Part 4 of 15. Integrality of the Cartan numbers forces every angle between roots to be exactly one of four values: 90°, 120°, 135°, or 150°. No other angle is possible. This discrete quantisation is why simple Lie algebras are so rigid, and it is the first real theorem of Act II.
Act I gave us a finite root system Δ in Euclidean space 𝔼 with a Weyl group acting by reflections. The Cartan integer nβ, α = 2(β, α)/(α, α) must be an integer for every ordered pair (α, β), by sl2 representation theory.
The geometric consequence: integrality plus Cauchy–Schwarz restricts the angle between two roots to exactly four values, 90°, 120°, 135°, 150°. This is the crystallographic restriction. Every subsequent classification argument is a combinatorial walk through those four options.
Take any two linearly independent roots α, β ∈ Δ. Both of the Cartan integers
are integers, by explainer 3. Their product is
where θ is the angle between α and β. The right side is symmetric in the pair, and 4 cos²θ is an integer because both factors are.
Since cos²θ ∈ [0, 1], 4 cos²θ ∈ [0, 4]. Integrality forces
five integer values. 4 cos²θ = 4 means parallel roots, which we excluded. For linearly independent roots the product is in {0, 1, 2, 3}: four possibilities, four allowed angles.
Converting each of the four integer values back to an angle:
The Cartan integers are asymmetric precisely when the roots have different lengths. The "more negative" integer comes from the longer root, and the length ratio is √k where k is the product.
Simple roots are obtuse. For simple roots (positive, part of a minimal generating set, see next explainer), (α, β) ≤ 0. This cuts each pair to its obtuse member: 120°, 135°, 150°. So between two distinct simple roots the angle is exactly 90°, 120°, 135°, or 150°.
Figure 1. Crystallographic angle picker. Drag the angle θ and the length ratio |β|/|α|, and watch the Cartan integers nα, β and nβ, α recompute live. A configuration is "legal" (green) iff both Cartan integers are integers and their product is in {0, 1, 2, 3}. Try the preset angles 90°, 120°, 135°, 150° with the default ratio 1.0 (then with √2 and √3) to see the four canonical legal configurations.
Each allowed configuration corresponds to a different kind of edge in a Dynkin diagram, recording how strongly two nodes interact:
| Product | Angle (simple-root) | Cartan integers | Length ratio | Dynkin edge | Seen in |
|---|---|---|---|---|---|
| 0 | 90° | (0, 0) | any | no edge | orthogonal generators |
| 1 | 120° | (−1, −1) | 1 : 1 | single edge | A, D, E |
| 2 | 135° | (−1, −2) | 1 : √2 | double edge with arrow | B, C, F4 |
| 3 | 150° | (−1, −3) | 1 : √3 | triple edge with arrow | G2 |
The triple edge is so restrictive it only appears in G2 (rank 2). No simple Lie algebra of rank 3 or more contains one. The double edge appears in Bn, Cn, F4, and only at the end of a chain (Bn, Cn) or between simply-laced arms (F4). The simple edge (120°) builds the entire ADE family.
The crystallographic restriction in one sentence: any two roots are either orthogonal or meet at 120°, 135°, or 150°, with non-orthogonal pairs in length ratio 1, √2, or √3. The classification reduces from vector configurations to graphs.
Once we know the angles and lengths between every pair of simple roots, we can reconstruct the full root system by Weyl reflections. The data lives in a Cartan matrix, an n × n integer matrix whose off-diagonals encode the edge type. Each Cartan matrix determines a Dynkin diagram, and the classification becomes: which connected graphs can be Dynkin diagrams of a positive-definite Cartan matrix?
The proof is short. Every admissible Dynkin diagram must be a tree with valency at most 3. Counting trees with valency ≤ 3 reduces to the Diophantine inequality 1/p + 1/q + 1/r > 1 on the arm lengths. It has two infinite families of solutions — linear chains (giving An) and one-fork trees (giving Dn) — plus exactly three exceptional solutions with all arms of length ≥ 2: (3, 3, 2), (4, 3, 2), (5, 3, 2), corresponding to E6, E7, E8.
What discreteness gives us. The classification problem becomes "which integer matrices of a specific form have strictly positive eigenvalues?" — a finite combinatorial question. Integrality collapses the continuum of angles to four, and that is what makes the classification finite.
The next explainer turns the combinatorics into a single diagram per algebra.