The p-n Junction — Question 4

Section 41-7 · Physics pages 6918–6919

Question 4 The depletion width follows from electrostatics and charge balance For an abrupt junction use NAxp = NDxn, W = xp + xn, and Vj = e(NAx2 p + NDx2 n)/(2ε). p n −xp xn W Schematic; labels, not drawing lengths, specify the data. (a) Derive W in terms of Vj, NA, and ND. (b) Evaluate W for NA = ND = 1022 m−3, Vj = .800 V, ε = 1.00 × 10−10 F/m, and e = 1.60 × 10−19 C.
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Question 4 - Solution The depletion width follows from electrostatics and charge balance p n −xp xn W (a) Method and calculation xp = NDW NA + ND , xn = NAW NA + ND . W = √ 2εVj e ( 1 NA + 1 ND ) . (b) Interpretation and further calculation W 2 = 2(10−10)(.800) 1.60 × 10−19 2 1022 = 2.00 × 10−13 m2. W = .4472 µm, xp = xn = .2236 µm . Physical check The dimensions under the square root are length squared. Larger doping reduces the distance needed to support the specified potential.

Question 4

The depletion width follows from electrostatics and charge balance

For an abrupt junction use NAxp=NDxnN_Ax_p=N_Dx_n, W=xp+xnW=x_p+x_n, and Vj=e(NAxp2+NDxn2)/(2ε)V_j=e(N_Ax_p^2+N_Dx_n^2)/(2\varepsilon).

Diagram shown in the original SVG worksheet.

  1. Derive W in terms of VjV_j, NAN_A, and NDN_D.

  2. Evaluate W for NA=ND=1022m−3N_A=N_D=10^{22}\,\mathrm{m^{-3}}, Vj=.800VV_j=.800\,\mathrm V, ε=1.00×10−10F/m\varepsilon=1.00\times10^{-10}\,\mathrm{F/m}, and e=1.60×10−19Ce=1.60\times10^{-19}\,\mathrm C.

Question 4 - Solution

The depletion width follows from electrostatics and charge balance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

xp=NDWNA+ND,xn=NAWNA+ND.x_p=\frac{N_DW}{N_A+N_D},\quad x_n=\frac{N_AW}{N_A+N_D}.W=2εVje(1NA+1ND).\boxed{W=\sqrt{\frac{2\varepsilon V_j}{e}\left(\frac1{N_A}+\frac1{N_D}\right)}}.

(b) Interpretation and further calculation

W2=2(10−10)(.800)1.60×10−1921022=2.00×10−13m2.W^2=\frac{2(10^{-10})(.800)}{1.60\times10^{-19}}\frac{2}{10^{22}}=2.00\times10^{-13}\,\mathrm{m^2}.W=.4472μm,xp=xn=.2236μm.\boxed{W=.4472\,\mu\mathrm m,\quad x_p=x_n=.2236\,\mu\mathrm m}.

Physical check

The dimensions under the square root are length squared. Larger doping reduces the distance needed to support the specified potential.