Coherence — Question 2

Section 35-4 · Physics pages 5774–5775

Question 2 Random phase noise reduces contrast without changing the average intensity Two equal-intensity beams each contribute I0. Their instantaneous intensity is I = 2I0[1 + cos(δ + φ)]. The fluctuating phase has zero-mean Gaussian statistics with standard deviation σ, and ⟨eiφ⟩= e−σ2/2. The exposure samples the distribution fully. δ ⟨I⟩ averaged fringes Schematic; labels, not drawing lengths, specify the data. (a) Derive the time-averaged intensity and fringe visibility V = (Imax −Imin)/(Imax + Imin). (b) Find the largest phase standard deviation compatible with V ≥0.90.
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Question 2 - Solution Random phase noise reduces contrast without changing the average intensity δ ⟨I⟩ averaged fringes (a) Method and calculation ⟨cos(δ + φ)⟩= ℜ[eiδ⟨eiφ⟩] = e−σ2/2 cos δ. ⟨I⟩= 2I0[1 + e−σ2/2 cos δ], V = e−σ2/2 . (b) Interpretation and further calculation e−σ2/2 ≥0.90 =⇒σ2 ≤−2 ln 0.90. σmax = 0.45904 rad = 26.30◦. Physical check A uniform scan of the controlled phase still has mean intensity 2I0; noise reduces modulation rather than removing beam power.

Question 2

Random phase noise reduces contrast without changing the average intensity

Two equal-intensity beams each contribute I0I_0. Their instantaneous intensity is I=2I0[1+cos⁡(δ+φ)]I=2I_0[1+\cos(\delta+\varphi)]. The fluctuating phase has zero-mean Gaussian statistics with standard deviation σ\sigma, and ⟨eiφ⟩=e−σ2/2\langle e^{i\varphi}\rangle=e^{-\sigma^2/2}. The exposure samples the distribution fully.

Diagram shown in the original SVG worksheet.

  1. Derive the time-averaged intensity and fringe visibility V=(Imax−Imin)/(Imax+Imin)V=(I_{\max}-I_{\min})/(I_{\max}+I_{\min}).

  2. Find the largest phase standard deviation compatible with V≥0.90V\geq0.90.

Question 2 - Solution

Random phase noise reduces contrast without changing the average intensity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨cos⁡(δ+φ)⟩=ℜ[eiδ⟨eiφ⟩]=e−σ2/2cos⁡δ.\langle\cos(\delta+\varphi)\rangle=\Re[e^{i\delta}\langle e^{i\varphi}\rangle]=e^{-\sigma^2/2}\cos\delta.⟨I⟩=2I0[1+e−σ2/2cos⁡δ],V=e−σ2/2.\boxed{\langle I\rangle=2I_0[1+e^{-\sigma^2/2}\cos\delta],\quad V=e^{-\sigma^2/2}}.

(b) Interpretation and further calculation

e−σ2/2≥0.90⇒σ2≤−2ln⁡0.90.e^{-\sigma^2/2}\geq0.90\Longrightarrow\sigma^2\leq-2\ln0.90.σmax=0.45904rad=26.30∘.\boxed{\sigma_{\max}=0.45904\,\mathrm{rad}=26.30^\circ}.

Physical check

A uniform scan of the controlled phase still has mean intensity 2I02I_0; noise reduces modulation rather than removing beam power.