Lasers and Laser Light — Question 6

Section 40-10 · Physics pages 6762–6763

Question 6 Two phase-stable laser frequencies produce a measurable beat signal Two collinear, equally polarized optical fields have intensities I1 = I2 = I0 and frequencies ν1 and ν2 = ν1 + 80.0 MHz. Their relative phase is stable. The detector averages over optical cycles but resolves the frequency difference. t I Schematic; labels, not drawing lengths, specify the data. (a) Derive the time-dependent intensity. (b) Find the beat period and the time-averaged intensity if the electronics also average over many beat cycles.
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Question 6 - Solution Two phase-stable laser frequencies produce a measurable beat signal t I (a) Method and calculation E = Ea cos(2πν1t) + Ea cos(2πν2t + ϕ). I(t) = 2I0[1 + cos(2π∆νt + ϕ)] . (b) Interpretation and further calculation Tb = 1/∆ν = 12.50 ns . ⟨cos(2π∆νt + ϕ)⟩= 0 ⇒¯I = 2I0 . Physical check The intensity can momentarily reach four times one-beam intensity, while its beat-cycle average is the sum of the two beam intensities. Limited detector bandwidth can hide the beat.

Question 6

Two phase-stable laser frequencies produce a measurable beat signal

Two collinear, equally polarized optical fields have intensities I1=I2=I0I_1=I_2=I_0 and frequencies ν1\nu_1 and ν2=ν1+80.0MHz\nu_2=\nu_1+80.0\,\mathrm{MHz}. Their relative phase is stable. The detector averages over optical cycles but resolves the frequency difference.

Diagram shown in the original SVG worksheet.

  1. Derive the time-dependent intensity.

  2. Find the beat period and the time-averaged intensity if the electronics also average over many beat cycles.

Question 6 - Solution

Two phase-stable laser frequencies produce a measurable beat signal

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E=Eacos⁡(2πν1t)+Eacos⁡(2πν2t+ϕ).E=E_a\cos(2\pi\nu_1t)+E_a\cos(2\pi\nu_2t+\phi).I(t)=2I0[1+cos⁡(2πΔνt+ϕ)].\boxed{I(t)=2I_0[1+\cos(2\pi\Delta\nu t+\phi)]}.

(b) Interpretation and further calculation

Tb=1/Δν=12.50ns.\boxed{T_b=1/\Delta\nu=12.50\,\mathrm{ns}}.⟨cos⁡(2πΔνt+ϕ)⟩=0⇒I‾=2I0.\langle\cos(2\pi\Delta\nu t+\phi)\rangle=0\Rightarrow\boxed{\bar I=2I_0}.

Physical check

The intensity can momentarily reach four times one-beam intensity, while its beat-cycle average is the sum of the two beam intensities. Limited detector bandwidth can hide the beat.