Energy Levels in a Crystalline Solid — Question 5

Section 41-2 · Physics pages 6820–6821

Question 5 A filled symmetric band has zero current even though individual states move At zero temperature every k state in an isolated band is occupied by both spins. The band obeys E(−k) = E(k) and v(k) = ℏ−1dE/dk. For a ring of length L, define current I = −(e/L) ∑ k,s v(k). k paired opposite velocities Schematic; labels, not drawing lengths, specify the data. (a) Show that the band current vanishes. (b) Remove one electron from a state of velocity v0. Find the change in current and its hole interpretation.
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Question 5 - Solution A filled symmetric band has zero current even though individual states move k paired opposite velocities (a) Method and calculation E(−k) = E(k) ⇒v(−k) = −v(k) . ∑ k,s v(k) = 0 ⇒Ifull = 0 . (b) Interpretation and further calculation ∆I = − ( −e Lv0 ) = +ev0/L . Ihole = qhvh/L ⇒qh = +e, vh = v0 . Physical check The hole represents a missing contribution from an otherwise full band. This cancellation is a property of occupied band states, not a claim that every occupied electron is stationary.

Question 5

A filled symmetric band has zero current even though individual states move

At zero temperature every k state in an isolated band is occupied by both spins. The band obeys E(−k)=E(k)E(-k)=E(k) and v(k)=ℏ−1dE/dkv(k)=\hbar^{-1}dE/dk. For a ring of length L, define current I=−(e/L)∑k,sv(k)I=-(e/L)\sum_{k,s}v(k).

Diagram shown in the original SVG worksheet.

  1. Show that the band current vanishes.

  2. Remove one electron from a state of velocity v0v_0. Find the change in current and its hole interpretation.

Question 5 - Solution

A filled symmetric band has zero current even though individual states move

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E(−k)=E(k)⇒v(−k)=−v(k).E(-k)=E(k)\Rightarrow\boxed{v(-k)=-v(k)}.∑k,sv(k)=0⇒Ifull=0.\sum_{k,s}v(k)=0\Rightarrow\boxed{I_{\mathrm{full}}=0}.

(b) Interpretation and further calculation

ΔI=−(−eLv0)=+ev0/L.\Delta I=-\left(-\frac{e}{L}v_0\right)=\boxed{+ev_0/L}.Ihole=qhvh/L⇒qh=+e,vh=v0.I_{\mathrm{hole}}=q_hv_h/L\Rightarrow\boxed{q_h=+e,\quad v_h=v_0}.

Physical check

The hole represents a missing contribution from an otherwise full band. This cancellation is a property of occupied band states, not a claim that every occupied electron is stationary.