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FIGURE 4.18 Measured return loss of the two-element dual-frequency microstrip array shown in Figure 4.17; r = 4.4, h = 1.6 mm, D = 50 mm, = 42 mm, S = 132.5 mm, and = 100 . (From Ref. 12, C 1999 IEE, reprinted with permission.)

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When you pick points to determine the hatch boundary, the hatching process uses the same mechanism as the BOUNDARY command to temporarily create a boundary for hatching. Check Retain Boundaries in the Boundary Retention section of the expanded dialog box if you want to draw the boundary as an object, and specify whether you want it to be a region or a polyline. Otherwise, the boundary is discarded when the hatch is placed. For more information, see the discussion of the BOUNDARY command earlier in this chapter. You can also specify a smaller boundary set than the objects that are visible on-screen. Use this when you re picking points and have such a complex drawing that the process of analyzing the visible objects takes a long time. To create a new boundary set, click the New button and specify a window in your drawing. You can hatch areas that are not completely closed using the Gap Tolerance feature. In the Tolerance text box, enter a value greater than the size of the gap. You can use values from 0 to 5000. In order to hatch an unclosed area in this way, you need to pick points rather than choose objects. When you do so, the Open Boundary Warning message opens. Click Yes to hatch the open boundary. Note that the hatch is not associative, which means that if you modify your almost closed area, you need to rehatch. Using this feature sets subsequent hatches as non-associative, so be sure to recheck the Associative check box in the main part of the dialog box. You can fine-tune how a hatch inherits properties, specifically the hatch s origin. Choose to use the current origin setting (from the left side of the dialog box) or use the setting of the source hatch.

Double Phase Conjugation Self-Starting Adaptive Gain-Grating Lasers Self-Adaptive Loop Resonators Using a Thermal Grating Hologram Experimental Characterization of a Thermal Grating 11.10.1 11.10.2 Time Dynamics and Diffraction Ef ciency Results Spatial Issues and Phase Conjugation Results

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FIGURE 12.57. Interferograms of an aspheric surface with three different defocusing values. The useful ring where the fringes can be processed has a larger contrast than the rest.

Table 12-5

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5.4.1. Some Reversal Shear Interferometers In this section, three different versions of a prism reversal shear interferometer are described. They are variations of a basic prism system invented by Kosters (1934), who pointed out that any combination of two exactly similar prisms can be used as an interferometer in the way he described, as long as one of the angles of the prism adjoining the common face is exactly half the angle that is opposite this common face. One of the two systems suggested by Gates (1955b), based on Kosters s prism, is illustrated in Figure 5.33; it uses two 30 -60 -90 prisms. The intersection of the plane de ned by the beam-splitting surface with the optical system de nes the axis of reversion. Lateral shear S is produced if the axis of reversion does not coincide with a diameter of the optical system under test. A tilting of the mirror under test provides a control of the separation of the interference fringes. A lens can be tested if an autocollimating at mirror is used behind the lens. The interferometer is compensated for use with white light because the optical paths are exactly equal. It is also compensated for the size of the light source, but in practice this size is limited to about 0.5 mm in diameter by small errors in construction, as pointed out by Gates.

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