Math 2.0

Statistical mechanics, structure of matter Definition

Fermi surface

Builds on Electronic band structureBrillouin zoneFermi–Dirac statistics

Definition

Consider non-interacting electrons in a crystal with band functions Em ⁣:B→ℝE_m \colon B \to \R, m≥1m \ge 1, on the Brillouin zone BB. Let EFE_F be the Fermi energy, the chemical potential at zero temperature fixed by the electron density. The Fermi surface is the set SF={k∈B:Em(k)=EF for some m≥1}.S_F = \set{k \in B : E_m(k) = E_F \text{ for some } m \ge 1}. At zero temperature, by Fermi–Dirac statistics, the states with Em(k)<EFE_m(k) < E_F are occupied and those with Em(k)>EFE_m(k) > E_F are empty. So SFS_F is the boundary of the occupied region in each band.

Remarks

Example: free electrons in ℝ3\R^3 with E(k)=ℏ2∣k∣2/2mE(k) = \hbar^2 \abs{k}^2 / 2m. The Fermi surface is the sphere ∣k∣=kF\abs{k} = k_F with EF=ℏ2kF2/2mE_F = \hbar^2 k_F^2 / 2m. Counting two spin states per wave vector, the density is n=2⋅43πkF3/(2π)3=kF3/3π2n = 2 \cdot \tfrac{4}{3}\pi k_F^3 / (2\pi)^3 = k_F^3 / 3\pi^2, so kF=(3π2n)1/3k_F = (3\pi^2 n)^{1/3}.

Example: for the one-dimensional tight-binding band E(k)=−2tcos⁡kE(k) = -2t\cos k at half filling, EF=0E_F = 0 and the Fermi surface is the pair of points k=±π/2k = \pm\pi/2.

Non-example: in a band insulator EFE_F lies in a spectral gap, so no EmE_m takes the value EFE_F and the Fermi surface is empty.

Reading path

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  1. Brillouin zone concept
  2. Electronic band structure concept
  3. Fermi–Dirac statistics concept
  4. Fermi surface definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Fermi_surface
About this page
TagE4VEYCFB25
URIm2://E4VEYCFB25
Kinddefinition
WritingW0 stub
MSC82D35, 82D20
DefinesFermi surface
UsesElectronic band structure, Brillouin zone, Fermi–Dirac statistics
Changed3 November 2026

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