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+### Statement
+
+$12.2.11.$ [Insert the problem statement]
+
+### Solution
+
+Data:
+
+· Parallel beam of monochromatic light of wavelength $\lambda$
+· Observation point A on the axis.
+· The plate has rings that coincide with the Fresnel zones.
+· It is considered that the plate covers the first m = 9 Fresnel zones.
+
+Reference amplitude (without plate):
+With the entire wavefront open, the amplitude at A is half of the first zone:
+
+$A_{\text{free}} \approx \frac{A_1}{2}$
+
+and the corresponding intensity is
+
+$ I_0 \propto \left(\frac{A_1}{2}\right)^2 = \frac{A_1^2}{4}$
+
+---
+
+Case (a): Opaque plate on even zones
+
+The plate has the even zones blackened out (blocked): 2, 4, 6, 8.
+The odd zones remain open: 1, 3, 5, 7, 9 (five zones).
+
+Since the amplitudes of the zones are $approximately equal (A_1 \approx A_3 \approx A_5 \approx A_7 \approx A_9)$, the total amplitude at A is:
+
+$A_a = 5 A_1$
+
+Intensity:
+
+$I_a \propto (5 A_1)^2 = 25 A_1^2$
+
+Compared with the intensity without the plate:
+
+$\frac{I_a}{I_0} = \frac{25 A_1^2}{A_1^2/4} = 25 \times 4 = 100$
+
+$\boxed{\text{The intensity increases by a factor of 100.}}$
+
+---
+
+Case (b): Phase plate (phase shift \pi) on even zones
+
+The rings that were previously opaque are replaced by dielectric layers that add a phase shift of \pi to the wave passing through.
+
+· The odd zones (1, 3, 5, 7, 9) pass with no phase change.
+· The even zones (2, 4, 6, 8) would normally arrive with a phase shift of $\pi $due to the path difference, but the layer adds another \pi, so they end up in phase with the odd ones.
+
+Now all zones (9 in total) contribute constructively:
+
+$A_b = 9 A_1$
+
+Intensity:
+
+$I_b \propto (9 A_1)^2 = 81 A_1^2$
+
+Compared with the intensity without the plate:
+
+$\frac{I_b}{I_0} = \frac{81 A_1^2}{A_1^2/4} = 81 \times 4 = 324$
+
+$\boxed{\text{The intensity increases by a factor of 324.}}$
+
+#### Answer
+
+[Insert a concise answer or boxed result]