Intensity in Single-Slit Diffraction, Qualitatively — Question 9

Section 36-3 · Physics pages 5908–5909

Question 9 A common random phase does not wash out a diffraction pattern An entire coherent aperture acquires a spatially uniform random phase ϕ(t). Its instantaneous far-field amplitude is F(q, t) = eiϕ(t)F0(q). Compare this with two equal aperture patches whose relative phase is uniformly random during an exposure; each patch alone gives intensity Ip. common ϕ(t) Schematic; labels, not drawing lengths, specify the data. (a) Calculate the time-averaged intensity for the common-phase fluctuation. (b) Calculate the average intensity of the two independent-phase patches and compare with their fully in-phase value.
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Question 9 - Solution A common random phase does not wash out a diffraction pattern common ϕ(t) (a) Method and calculation I(q, t) ∝|eiϕ(t)F0(q)|2 = |F0(q)|2. ⟨I(q)⟩= I0(q) for arbitrary common phase noise. (b) Interpretation and further calculation I = 2Ip(1 + cos δ), ⟨cos δ⟩= 0 =⇒⟨I⟩= 2Ip . δ = 0 : Icoherent = 4Ip, ⟨I⟩/Icoherent = 1/2 . Physical check Diffraction depends on relative phase across the opening, so common phase noise and differential phase noise have different consequences.

Question 9

A common random phase does not wash out a diffraction pattern

An entire coherent aperture acquires a spatially uniform random phase ϕ(t)\phi(t). Its instantaneous far-field amplitude is F(q,t)=eiϕ(t)F0(q)F(q,t)=e^{i\phi(t)}F_0(q). Compare this with two equal aperture patches whose relative phase is uniformly random during an exposure; each patch alone gives intensity IpI_p.

Diagram shown in the original SVG worksheet.

  1. Calculate the time-averaged intensity for the common-phase fluctuation.

  2. Calculate the average intensity of the two independent-phase patches and compare with their fully in-phase value.

Question 9 - Solution

A common random phase does not wash out a diffraction pattern

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I(q,t)∝|eiϕ(t)F0(q)|2=|F0(q)|2.I(q,t)\propto|e^{i\phi(t)}F_0(q)|^2=|F_0(q)|^2.⟨I(q)⟩=I0(q)for arbitrary common phase noise.\boxed{\langle I(q)\rangle=I_0(q)}\quad\text{for arbitrary common phase noise}.

(b) Interpretation and further calculation

I=2Ip(1+cos⁡δ),⟨cos⁡δ⟩=0⇒⟨I⟩=2Ip.I=2I_p(1+\cos\delta),\quad\langle\cos\delta\rangle=0\Longrightarrow\boxed{\langle I\rangle=2I_p}.δ=0:Icoherent=4Ip,⟨I⟩/Icoherent=1/2.\delta=0:\quad\boxed{I_{\mathrm{coherent}}=4I_p,\quad\langle I\rangle/I_{\mathrm{coherent}}=1/2}.

Physical check

Diffraction depends on relative phase across the opening, so common phase noise and differential phase noise have different consequences.