The p-n Junction — Question 3

Section 41-7 · Physics pages 6916–6917

Question 3 Poisson integration gives the triangular electric field An abrupt junction has depletion charges −eNA for −xp < x < 0 and +eND for 0 < x < xn, uniform permittivity ε, and zero field at both outer depletion edges. x E −xp xn Schematic; labels, not drawing lengths, specify the data. (a) Integrate dE/dx = ρ/ε to find the signed field on each side. (b) Find the potential rise Vj = ϕ(xn) −ϕ(−xp) in terms of peak field magnitude and W, then in terms of doping and widths.
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Question 3 - Solution Poisson integration gives the triangular electric field x E −xp xn (a) Method and calculation Ep(x) = −eNA ε (x + xp), En(x) = eND ε (x −xn) . Emax = |E(0)| = eNAxp/ε = eNDxn/ε . (b) Interpretation and further calculation Vj = − ∫xn −xp E dx = 1 2Emax(xp + xn) = 1 2EmaxW . Vj = e 2ε(NAx2 p + NDx2 n) . Physical check The field points from the positive donor ions on the n side toward negative acceptor ions on the p side. Its negative area gives a positive potential rise toward n.

Question 3

Poisson integration gives the triangular electric field

An abrupt junction has depletion charges −eNA-eN_A for −xp<x<0-x_p<x<0 and +eND+eN_D for 0<x<xn0<x<x_n, uniform permittivity ε\varepsilon, and zero field at both outer depletion edges.

Diagram shown in the original SVG worksheet.

  1. Integrate dE/dx=ρ/εdE/dx=\rho/\varepsilon to find the signed field on each side.

  2. Find the potential rise Vj=ϕ(xn)−ϕ(−xp)V_j=\phi(x_n)-\phi(-x_p) in terms of peak field magnitude and W, then in terms of doping and widths.

Question 3 - Solution

Poisson integration gives the triangular electric field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ep(x)=−eNAε(x+xp),En(x)=eNDε(x−xn).\boxed{E_p(x)=-\frac{eN_A}{\varepsilon}(x+x_p),\quad E_n(x)=\frac{eN_D}{\varepsilon}(x-x_n)}.Emax=|E(0)|=eNAxp/ε=eNDxn/ε.\boxed{E_{\max}=|E(0)|=eN_Ax_p/\varepsilon=eN_Dx_n/\varepsilon}.

(b) Interpretation and further calculation

Vj=−∫−xpxnEdx=12Emax(xp+xn)=12EmaxW.V_j=-\int_{-x_p}^{x_n}E\,dx=\boxed{\tfrac12E_{\max}(x_p+x_n)=\tfrac12E_{\max}W}.Vj=e2ε(NAxp2+NDxn2).\boxed{V_j=\frac{e}{2\varepsilon}(N_Ax_p^2+N_Dx_n^2)}.

Physical check

The field points from the positive donor ions on the n side toward negative acceptor ions on the p side. Its negative area gives a positive potential rise toward n.