The Light-Emitting Diode (LED) — Question 1

Section 41-9 · Physics pages 6952–6953

Question 1 The recombination energy selects the LED wavelength In an ideal direct-gap LED, radiative recombination produces photons with energy approximately equal to Eg = 2.20 eV. Use hc = 1240 eV nm. The gap temperature coefficient near the operating point is dEg/dT = −4.00 × 10−4 eV/K. + − light Schematic; labels, not drawing lengths, specify the data. (a) Find the peak wavelength. (b) Derive the wavelength temperature coefficient and estimate the wavelength shift for a 20.0 K rise using linearization.
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Question 1 - Solution The recombination energy selects the LED wavelength + − light (a) Method and calculation Eγ = hc/λ ≃Eg ⇒λ = hc/Eg . λ = 1240/2.20 = 563.6 nm . (b) Interpretation and further calculation dλ dT = −hc E2g dEg dT = +.1025 nm/K . ∆λ ≃(dλ/dT)∆T = +2.05 nm . Physical check A decreasing gap shifts emission to longer wavelength. Carrier kinetic energies and spectral broadening can shift the actual peak from this band-edge estimate.

Question 1

The recombination energy selects the LED wavelength

In an ideal direct-gap LED, radiative recombination produces photons with energy approximately equal to Eg=2.20eVE_g=2.20\,\mathrm{eV}. Use hc=1240eVnmhc=1240\,\mathrm{eV\,nm}. The gap temperature coefficient near the operating point is dEg/dT=−4.00×10−4eV/KdE_g/dT=-4.00\times10^{-4}\,\mathrm{eV/K}.

Diagram shown in the original SVG worksheet.

  1. Find the peak wavelength.

  2. Derive the wavelength temperature coefficient and estimate the wavelength shift for a 20.0 K rise using linearization.

Question 1 - Solution

The recombination energy selects the LED wavelength

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Eγ=hc/λ≃Eg⇒λ=hc/Eg.E_\gamma=hc/\lambda\simeq E_g\Rightarrow\boxed{\lambda=hc/E_g}.λ=1240/2.20=563.6nm.\boxed{\lambda=1240/2.20=563.6\,\mathrm{nm}}.

(b) Interpretation and further calculation

dλdT=−hcEg2dEgdT=+.1025nm/K.\boxed{\frac{d\lambda}{dT}=-\frac{hc}{E_g^2}\frac{dE_g}{dT}=+.1025\,\mathrm{nm/K}}.Δλ≃(dλ/dT)ΔT=+2.05nm.\boxed{\Delta\lambda\simeq(d\lambda/dT)\Delta T=+2.05\,\mathrm{nm}}.

Physical check

A decreasing gap shifts emission to longer wavelength. Carrier kinetic energies and spectral broadening can shift the actual peak from this band-edge estimate.