Coherence — Question 9

Section 35-4 · Physics pages 5788–5789

Question 9 A phase-diffusion model gives an exponential coherence envelope Assume the phase difference accumulated over delay τ is Gaussian with zero mean and variance 2D|τ|, where D = 2.0 × 108 s−1. Use ⟨eiX⟩= e−Var(X)/2 for zero-mean Gaussian X. Equal-intensity beams have visibility equal to the modulus of this average. |au| V e−D|τ| Schematic; labels, not drawing lengths, specify the data. (a) Derive the visibility and find the delay at which it equals e−1. (b) Calculate the maximum vacuum optical path difference allowed for V ≥0.80, using c = 3.00 × 108 m/s.
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Question 9 - Solution A phase-diffusion model gives an exponential coherence envelope |au| V e−D|τ| (a) Method and calculation V (τ) = exp[−(2D|τ|)/2] = e−D|τ| . Dτ1/e = 1 =⇒τ1/e = 5.00 ns . (b) Interpretation and further calculation e−D|τ| ≥0.80 =⇒|τ| ≤−ln(0.80)/D. |τ|max = 1.11572 ns, ∆Lmax = 0.334715 m . Physical check The visibility decay is exponential in delay even though each phase increment has a Gaussian distribution, because its variance grows linearly with delay.

Question 9

A phase-diffusion model gives an exponential coherence envelope

Assume the phase difference accumulated over delay τ\tau is Gaussian with zero mean and variance 2D|τ|2D|\tau|, where D=2.0×108s−1D=2.0\times10^8\,\mathrm{s^{-1}}. Use ⟨eiX⟩=e−Var⁡(X)/2\langle e^{iX}\rangle=e^{-\operatorname{Var}(X)/2} for zero-mean Gaussian X. Equal-intensity beams have visibility equal to the modulus of this average.

Diagram shown in the original SVG worksheet.

  1. Derive the visibility and find the delay at which it equals e−1e^{-1}.

  2. Calculate the maximum vacuum optical path difference allowed for V≥0.80V\geq0.80, using c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s}.

Question 9 - Solution

A phase-diffusion model gives an exponential coherence envelope

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(τ)=exp⁡[−(2D|τ|)/2]=e−D|τ|.V(\tau)=\exp[-(2D|\tau|)/2]=\boxed{e^{-D|\tau|}}.Dτ1/e=1⇒τ1/e=5.00ns.D\tau_{1/e}=1\Longrightarrow\boxed{\tau_{1/e}=5.00\,\mathrm{ns}}.

(b) Interpretation and further calculation

e−D|τ|≥0.80⇒|τ|≤−ln⁡(0.80)/D.e^{-D|\tau|}\geq0.80\Longrightarrow|\tau|\leq-\ln(0.80)/D.|τ|max=1.11572ns,Δℒmax=0.334715m.\boxed{|\tau|_{\max}=1.11572\,\mathrm{ns},\quad\Delta\mathcal L_{\max}=0.334715\,\mathrm m}.

Physical check

The visibility decay is exponential in delay even though each phase increment has a Gaussian distribution, because its variance grows linearly with delay.