Metals — Question 10

Section 41-4 · Physics pages 6870–6871

Question 10 Independent scattering channels add as inverse lifetimes A metal has independent impurity and phonon relaxation times τi = 6.00 × 10−14 s and τp = 3.00 × 10−14 s. Survival probabilities multiply: P(t) = e−t/τie−t/τp. t/τ P dashed: impurities only Schematic; labels, not drawing lengths, specify the data. (a) Derive the effective relaxation time and the fraction of scattering events due to impurities. (b) If phonon scattering is suppressed while impurities remain, find the conductivity increase and explain why resistivities add.
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Question 10 - Solution Independent scattering channels add as inverse lifetimes t/τ P dashed: impurities only (a) Method and calculation P(t) = e−t(1/τi+1/τp) ⇒τ = τiτp τi + τp = 2.00 × 10−14 s . fi = (1/τi)/(1/τi + 1/τp) = 1/3 . (b) Interpretation and further calculation σ ∝τ ⇒σcold/σ = τi/τ = 3 . ρ = m ne2 ( 1 τi + 1 τp ) = ρi + ρp . Physical check Adding rates assumes independent mechanisms with the same simple transport weighting. The result need not hold for strongly anisotropic or correlated scattering.

Question 10

Independent scattering channels add as inverse lifetimes

A metal has independent impurity and phonon relaxation times τi=6.00×10−14s\tau_i=6.00\times10^{-14}\,\mathrm s and τp=3.00×10−14s\tau_p=3.00\times10^{-14}\,\mathrm s. Survival probabilities multiply: P(t)=e−t/τie−t/τpP(t)=e^{-t/\tau_i}e^{-t/\tau_p}.

Diagram shown in the original SVG worksheet.

  1. Derive the effective relaxation time and the fraction of scattering events due to impurities.

  2. If phonon scattering is suppressed while impurities remain, find the conductivity increase and explain why resistivities add.

Question 10 - Solution

Independent scattering channels add as inverse lifetimes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P(t)=e−t(1/τi+1/τp)⇒τ=τiτpτi+τp=2.00×10−14s.P(t)=e^{-t(1/\tau_i+1/\tau_p)}\Rightarrow\boxed{\tau=\frac{\tau_i\tau_p}{\tau_i+\tau_p}=2.00\times10^{-14}\,\mathrm s}.fi=(1/τi)/(1/τi+1/τp)=1/3.\boxed{f_i=(1/\tau_i)/(1/\tau_i+1/\tau_p)=1/3}.

(b) Interpretation and further calculation

σ∝τ⇒σcold/σ=τi/τ=3.\sigma\propto\tau\Rightarrow\boxed{\sigma_{\mathrm{cold}}/\sigma=\tau_i/\tau=3}.ρ=mne2(1τi+1τp)=ρi+ρp.\boxed{\rho=\frac{m}{ne^2}\left(\frac1{\tau_i}+\frac1{\tau_p}\right)=\rho_i+\rho_p}.

Physical check

Adding rates assumes independent mechanisms with the same simple transport weighting. The result need not hold for strongly anisotropic or correlated scattering.