Description:
Performs a self-correlation
calculation on an input NDF image file. The resulting correlation image/plot is stored to
disk.
The self-correlated image may be used to find flat-fielding faults and faint diffuse objects of a given
size.
To reduce the influence of bright objects or cosmic rays; the user may elect to employ a cut out pixel
count value where any pixel found to be above that value is ignored. The cutout value is determined
by the user inputting a global mode value (usually the sky background count - obtained via
HISTPEAK), the background count standard deviation and the number of standard deviations above
sky level at which the cutout should occur.
The user is required to enter a value for the size of object(s) of interest (roughly the template size) and
also the image pixel size.
The value for each pixel of the output image is determined as follows. An imaginary circle is drawn
about the pixel and all pixel pairs within that circle, that lie on opposite sides of the centre from each
other, are stored.
Each pair is then considered in turn and the modal count value subtracted from each. The resultant
residual pixel count values are then multiplied together. The values found for all the pairs are then
summed, the total divided by the number of pixel pairs found and the square root taken. In the event
of a negative sum being found the value given is the square root of the magnitude of the
self-correlation multiplied by -1.
The resultant value is some measure of the extent to which points within that circle (about the current
pixel) are correlated.
The method assumes some sort of symmetry is present in the objects detected but appears to work
well on a wide range of image types.
A border is present in the output image which the same width as the radius of the template. All pixels
within this border are assigned the value bad.
Usage:
SELFC IN OUT DIAM PSIZE BACK USEALL
[SIGMA] [NSIGMA]
Parameters:
BACK = _REAL (Read)
The modal pixel count value found in the
input NDF. Units counts.
DIAM = _REAL (Read)
The diameter of the galaxies to be searched for in
the image. Units arc seconds.
IN = _NDF (Read)
The name of the NDF data that is to be examined.
NSIGMA = _REAL(Read)
The number of standard deviations above the sky level count value, where
the pixel count cutoff occurs.
OUT = _NDF (Write)
The name of the NDF that will be created.
PSIZE = _REAL (Read)
The size of each pixel in arc seconds. If the image contains a
SKY co-ordinate frame this value will be determined automatically.
SIGMA = _REAL
(Read)
The standard deviation of the background count within the input NDF. Should
be determined using a routine such as HISTPEAK which ignores outliers.
USEALL =
_LOGICAL (Read)
Used to indicate whether a pixel count threshold is to be a applied when
calculating the self-correlation.
Examples:
selfc in=search out=scorr diam=15. psize=0.5
back=727.
useall=true
A self-correlation is carried out on image GALAXIES. The search is for an object 15
arc seconds across. The image pixel size is .5 arc seconds and the background count level is 727.
USEALL=TRUE ensures that no pixels are excluded from the correlation calculation. selfc in=plate
out=plates diam=5. back=6600.
useall=false sigma=35. nsigma=5.
A self-correlation is carried out on image PLATE. The search
is for an object 5 arc seconds across. The background count level is 6600 and the image
pixel size in arc seconds will be determined from a SKY coordinate frame in the image’s
WCS component if possible. Since USEALL=FALSE, all pixels with a count value above
660035.x5.
are excluded from the correlation calculation. The output image is named PLATES. Notes:
It is
assumed through out that the x and y axis pixels sizes are the same.
Implementation Status:
At
present suitable normalisation factors have not been implemented. These may be added. As the
program stands it is useful for looking at an image to detect faint objects and provides a
comparison for users employing cross-correlation techniques. In addition, it provides a simple
way of detecting areas of an image where flatfielding has not been entirely successful.