The virtual photons generated in this process were then allowed to interact with the CCD via the acis_sim program. Before we compare the simulated CCD output to the XRCF data, a useful aside is to compare the rays incident upon the CCD to the set of events generated by the interaction of those rays with the CCD. This illustrates the degradation of the PSF by convolving it with the quantized detector picture elements.
Figure 6.13 shows the SAOSAC rays
configured to match the geometry of the XRCF for test H-IAI-CR-1.001. In
order to facilitate comparison between the rays and the simulated CCD events,
Figure 6.14 and Figure 6.15
show the rays grouped into 1X1 pixel bins beside the CCD simulator output.
Because Al K
photons often produce single-pixel events, the simulated output very closely
resembles the binned rays. This is not to be expected at higher energies,
where split events are more prevalent. The ``lego'' plots (Figure 6.15)
better illustrate the PSF broadening due to pixelization.
Figure 6.13: The left-hand panel
shows a scatter plot of
the rays for test H-IAI-CR-1.001. The right-hand panel shows
the same
rayfile, displayed as a surface and binned arbitrarily at 0.2 pixels.
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Figure 6.14: The left-hand
panel shows an image of
the rays for test H-IAI-CR-1.001, grouped in 1X1 pixel bins.
The right-hand panel shows the simulated CCD events binned similarly.
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Figure 6.15: The left-hand panel shows a 2-dimensional histogram (``lego plot'') of the rays for test H-IAI-CR-1.001, grouped in 1X1 pixel bins. The right-hand panel shows the simulated CCD events binned similarly.
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