Doped Semiconductors — Question 7

Section 41-6 · Physics pages 6904–6905

Question 7 Impurity scattering makes conductivity gains saturate For a fully ionized donor-dominated semiconductor, use n = ND and the empirical mobility law µ(ND) = µ0/(1 + ND/N∗). Neglect holes. ND/N∗ σ Schematic; labels, not drawing lengths, specify the data. (a) Derive conductivity and its high-density limit within this model. (b) Find the donor density at which conductivity reaches 90 percent of that limit, and the mobility there.
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Question 7 - Solution Impurity scattering makes conductivity gains saturate ND/N∗ σ (a) Method and calculation σ = eNDµ0/(1 + ND/N∗) = eµ0N∗ x 1 + x, x = ND/N∗. σ∞= eµ0N∗. (b) Interpretation and further calculation x/(1 + x) = .90 ⇒x = 9, ND = 9N∗. µ(9N∗) = µ0/10, σ = .9eµ0N∗. Physical check The asymptote is a property of the stated mobility law, not a universal bound. Increasing dopant density raises carrier count while also increasing scattering.

Question 7

Impurity scattering makes conductivity gains saturate

For a fully ionized donor-dominated semiconductor, use n=NDn=N_D and the empirical mobility law μ(ND)=μ0/(1+ND/N*)\mu(N_D)=\mu_0/(1+N_D/N_*). Neglect holes.

Diagram shown in the original SVG worksheet.

  1. Derive conductivity and its high-density limit within this model.

  2. Find the donor density at which conductivity reaches 90 percent of that limit, and the mobility there.

Question 7 - Solution

Impurity scattering makes conductivity gains saturate

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σ=eNDμ0/(1+ND/N*)=eμ0N*x1+x,x=ND/N*.\sigma=eN_D\mu_0/(1+N_D/N_*)=e\mu_0N_*\frac{x}{1+x},\quad x=N_D/N_*.σ∞=eμ0N*.\boxed{\sigma_{\infty}=e\mu_0N_*}.

(b) Interpretation and further calculation

x/(1+x)=.90⇒x=9,ND=9N*.x/(1+x)=.90\Rightarrow\boxed{x=9,\quad N_D=9N_*}.μ(9N*)=μ0/10,σ=.9eμ0N*.\boxed{\mu(9N_*)=\mu_0/10,\quad\sigma=.9e\mu_0N_*}.

Physical check

The asymptote is a property of the stated mobility law, not a universal bound. Increasing dopant density raises carrier count while also increasing scattering.