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Figure 12
Plots of the mean fringe contrast of computed moiré images versus the incident-wave angular width [\Delta {\Theta _{\rm inc}}]. Numerical conditions for the computation are as follows: curve (A) t1 = t2 = 0.8, tgap = 0.0, s2 = 0; (B) t1 = t2 = 0.8, tgap = 0.0; (C) t1 = t2 = 0.8, tgap = 0.02; (D) t1 = t2 = 0.8, tgap = 0.05; (E) t1 = t2 = 0.8, tgap = 0.2; (F) t1 = t2 = 0.8, tgap = 0.24; (G) t1 = t2 = 1.5, tgap = 0.24; (H) t1 = t2 = 2.5, tgap = 0.24; (I) t1 = t2 = 1.5, tgap = 0.0; (J) t1 = t2 = 2.5, tgap = 0.0. The curvature strength of the rear crystal was s2 = 0.045′′ mm−1 for all the curves from (B) to (J).

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