The Light-Emitting Diode (LED) — Question 6

Section 41-9 · Physics pages 6962–6963

Question 6 The ABC recombination model predicts an efficiency maximum In a supplied uniform LED model with equal electron and hole densities n, the total recombination rate per volume is R = An + Bn2 + Cn3. Only Bn2 is radiative. Assume constant positive coefficients. n/n∗ η Schematic; labels, not drawing lengths, specify the data. (a) Derive internal efficiency and the carrier density maximizing it. (b) For A = 107 s−1, B = 10−16 m3/s, and C = 10−41 m6/s, evaluate the optimum density and efficiency.
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Question 6 - Solution The ABC recombination model predicts an efficiency maximum n/n∗ η (a) Method and calculation η(n) = Bn2 An + Bn2 + Cn3 = Bn A + Bn + Cn2 . dη dn = B(A −Cn2) (A + Bn + Cn2)2 = 0 ⇒n∗= √ A/C . (b) Interpretation and further calculation n∗= 1024 m−3 . η(n∗) = B √ A/C 2A + B √ A/C = 108 1.2 × 108 = .8333 . Physical check At the optimum, the linear and cubic nonradiative rates are equal. The high-density decrease follows from the supplied cubic term; actual LED droop may involve additional mechanisms.

Question 6

The ABC recombination model predicts an efficiency maximum

In a supplied uniform LED model with equal electron and hole densities n, the total recombination rate per volume is R=An+Bn2+Cn3R=An+Bn^2+Cn^3. Only Bn2Bn^2 is radiative. Assume constant positive coefficients.

Diagram shown in the original SVG worksheet.

  1. Derive internal efficiency and the carrier density maximizing it.

  2. For A=107s−1A=10^7\,\mathrm{s^{-1}}, B=10−16m3/sB=10^{-16}\,\mathrm{m^3/s}, and C=10−41m6/sC=10^{-41}\,\mathrm{m^6/s}, evaluate the optimum density and efficiency.

Question 6 - Solution

The ABC recombination model predicts an efficiency maximum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

η(n)=Bn2An+Bn2+Cn3=BnA+Bn+Cn2.\boxed{\eta(n)=\frac{Bn^2}{An+Bn^2+Cn^3}=\frac{Bn}{A+Bn+Cn^2}}.dηdn=B(A−Cn2)(A+Bn+Cn2)2=0⇒n*=A/C.\frac{d\eta}{dn}=\frac{B(A-Cn^2)}{(A+Bn+Cn^2)^2}=0\Rightarrow\boxed{n_*=\sqrt{A/C}}.

(b) Interpretation and further calculation

n*=1024m−3.\boxed{n_*=10^{24}\,\mathrm{m^{-3}}}.η(n*)=BA/C2A+BA/C=1081.2×108=.8333.\boxed{\eta(n_*)=\frac{B\sqrt{A/C}}{2A+B\sqrt{A/C}}=\frac{10^8}{1.2\times10^8}=.8333}.

Physical check

At the optimum, the linear and cubic nonradiative rates are equal. The high-density decrease follows from the supplied cubic term; actual LED droop may involve additional mechanisms.