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69-cm-diameter off-axis segment whose center lies 81 cm from the axis of symmetry of the parent aspheric surface. The null optics was a Maksutov sphere (as illustrated in Figure 12.55), which reduces the departure and slope of the aspheric wavefront from 910 to 45 waves and from 3000 to 70 waves per radius, respectively. A hologram was then used to remove the remaining asphericity. Figure 12.55(a) shows interferograms obtained using the CGH-Maksutov test of the mirror under test. Figure 12.55(b) shows the results when the same test was performed using a rather expensive refractive null lens. When allowance is made for the fact that the interferogram obtained with the null lens has much more distortion than the CGH-Maksutov interferogram, and for the difference in sensitivity (l 632:8 nm for the null lens test and 514.5 nm for the CGH-Maksutov test), the results for the two tests are seen to be very similar. The hills and valleys on the mirror surface appear the same for both tests, as expected. The peak-to-peak surface error measured using the null lens was 0.46 waves (l 632:8 nm), while for the CGH-Maksutov test it was 0.39 waves (514.5 nm). The rms surface error measured was 0.06 waves (632.8 nm) for the null lens, while the CGH-Maksutov test gave 0.07 waves (l 514:5 nm). These results certainly demonstrate that expensive null optics can be replaced by a combination of relatively inexpensive null optics and a CGH. winforms upc-a reader Packages matching Tags:"UPC-A" - NuGet Gallery
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