Coherence — Question 4

Section 35-4 · Physics pages 5778–5779

Question 4 A Gaussian spectrum predicts a Gaussian visibility envelope For a stationary source, the normalized temporal coherence is g(τ) = ∫S(ν)ei2πντdν/ ∫S(ν)dν. Its spectrum is Gaussian about ν0 with standard deviation σν. Use the Gaussian-transform identity to obtain g(τ) = ei2πν0τe−2π2σ2 ντ 2. Equal beams have V = |g|. |au| V 1/2 Schematic; labels, not drawing lengths, specify the data. (a) Derive the positive delay at which visibility falls to one half. (b) For σν = 1.0 GHz, calculate that delay and the corresponding vacuum optical path difference with c = 3.00 × 108 m/s.
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Question 4 - Solution A Gaussian spectrum predicts a Gaussian visibility envelope |au| V 1/2 (a) Method and calculation V (τ) = e−2π2σ2 ντ 2, V (τ1/2) = 1/2. τ1/2 = √ 2 ln 2 2πσν . (b) Interpretation and further calculation τ1/2 = 0.18739 ns . D1/2 = cτ1/2 = 5.6217 cm . Physical check The quoted bandwidth is a standard deviation, not a full width at half maximum; mixing those conventions would change the numerical coherence scale.

Question 4

A Gaussian spectrum predicts a Gaussian visibility envelope

For a stationary source, the normalized temporal coherence is g(τ)=∫S(ν)ei2πντdν/∫S(ν)dνg(\tau)=\int S(\nu)e^{i2\pi\nu\tau}d\nu/\int S(\nu)d\nu. Its spectrum is Gaussian about ν0\nu_0 with standard deviation σν\sigma_\nu. Use the Gaussian-transform identity to obtain g(τ)=ei2πν0τe−2π2σν2τ2g(\tau)=e^{i2\pi\nu_0\tau}e^{-2\pi^2\sigma_\nu^2\tau^2}. Equal beams have V=|g|V=|g|.

Diagram shown in the original SVG worksheet.

  1. Derive the positive delay at which visibility falls to one half.

  2. For σν=1.0GHz\sigma_\nu=1.0\,\mathrm{GHz}, calculate that delay and the corresponding vacuum optical path difference with c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s}.

Question 4 - Solution

A Gaussian spectrum predicts a Gaussian visibility envelope

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(τ)=e−2π2σν2τ2,V(τ1/2)=1/2.V(\tau)=e^{-2\pi^2\sigma_\nu^2\tau^2},\quad V(\tau_{1/2})=1/2.τ1/2=2ln⁡22πσν.\boxed{\tau_{1/2}=\frac{\sqrt{2\ln2}}{2\pi\sigma_\nu}}.

(b) Interpretation and further calculation

τ1/2=0.18739ns.\boxed{\tau_{1/2}=0.18739\,\mathrm{ns}}.D1/2=cτ1/2=5.6217cm.\boxed{D_{1/2}=c\tau_{1/2}=5.6217\,\mathrm{cm}}.

Physical check

The quoted bandwidth is a standard deviation, not a full width at half maximum; mixing those conventions would change the numerical coherence scale.