Semiconductors — Question 1

Section 41-5 · Physics pages 6872–6873

Question 1 Band-edge populations determine the intrinsic carrier density In a nondegenerate semiconductor, n = Nce−(Ec−EF )/(kBT) and p = Nve−(EF −Ev)/(kBT). Let Eg = Ec −Ev. Ev Ec Eg Schematic; labels, not drawing lengths, specify the data. (a) Derive the equilibrium mass-action relation and intrinsic density. (b) Evaluate ni for Nc = 4.00 × 1025 m−3, Nv = 1.00 × 1025 m−3, Eg = 1.00 eV, and kBT = .0250 eV.
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Question 1 - Solution Band-edge populations determine the intrinsic carrier density Ev Ec Eg (a) Method and calculation np = NcNve−(Ec−Ev)/(kBT) ≡n2 i . n = p = ni ⇒ni = √ NcNv e−Eg/(2kBT) . (b) Interpretation and further calculation √ NcNv = 2.00 × 1025 m−3, Eg/(2kBT) = 20. ni = 2.00 × 1025e−20 = 4.12 × 1016 m−3 . Physical check The Fermi level cancels from np at thermal equilibrium. Illumination or carrier injection can produce distinct quasi-Fermi levels and invalidate this equilibrium product.

Question 1

Band-edge populations determine the intrinsic carrier density

In a nondegenerate semiconductor, n=Nce−(Ec−EF)/(kBT)n=N_c e^{-(E_c-E_F)/(k_BT)} and p=Nve−(EF−Ev)/(kBT)p=N_v e^{-(E_F-E_v)/(k_BT)}. Let Eg=Ec−EvE_g=E_c-E_v.

Diagram shown in the original SVG worksheet.

  1. Derive the equilibrium mass-action relation and intrinsic density.

  2. Evaluate nin_i for Nc=4.00×1025m−3N_c=4.00\times10^{25}\,\mathrm{m^{-3}}, Nv=1.00×1025m−3N_v=1.00\times10^{25}\,\mathrm{m^{-3}}, Eg=1.00eVE_g=1.00\,\mathrm{eV}, and kBT=.0250eVk_BT=.0250\,\mathrm{eV}.

Question 1 - Solution

Band-edge populations determine the intrinsic carrier density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

np=NcNve−(Ec−Ev)/(kBT)≡ni2.np=N_cN_v e^{-(E_c-E_v)/(k_BT)}\equiv n_i^2.n=p=ni⇒ni=NcNve−Eg/(2kBT).n=p=n_i\Rightarrow\boxed{n_i=\sqrt{N_cN_v}\,e^{-E_g/(2k_BT)}}.

(b) Interpretation and further calculation

NcNv=2.00×1025m−3,Eg/(2kBT)=20.\sqrt{N_cN_v}=2.00\times10^{25}\,\mathrm{m^{-3}},\quad E_g/(2k_BT)=20.ni=2.00×1025e−20=4.12×1016m−3.\boxed{n_i=2.00\times10^{25}e^{-20}=4.12\times10^{16}\,\mathrm{m^{-3}}}.

Physical check

The Fermi level cancels from np at thermal equilibrium. Illumination or carrier injection can produce distinct quasi-Fermi levels and invalidate this equilibrium product.