Machine-translated by Google. Questions are authored in English.
Top

Discussion

Crystal structures of two metals A and B are two-dimensional square lattices with same lattice constant a. Electrons in metals behave as free electrons. The Fermi surfaces corresponding to A and B are shown by solid circles in figures.

Two k-space diagrams with a dotted square of half-width pi/a. Metal A: the Fermi circle touches the middle of each side of the square, at (pi/a, 0). Metal B: the Fermi circle passes through the four corners of the square

The electron concentrations in A and B are \(n_{A}\) and \(n_{B}\), respectively. The value of \(\left(\dfrac{n_{B}}{n_{A}}\right)\) is

  • A.3
  • B.2
  • C.\(3\sqrt{3}\)
  • D.\(\sqrt{2}\)

Answer: B

The ratio nB/nA is 2.

For free electrons in two dimensions the electron concentration is proportional to the area of the Fermi circle, πkF2, so n ∝ kF2.

  • Metal A: the circle touches the zone boundary at (π/a, 0), so kF = π/a.
  • Metal B: the circle passes through the corners of the square zone, at (π/a, π/a), so kF = √2 π/a.

\[ \begin{aligned} \frac{n_{B}}{n_{A}} &= \left(\frac{\sqrt{2}\,\pi/a}{\pi/a}\right)^{2} \\ &= 2 \end{aligned} \]

√2 is the ratio of the Fermi wavevectors, not of the concentrations. 3 and 3√3 would need other radii, and 3√3 a three-dimensional kF3 scaling.

No comment is present. Be the first to comment.
Loading…

Post your comment

Please log in or register to post a comment.