Doped Semiconductors — Question 2

Section 41-6 · Physics pages 6894–6895

Question 2 Compensation changes the majority type through the net dopant density A fully ionized sample has ND = 2.00 × 1022 m−3, NA = 5.00 × 1022 m−3, and ni = 1016 m−3. It is in nondegenerate thermal equilibrium. N + D N − A p −n = NA −ND Schematic; labels, not drawing lengths, specify the data. (a) Find the majority and minority carrier densities to appropriate accuracy. (b) If µp = .0400 m2/(V s) and e = 1.60 × 10−19 C, estimate conductivity and state why the total dopant count is not the carrier count.
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Question 2 - Solution Compensation changes the majority type through the net dopant density N + D N − A p −n = NA −ND (a) Method and calculation p −n = NA −ND = 3.00 × 1022 m−3 ≡∆N. p ≃∆N = 3.00 × 1022, n = n2 i /p = 3.333 × 109 m−3 . (b) Interpretation and further calculation σ ≃epµp = 192 S/m . p ≃NA −ND̸ = NA + ND (n ≪p). Physical check Donors compensate acceptors, leaving the difference to set the majority population. Both kinds of ionized impurities can still contribute to scattering.

Question 2

Compensation changes the majority type through the net dopant density

A fully ionized sample has ND=2.00×1022m−3N_D=2.00\times10^{22}\,\mathrm{m^{-3}}, NA=5.00×1022m−3N_A=5.00\times10^{22}\,\mathrm{m^{-3}}, and ni=1016m−3n_i=10^{16}\,\mathrm{m^{-3}}. It is in nondegenerate thermal equilibrium.

Diagram shown in the original SVG worksheet.

  1. Find the majority and minority carrier densities to appropriate accuracy.

  2. If μp=.0400m2/(Vs)\mu_p=.0400\,\mathrm{m^2/(V\,s)} and e=1.60×10−19Ce=1.60\times10^{-19}\,\mathrm C, estimate conductivity and state why the total dopant count is not the carrier count.

Question 2 - Solution

Compensation changes the majority type through the net dopant density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

p−n=NA−ND=3.00×1022m−3≡ΔN.p-n=N_A-N_D=3.00\times10^{22}\,\mathrm{m^{-3}}\equiv\Delta N.p≃ΔN=3.00×1022,n=ni2/p=3.333×109m−3.\boxed{p\simeq\Delta N=3.00\times10^{22},\quad n=n_i^2/p=3.333\times10^9\,\mathrm{m^{-3}}}.

(b) Interpretation and further calculation

σ≃epμp=192S/m.\boxed{\sigma\simeq ep\mu_p=192\,\mathrm{S/m}}.p≃NA−ND≠NA+ND(n≪p).\boxed{p\simeq N_A-N_D\ne N_A+N_D}\quad(n\ll p).

Physical check

Donors compensate acceptors, leaving the difference to set the majority population. Both kinds of ionized impurities can still contribute to scattering.