Qualitatively all the tests produce the same pattern of spatial response nonuniformity across the focal plane. This is especially true for the 660 nm light source(s). There is no indication that the instrument response to light at 660 nm has changed in any way between April 1997 and May 1998. Because the spatial response features reproduce under all test scenarios (at least for 660 nm) the inference is that these features are not caused by nonuniformities of the light source. However, uncertainties in illumination pattern and intensity introduce a considerable error in determination of numeric result. ACIS memo PS-136 and PS-137 describe the Lincoln Lab test which is the source of the quantitative results.
Figure 4.118 shows the responsivity (in electrons per pixel per incident photon at 660 nm) measured during the ACIS instrument thermal vacuum test at MIT Lincoln Laboratories in April, 1997.
Figure 4.119 shows the spatial
variation in light sensitivity observed in various tests. The most noticeable
feature in this figure is a "leak" in the region between S0, S1 and I2
with an order of magnitude enhanced response. Also evident, especially
in the S array, are features clearly attributable to wrinkles in the blocking
filter. Another constant result is the relative insensitivity of I1 and
I3 relative to adjacent I0 and I2.
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