nLab Brillouin torus

Idea

Given a crystalline material, its Brillouin torus is the space of distinguishable momenta/wave vectors of its electronic excitations. Due to the periodicity of the crystal, also these momenta/wave vectors are (dually) periodically identified, which makes this space an n-torus.

Mathematically, the discrete space underlying a crystal is a subset of a Euclidean space $S \;\subset\;E^n \simeq \mathbb{R}^n$ (the set of atomic sites) which is preserved (as a subset) by the action of a crystallographic group $\Lambda \rtimes G \,\subset\, Iso(E)$, where $\Lambda$ is a full lattice (and $G$ the corresponding point group). Then its Brillouin torus is the Pontrjagin dual group of this lattice (eg. Freed-Moore 13):

$$\mathbb{T}^n_{Br} \,=\, Hom_{Grp}\big(\Lambda, \, S^1 \big) \,.$$

Related concepts

• Brillouin zone

• Bravais lattice

• Bloch-Floquet theory

• valence bundle, conduction bundle

References

The concept is named after:

• Léon Brillouin, Les électrons libres dans les métaux et le role des réflexions de Bragg, J. Phys. Radium 1 (1930) 377-400 [doi:10.1051/jphysrad:01930001011037700, hal:jpa-00233038, pdf]

Textbooks on solid state physics traditionally speak of the “reciprocal lattice” (e.g. Kittel 1953, p. 27) which is the dual lattice $Hom_{Grp}\big(\Lambda, \, \mathbb{Z} \big)$, e.g.:

• Michael Reed, Barry Simon, p. 311 of: Sec. XIII.16 Schrödinger operators with periodic potentials, of: Methods of Modern Mathematical Physics – IV: Analysis of Operators, Academic Press (1978)

  (ISBN:9780080570457)

• David Tong, §2.2.2 in: Lectures on solid state physics (2017) $[$pdf, webpage$]$

The resulting Brillouin torus $Hom_{Grp}\big(\Lambda, \, \mathbb{R} \big)/Hom_{Grp}\big(\Lambda, \, \mathbb{Z} \big)$ is often left implicit. It is made explicit in:

• Daniel Freed, Gregory Moore, p. 52 of: Twisted equivariant matter, Ann. Henri Poincaré (2013) 14: 1927 $[$arXiv:1208.5055, doi:10.1007/s00023-013-0236-x$]$