Fig. 11.10. Encircled energy fraction for perfect system (s = 0.33) with pointing error. The a is
the normaHzed rms Gaussian error. Results are calculated from Eq. (11.1.13).
With these examples it should be clear that the MTF approach is a powerful
technique, especially when errors other than figure errors are present. We
conclude our introduction to the MTF approach in Section 11.4 following a
discussion of the Hubble Space Telescope.
11.2.
HUBBLE SPACE TELESCOPE, PRELAUNCH EXPECTATIONS
NOTE: This section on the Hubble Space Telescope is essentially unchanged
from the version ...
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