Lasers and Laser Light — Question 10

Section 40-10 · Physics pages 6770–6771

Question 10 Two unequal pulse trains can share average power but differ greatly in peak power A laser emits Gaussian power pulses P(t) = Ppk exp[−4 ln 2 t2/∆t2] at repetition rate f, with negligible overlap. Use ∫∞ −∞e−at2dt = √ π/a. Let average power be 2.00 W, f = 80.0 MHz, and ∆t = 200 fs. t P Schematic; labels, not drawing lengths, specify the data. (a) Derive the pulse energy in terms of peak power and find the pulse energy numerically. (b) Find the peak power and how it changes if f is halved at fixed average power and pulse duration.
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Question 10 - Solution Two unequal pulse trains can share average power but differ greatly in peak power t P (a) Method and calculation U = Ppk∆t √ π 4 ln 2, ¯P = fU. U = ¯P/f = 25.0 nJ . (b) Interpretation and further calculation Ppk = U ∆t √ 4 ln 2 π = 1.174 × 105 W . Ppk ∝f−1 ⇒Ppk′ = 2Ppk . Physical check The Gaussian pulse-shape factor is retained; dividing energy by FWHM alone overestimates the peak. The pulse spacing is much longer than its duration, consistent with negligible overlap.

Question 10

Two unequal pulse trains can share average power but differ greatly in peak power

A laser emits Gaussian power pulses P(t)=Ppkexp⁡[−4ln⁡2t2/Δt2]P(t)=P_{\mathrm{pk}}\exp[-4\ln2\,t^2/\Delta t^2] at repetition rate f, with negligible overlap. Use ∫−∞∞e−at2dt=π/a\int_{-\infty}^{\infty}e^{-at^2}dt=\sqrt{\pi/a}. Let average power be 2.00 W, f=80.0MHzf=80.0\,\mathrm{MHz}, and Δt=200fs\Delta t=200\,\mathrm{fs}.

Diagram shown in the original SVG worksheet.

  1. Derive the pulse energy in terms of peak power and find the pulse energy numerically.

  2. Find the peak power and how it changes if f is halved at fixed average power and pulse duration.

Question 10 - Solution

Two unequal pulse trains can share average power but differ greatly in peak power

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=PpkΔtπ4ln⁡2,P‾=fU.U=P_{\mathrm{pk}}\Delta t\sqrt{\frac{\pi}{4\ln2}},\quad\bar P=fU.U=P‾/f=25.0nJ.\boxed{U=\bar P/f=25.0\,\mathrm{nJ}}.

(b) Interpretation and further calculation

Ppk=UΔt4ln⁡2π=1.174×105W.\boxed{P_{\mathrm{pk}}=\frac{U}{\Delta t}\sqrt{\frac{4\ln2}{\pi}}=1.174\times10^5\,\mathrm W}.Ppk∝f−1⇒Ppk′=2Ppk.P_{\mathrm{pk}}\propto f^{-1}\Rightarrow\boxed{P_{\mathrm{pk}}\prime=2P_{\mathrm{pk}}}.

Physical check

The Gaussian pulse-shape factor is retained; dividing energy by FWHM alone overestimates the peak. The pulse spacing is much longer than its duration, consistent with negligible overlap.