It performs a null debiassing, bad-pixel masking, dark subtraction, flat-field creation and division, amd integer shifts of pixel origin to register to fixed sky co-ordinates. See the “Notes” for further information.

The registration is adjusted to track the motion of the moving target using ephemeris data stored in file target_ephem.dat. See “Ephemeris-file Format” for details of this file’s format.

This recipe aims to keep pace with the pipeline’s incoming data. It works well for faint moving sources and in moderately crowded fields. It should not be used for frames where the telescope guided on the moving object. In that case reduction should be performed by JITTER_SELF_FLAT_TELE which registers using the telescope offsets alone.

• 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 by combining normalised object frames using the median at each pixel.

• Registration is performed using the telescope offsets transformed to pixels. Once the offsets are determined, they are adjusted for the motion of the target, so that the final mosaic registers the target, not the background stars.

• There is no resampling, merely integer shifts of origin.

• The ephemeris file is specified by environment variable ORAC_EPHEMERIS, defaulting to $ORAC_DATA_OUT/target_ephem.dat.

• 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 mosaic is not normalised by its exposure time (that being the exposure time of a single frame).

• For each cycle of jittered frames, the recipe creates a mosaic, which 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 objectname, which may contain embedded spaces; and

• the motion in the plane of the sky in arcsec/second for right ascension then declination.

Note that the right-ascension motion is the change in right ascension multiplied by the cosine of the declination. The format may change to include UT and possibly date.

• The integrated mosaic in $<$m$>$$<$date$>$_$<$group_number$>$_mos, where $<$m$>$ is the instrument’s group prefix.

• A mosaic for each cycle of jittered frames in
  $<$m$>$$<$date$>$_$<$group_number$>$_mos$<$cycle_number$>$, where $<$cycle_number$>$
  counts from 0.

• The individual flat-fielded frames in $<$i$>$$<$date$>$_$<$obs_number$>$_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$>$_c$<$cycle_number$>$ for subsequent cycles.

NUMBER = INTEGER

• The processing engines are from the Starlink packages: Ccdpack, Kappa, and Figaro.

• Uses the Starlink NDF format.

• History is recorded within the data files.

• The title of the data is propagated through intermediate files to the mosaic.

• Error propagation is controlled by the USEVAR parameter.