The Light-Emitting Diode (LED) — Question 3

Section 41-9 · Physics pages 6956–6957

Question 3 Competing lifetimes set the internal quantum efficiency An injected carrier population N recombines radiatively at rate N/τr and nonradiatively at rate N/τnr. Let τr = 20.0 ns and τnr = 30.0 ns. Every radiative event emits one photon. N N/τr: photons N/τnr: heat Schematic; labels, not drawing lengths, specify the data. (a) Derive and evaluate total lifetime and internal quantum efficiency. (b) If passivation doubles only τnr, find the new efficiency and total lifetime.
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Question 3 - Solution Competing lifetimes set the internal quantum efficiency N N/τr: photons N/τnr: heat (a) Method and calculation τ −1 = τ −1 r + τ −1 nr , τ = 12.0 ns . ηint = 1/τr 1/τr + 1/τnr = τnr τr + τnr = .600 . (b) Interpretation and further calculation ηint,new = 60/(20 + 60) = .750 . τnew = 20(60)/(20 + 60) = 15.0 ns . Physical check Suppressing nonradiative loss improves efficiency but lengthens the population decay time. The two rates add because they act on the same carrier population.

Question 3

Competing lifetimes set the internal quantum efficiency

An injected carrier population N recombines radiatively at rate N/τrN/\tau_r and nonradiatively at rate N/τnrN/\tau_{nr}. Let τr=20.0ns\tau_r=20.0\,\mathrm{ns} and τnr=30.0ns\tau_{nr}=30.0\,\mathrm{ns}. Every radiative event emits one photon.

Diagram shown in the original SVG worksheet.

  1. Derive and evaluate total lifetime and internal quantum efficiency.

  2. If passivation doubles only τnr\tau_{nr}, find the new efficiency and total lifetime.

Question 3 - Solution

Competing lifetimes set the internal quantum efficiency

Diagram shown in the original SVG worksheet.

(a) Method and calculation

τ−1=τr−1+τnr−1,τ=12.0ns.\boxed{\tau^{-1}=\tau_r^{-1}+\tau_{nr}^{-1},\quad\tau=12.0\,\mathrm{ns}}.ηint=1/τr1/τr+1/τnr=τnrτr+τnr=.600.\boxed{\eta_{\mathrm{int}}=\frac{1/\tau_r}{1/\tau_r+1/\tau_{nr}}=\frac{\tau_{nr}}{\tau_r+\tau_{nr}}=.600}.

(b) Interpretation and further calculation

ηint,new=60/(20+60)=.750.\boxed{\eta_{\mathrm{int,new}}=60/(20+60)=.750}.τnew=20(60)/(20+60)=15.0ns.\boxed{\tau_{\mathrm{new}}=20(60)/(20+60)=15.0\,\mathrm{ns}}.

Physical check

Suppressing nonradiative loss improves efficiency but lengthens the population decay time. The two rates add because they act on the same carrier population.