Semiconductors — Question 7

Section 41-5 · Physics pages 6884–6885

Question 7 Diffusion and recombination set a carrier penetration length For x greater than zero, steady excess holes satisfy Dp d2∆p/dx2 −∆p/τ = 0, with ∆p(0) = ps and ∆p(∞) = 0. Use Dp = .00100 m2/s and τ = 4.00 µs. x/Lp ∆p Schematic; labels, not drawing lengths, specify the data. (a) Solve the boundary-value problem and evaluate the diffusion length. (b) Find the injected hole diffusion current density at the boundary and the distance where the excess density falls to one tenth.
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Question 7 - Solution Diffusion and recombination set a carrier penetration length x/Lp ∆p (a) Method and calculation ∆p = Aex/Lp + Be−x/Lp, Lp = q Dpτ. ∆p = pse−x/Lp, Lp = 63.25 µm . (b) Interpretation and further calculation Jp(0) = −eDp d∆p dx 0 = eDpps/Lp . x10 = Lp ln 10 = 145.6 µm . Physical check The growing exponential is excluded by the far boundary condition. Integrating the recombination rate over depth reproduces the boundary particle flux.

Question 7

Diffusion and recombination set a carrier penetration length

For x greater than zero, steady excess holes satisfy Dpd2Δp/dx2−Δp/τ=0D_p\,d^2\Delta p/dx^2-\Delta p/\tau=0, with Δp(0)=ps\Delta p(0)=p_s and Δp(∞)=0\Delta p(\infty)=0. Use Dp=.00100m2/sD_p=.00100\,\mathrm{m^2/s} and τ=4.00μs\tau=4.00\,\mu\mathrm s.

Diagram shown in the original SVG worksheet.

  1. Solve the boundary-value problem and evaluate the diffusion length.

  2. Find the injected hole diffusion current density at the boundary and the distance where the excess density falls to one tenth.

Question 7 - Solution

Diffusion and recombination set a carrier penetration length

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δp=Aex/Lp+Be−x/Lp,Lp=Dpτ.\Delta p=Ae^{x/L_p}+Be^{-x/L_p},\qquad L_p=\sqrt{D_p\tau}.Δp=pse−x/Lp,Lp=63.25μm.\boxed{\Delta p=p_se^{-x/L_p},\quad L_p=63.25\,\mu\mathrm m}.

(b) Interpretation and further calculation

Jp(0)=−eDpdΔpdx|0=eDpps/Lp.\boxed{J_p(0)=-eD_p\left.\frac{d\Delta p}{dx}\right|_0=eD_pp_s/L_p}.x10=Lpln⁡10=145.6μm.\boxed{x_{10}=L_p\ln10=145.6\,\mu\mathrm m}.

Physical check

The growing exponential is excluded by the far boundary condition. Integrating the recombination rate over depth reproduces the boundary particle flux.