Introduction to Solid State Physics · Problem 10

FREE ELECTRON FERMI GAS — Charles Kittel

Physics — Solid State · maximum-surface-resistance

Problem

Maximum surface resistance. Consider a square sheet of side LL, thickness dd, and electrical resistivity ρ\rho. The resistance measured between opposite edges of the sheet is called the surface resistance: Rsq=ρL/Ld=ρ/dR_{\rm sq} = \rho L/Ld = \rho/d, which is independent of the area L2L^2 of the sheet. (RsqR_{\rm sq} is called the resistance per square and is expressed in ohms per square, because ρ/d\rho/d has the dimensions of ohms.) If we express ρ\rho by (44), then Rsq=m/nde2τR_{\rm sq} = m/nde^2\tau. Suppose now that the minimum value of the collision time is determined by scattering from the surfaces of the sheet, so that τ≈d/vF\tau \approx d/v_F, where vFv_F is the Fermi velocity. Thus the maximum surface resistivity is Rsq≈mvF/nd2e2R_{\rm sq} \approx mv_F/nd^2e^2. Show for a monatomic metal sheet one atom in thickness that Rsq≈ℏ/e2=4.1  kΩR_{\rm sq} \approx \hbar/e^2 = 4.1\;\mathrm{k}\Omega.

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