Reduces a “Quadrant Jitter” observation without object masking
QUADRANT_JITTER_NO_MASK
It performs bad-pixel masking, null debiassing, dark subtraction, flat-field creation and division, feature detection and matching between object frames, and resampling. See the “Notes” for further information.
This recipe is suitable for faint objects or objects within a comparatively bright core embedded in faint extended emission, e.g. a quasar; or extended objects less than 45 arcseconds across with UFTI, 10 arcseconds with IRCAM, and 2 arcminutes with IRIS2. If there are other objects of comparable brightness to the principal target in other quadrants, they will introduce artifacts into the flat field. Use QUADRANT_JITTER for those.
A World Co-ordinate System (WCS) using the AIPS convention is created in the headers should no WCS already exist.
For IRCAM, old headers are reordered and structured with headings before groups of related keywords. The comments have units added or appear in a standard format. Four deprecated headers are removed. FITS-violating headers are corrected. Spurious instrument names are changed to IRCAM3.
The bad-pixel mask applied is $ORAC_DATA_CAL/bpm.
Each dark-subtracted frame has thresholds applied beyond which pixels are flagged as bad. The lower limit is 5 standard deviations below the mode, but constrained to the range 100 to 1. The upper limit is 1000 above the saturation limit for the detector in the mode used.
The flat field is created in two steps. The quadrant containing the object is masked in each object frame. Then the recipe combines the normalised and quadrant-masked object frames using the median at each pixel.
Registration is performed using common point sources in the overlap regions. If the recipe cannot identify sufficient common objects, it matches the centroid of the central source. If this fails, the script resorts to using the telescope offsets transformed to pixels.
The resampling applies non-integer shifts of origin using bilinear interpolation. There is no rotation to align the Cartesian axes with the cardinal directions.
The recipe makes the mosaics by applying offsets in intensity to give the most consistent result amongst the overlapping regions. The mosaic is not trimmed to the dimensions of a single frame. Thus the noise will be greater in the peripheral areas having received less exposure time. The full signal will be in the central ninth containing the main object. The mosaic is not normalised by its exposure time (that being the exposure time of a single frame).
For each cycle of four, the recipe creates a mosaic, which has its bad pixels filled and is then added into a master mosaic of improving signal to noise. The exposure time is also summed and stored in the mosaic’s corresponding header. Likewise the end airmass header and end UT headers are updated to match that of the last-observed frame contributing to the mosaic.
Intermediate frames are deleted except for the flat-fielded (_ff suffix) frames.
The integrated mosaic in mdate_group_number_mos, where m is the instrument’s group prefix.
A mosaic for each cycle of four in
mdate_group_number_moscycle_number,
where cycle_number
counts from 0.
The individual flat-fielded frames in idate_obs_number_ff, where i is the frame prefix. The naming format is slightly different for some non-UKIRT instruments.
The created flat fields in flat_filter_group_number for the first or only cycle, and flat_filter_group_number_ccycle_number for subsequent cycles.