.) from the optical surfaces except the coronographic mask itself.
     But keep in mind that the clear mask may have dust on it as well,
     that is not on the hard masks!
 -  The Lyot stop is in the pupil plane and has no optical surfaces,
     and should not have any effect on the flat-field (except that it
     steals about 50% of the light).
  
 
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