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The analysis of the M92 photometry indicates that for point sources
with 13.5 aperture photometry provides measurements with
better internal consistency than psf-fit pphotometry. For fainter sources,
psf-fitting performs better. Consequently, optimum photometric measurements
should use aperture photometry for bright sources, and transition
smoothly to psf-fitting for fainter objects. This can be accomplished in
one of two ways:
- Measure both the aperture and psf-fit magnitudes, and intelligently
interpolate between the two. The interpolation would need to be calibrated
using measurements on additional large sets of multiply scanned regions
such as the M92 fields. This approach could be keyed to source density
and revert to pure psf-fitting in very crowded fields.
- Apply a weighting function to pixel values in a source to be
photometered that varies with source brightness. For bright sources,
the weighting function is a boxcar, so each pixel is given uniform
weight and the integrated brightness gives the same value as simple
aperture photometry.
For successively fainter sources, the weighting function gradually
"softens" to a more psf-like profile, until for faint sources it becomes
identically the psf. Again, the brightness dependence of the weighting
function would need to be calibrated using measurents on additional large
sets of multiply scanned regions.
Gaylin Laughlin
Wed Feb 22 09:42:23 PST 1995