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Classical root systems in coordinates

Example

For n≥2, in the standard coordinates ε1,…,εn of Rn (and the sum-zero hyperplane for type A):

An−1={εi−εj:i≠j},Bn={±εi}∪{±εi±εj:i<j}, Cn={±2εi}∪{±εi±εj:i<j},Dn={±εi±εj:i<j}.

Each is a reduced crystallographic Euclidean root system with the standard simple roots and Dynkin diagram, and each is the root system computed from the corresponding classical matrix Lie algebra.

Facts & Assumptions

Given: An integer n≥2, the standard orthonormal basis ε1,…,εn of Rn, and the four displayed sets.

[L1]

A reduced crystallographic root system is a finite spanning set of nonzero vectors that is closed under its root reflections, has integral Cartan integers, and meets each root line in exactly the two signs (Reduced crystallographic Euclidean root system).

[L2]

The root systems of the classical matrix Lie algebras with diagonal Cartan subalgebras are these same sets, with one-dimensional root spaces (Root systems of the classical complex Lie algebras).

[L3]

In the cited coordinate models, the standard simple roots are εi−εi+1 for An−1; ε1−ε2,…,εn−1−εn,εn for Bn; ε1−ε2,…,εn−1−εn,2εn for Cn; and, for Dn with n≥3, ε1−ε2,…,εn−2−εn−1,εn−1−εn,εn−1+εn. For D2 the two simple roots are ε1−ε2 and ε1+ε2.

Verification

technique · direct
1.1L1algebra

Each set is finite, omits 0, and is reduced. The differences εi−εn span the sum-zero hyperplane for An−1; Bn and Cn contain a nonzero multiple of every coordinate vector; and in Dn, (εi+εj)+(εi−εj)=2εi for any j≠i, which exists because n≥2. Thus each set spans its stated Euclidean space.

1.2L1algebra

Reflection closure: sεi and s2εi negate the ith coordinate and preserve Bn,Cn,Dn; sεi−εj swaps coordinates i,j and preserves all four sets; and sεi+εj swaps and negates those two coordinates and preserves Bn,Cn,Dn. These are precisely the root reflections that occur in the displayed sets.

2.1L1step 1.1step 1.2algebra

Integrality: proportional pairs give Cartan integer ±2. For nonproportional pairs, roots of squared length 2 pair by 0 or ±1; a short root of squared length 1 in Bn pairs by 0 or ±1; and a long root 2εi of squared length 4 in Cn pairs with a mixed root by 0 or ±2. Hence every Cartan integer is in {0,±1,±2}. Together with steps 1.1 and 1.2, [L1] proves that all four displayed sets are reduced crystallographic root systems.

3.1L2L3step 2.1algebra∎

The listed simple roots of [L3] have the standard Cartan matrices of An−1,Bn,Cn,Dn (with D2=A1⊔A1), giving the stated Dynkin diagrams; and [L2] identifies these coordinate sets as the root systems of sln,so2n+1,sp2n,so2n respectively.

Remarks

The following Dynkin schematics use the simple roots of [L3], numbered in their listed order. For An−1, αi=εi−εi+1. For Bn and Cn the same formula holds for i<n, with αn=εn and αn=2εn, respectively. For Dn, αi=εi−εi+1 for i<n and αn=εn−1+εn. The schematics are drawn for n≥5; dots abbreviate intermediate chain vertices. An arrow on a double edge points toward the shorter simple root.

An¡1®1¢¢¢®n¡2®n¡1Bn®1¢¢¢®n¡1®nCn®1¢¢¢®n¡1®nDn®1¢¢¢®n¡2®n¡1®n

The smaller ranks are obtained by shortening the chains, with A1 a single vertex. In D3 the chain is α2−α1−α3; in D4 the fork vertex is α2. In D2, the roots α1=ε1−ε2 and α2=ε1+ε2 are orthogonal, so its two vertices are disconnected:

D2®1®2

Indeed, the adjacent difference roots have squared length 2 and inner product −1. The last Bn pair has squared lengths 2,1 and inner product −1; the last Cn pair has squared lengths 2,4 and inner product −2. For Dn, both fork edges have inner product −1, while the two terminal roots are orthogonal. Thus the double edges point in opposite directions in Bn and Cn, and the Dn fork has only single edges, as in step 3.1. The verification above is independent of these illustrations.

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