How Lasers Work — Question 6

Section 40-11 · Physics pages 6782–6783

Question 6 Passive photon lifetime follows the logarithm of the round-trip retention A cavity has round-trip time tr = 2.00 ns. With gain switched off, each round trip retains fraction R = .90 of its intracavity energy. Define photon lifetime by U(t) = U0e−t/τc at successive round-trip times. gain medium output L Schematic; labels, not drawing lengths, specify the data. (a) Derive and calculate τc. (b) Find the time for the energy to fall to one percent and the approximate number of round trips.
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Question 6 - Solution Passive photon lifetime follows the logarithm of the round-trip retention gain medium output L (a) Method and calculation U(mtr) = U0Rm = U0em ln R = U0e−mtr/τc. τc = −tr/ ln R = 18.982 ns . (b) Interpretation and further calculation .01 = e−t/τc ⇒t = τc ln 100 = 87.42 ns . t/tr = 43.71 ; 44 complete round trips to fall below 1% . Physical check The continuous exponential matches the exact discrete decay at round-trip times. Replacing minus log R by one minus R is only a small-loss approximation.

Question 6

Passive photon lifetime follows the logarithm of the round-trip retention

A cavity has round-trip time tr=2.00nst_r=2.00\,\mathrm{ns}. With gain switched off, each round trip retains fraction ℛ=.90\mathcal R=.90 of its intracavity energy. Define photon lifetime by U(t)=U0e−t/τcU(t)=U_0e^{-t/\tau_c} at successive round-trip times.

Diagram shown in the original SVG worksheet.

  1. Derive and calculate τc\tau_c.

  2. Find the time for the energy to fall to one percent and the approximate number of round trips.

Question 6 - Solution

Passive photon lifetime follows the logarithm of the round-trip retention

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(mtr)=U0ℛm=U0emln⁡ℛ=U0e−mtr/τc.U(mt_r)=U_0\mathcal R^m=U_0e^{m\ln\mathcal R}=U_0e^{-mt_r/\tau_c}.τc=−tr/ln⁡ℛ=18.982ns.\boxed{\tau_c=-t_r/\ln\mathcal R=18.982\,\mathrm{ns}}.

(b) Interpretation and further calculation

.01=e−t/τc⇒t=τcln⁡100=87.42ns..01=e^{-t/\tau_c}\Rightarrow\boxed{t=\tau_c\ln100=87.42\,\mathrm{ns}}.t/tr=43.71;44 complete round trips to fall below 1%.\boxed{t/t_r=43.71};\qquad\boxed{44\text{ complete round trips to fall below }1\%}.

Physical check

The continuous exponential matches the exact discrete decay at round-trip times. Replacing minus log R by one minus R is only a small-loss approximation.