Intensity in Single-Slit Diffraction, Qualitatively — Question 3

Section 36-3 · Physics pages 5896–5897

Question 3 A real aperture profile produces an even far-field intensity A real aperture amplitude A(u) may be asymmetric in u. Its Fourier amplitude is F(q) = ∫A(u)e−iqudu. There is no imposed complex phase profile. β/π I/Ic Schematic; labels, not drawing lengths, specify the data. (a) Relate F(−q) to F(q) and prove the symmetry of the intensity. (b) Explain why unequal illumination of the two slit edges alone cannot shift the centroid of a fully collected, integrable far-field intensity.
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Question 3 - Solution A real aperture profile produces an even far-field intensity β/π I/Ic (a) Method and calculation F(−q) = ∫ A(u)eiqudu = [∫ A(u)e−iqudu ]∗ . F(−q) = F(q)∗, I(−q) = I(q) . (b) Interpretation and further calculation ∫∞ −∞ qI(q)dq = 0 when the integral exists. ⟨q⟩= ∫qI(q)dq ∫I(q)dq = 0 . Physical check Amplitude asymmetry can fill minima and reshape lobes while preserving reflection symmetry in the far field.

Question 3

A real aperture profile produces an even far-field intensity

A real aperture amplitude A(u)A(u) may be asymmetric in u. Its Fourier amplitude is F(q)=∫A(u)e−iquduF(q)=\int A(u)e^{-iqu}du. There is no imposed complex phase profile.

Diagram shown in the original SVG worksheet.

  1. Relate F(−q)F(-q) to F(q)F(q) and prove the symmetry of the intensity.

  2. Explain why unequal illumination of the two slit edges alone cannot shift the centroid of a fully collected, integrable far-field intensity.

Question 3 - Solution

A real aperture profile produces an even far-field intensity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F(−q)=∫A(u)eiqudu=[∫A(u)e−iqudu]*.F(-q)=\int A(u)e^{iqu}du=\left[\int A(u)e^{-iqu}du\right]^*.F(−q)=F(q)*,I(−q)=I(q).\boxed{F(-q)=F(q)^*,\quad I(-q)=I(q)}.

(b) Interpretation and further calculation

∫−∞∞qI(q)dq=0when the integral exists.\int_{-\infty}^{\infty}qI(q)dq=0\quad\text{when the integral exists}.⟨q⟩=∫qI(q)dq∫I(q)dq=0.\boxed{\langle q\rangle=\frac{\int qI(q)dq}{\int I(q)dq}=0}.

Physical check

Amplitude asymmetry can fill minima and reshape lobes while preserving reflection symmetry in the far field.