Semiconductors — Question 2

Section 41-5 · Physics pages 6874–6875

Question 2 Unequal band densities shift the intrinsic Fermi level from midgap Use the nondegenerate population formulas n = Nce−(Ec−EF )/kBT and p = Nve−(EF −Ev)/kBT . An intrinsic sample has n=p and Nc/Nv = 4. Ev Ec Eg Ei Schematic; labels, not drawing lengths, specify the data. (a) Derive the intrinsic Fermi energy Ei relative to midgap. (b) At kBT = .0250 eV, calculate the shift and explain its direction.
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Question 2 - Solution Unequal band densities shift the intrinsic Fermi level from midgap Ev Ec Eg Ei (a) Method and calculation ln(Nc/Nv) = Ec + Ev −2Ei kBT . Ei = Ec + Ev 2 + kBT 2 ln(Nv/Nc) . (b) Interpretation and further calculation Ei −Emid = −(.0250/2) ln 4 = −.0173 eV . n p = Nc Nv e2(EF −Emid)/kBT = 1 at EF = Ei. Physical check A larger conduction-band state count requires the Fermi level to move downward to maintain equal electron and hole populations.

Question 2

Unequal band densities shift the intrinsic Fermi level from midgap

Use the nondegenerate population formulas n=Nce−(Ec−EF)/kBTn=N_ce^{-(E_c-E_F)/k_BT} and p=Nve−(EF−Ev)/kBTp=N_ve^{-(E_F-E_v)/k_BT}. An intrinsic sample has n=p and Nc/Nv=4N_c/N_v=4.

Diagram shown in the original SVG worksheet.

  1. Derive the intrinsic Fermi energy EiE_i relative to midgap.

  2. At kBT=.0250eVk_BT=.0250\,\mathrm{eV}, calculate the shift and explain its direction.

Question 2 - Solution

Unequal band densities shift the intrinsic Fermi level from midgap

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ln⁡(Nc/Nv)=Ec+Ev−2EikBT.\ln(N_c/N_v)=\frac{E_c+E_v-2E_i}{k_BT}.Ei=Ec+Ev2+kBT2ln⁡(Nv/Nc).\boxed{E_i=\frac{E_c+E_v}{2}+\frac{k_BT}{2}\ln(N_v/N_c)}.

(b) Interpretation and further calculation

Ei−Emid=−(.0250/2)ln⁡4=−.0173eV.\boxed{E_i-E_{\mathrm{mid}}=-(.0250/2)\ln4=-.0173\,\mathrm{eV}}.np=NcNve2(EF−Emid)/kBT=1at EF=Ei.\frac{n}{p}=\frac{N_c}{N_v}e^{2(E_F-E_{\mathrm{mid}})/k_BT}=1\quad\text{at }E_F=E_i.

Physical check

A larger conduction-band state count requires the Fermi level to move downward to maintain equal electron and hole populations.