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The point group of a crystallographic group is integral in a lattice basis

Proved
LeanEval.Geometry.SpaceGroupsProblem.pointGroup_integral_matrix

by Gabewhigham · Sep 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

crystallographygeometrygroup-theory

Let GGG be a crystallographic group in dimension ddd — a discrete subgroup of the Euclidean motion group EdE_dEd​ containing ddd linearly independent translations — with translation lattice T(G)T(G)T(G) and point group P(G)P(G)P(G), the group of linear parts of the elements of GGG.

The theorem asserts that one may choose a basis adapted to the lattice in which every element of the point group becomes an integer matrix: there are vectors w1,…,wdw_1,\dots,w_dw1​,…,wd​, linearly independent over R\mathbb{R}R, with T(G)=Zw1⊕⋯⊕ZwdT(G)=\mathbb{Z}w_1\oplus\cdots\oplus\mathbb{Z}w_dT(G)=Zw1​⊕⋯⊕Zwd​, such that for every A∈P(G)A\in P(G)A∈P(G) there is a matrix M∈Md(Z)M\in M_d(\mathbb{Z})M∈Md​(Z) with

Awj=∑i=1dMij wi(1≤j≤d).A w_j=\sum_{i=1}^{d} M_{ij}\,w_i \qquad (1\le j\le d).Awj​=i=1∑d​Mij​wi​(1≤j≤d).

Equivalently, the point group acts on the translation lattice T(G)≅ZdT(G)\cong\mathbb{Z}^dT(G)≅Zd by Z\mathbb{Z}Z-linear automorphisms, so that P(G)P(G)P(G) is represented inside GLd(Z)GL_d(\mathbb{Z})GLd​(Z). This integrality is the source of the arithmetic constraints on point groups, such as the crystallographic restriction on the possible orders of their elements.

Preamble
import Mathlib
import Definitions.Def_LeanEval_SpaceGroups_Definitions
import Definitions.Def_SpaceGroupsPointGroupDefs
Formal statement
namespace LeanEval
namespace Geometry
namespace SpaceGroupsProblem

theorem pointGroup_integral_matrix {d : ℕ} {G : Subgroup (EuclideanIsom d)}
    (hG : IsCrystallographicGroup G) :
    ∃ w : Fin d → E d, LinearIndependent ℝ w ∧
      Submodule.span ℤ (Set.range w) = transSubmoduleZ G ∧
      ∀ A ∈ pointGroup G, ∃ M : Matrix (Fin d) (Fin d) ℤ,
        ∀ j, A (w j) = ∑ i, (M i j : ℝ) • w i := by sorry

end SpaceGroupsProblem
end Geometry
end LeanEval
Source
L. S. Charlap, Bieberbach Groups and Flat Manifolds, Springer 1986, Chapter I, Section 2 (the holonomy/point group acts on the translation lattice, giving an integral representation).

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