ConceptComplete

Root Systems and Dynkin Diagrams - Examples and Constructions

Explicit construction of root systems for classical Lie algebras provides concrete realization of the abstract theory. These examples demonstrate how Dynkin diagrams encode algebraic structure.

Example

Type AnA_n (sln+1\mathfrak{sl}_{n+1}):

The root system consists of vectors eieje_i - e_j for 1ijn+11 \leq i \neq j \leq n+1 in Rn+1\mathbb{R}^{n+1} subject to ei=0\sum e_i = 0. There are n(n+1)n(n+1) roots total.

Simple roots: αi=eiei+1\alpha_i = e_i - e_{i+1} for i=1,,ni = 1, \ldots, n

Dynkin diagram: \circ - \circ - \cdots - \circ (nn nodes)

The Weyl group is W=Sn+1W = S_{n+1} (symmetric group), acting by permuting coordinates.

Example

Type BnB_n (so2n+1\mathfrak{so}_{2n+1}):

Root system: {±ei±ej:ij}{±ei}\{\pm e_i \pm e_j : i \neq j\} \cup \{\pm e_i\} in Rn\mathbb{R}^n

Simple roots: αi=eiei+1\alpha_i = e_i - e_{i+1} (i<ni < n), αn=en\alpha_n = e_n

Dynkin diagram: \circ - \circ - \cdots - \circ \Rightarrow \circ (arrow points to last node)

This system has short roots {±ei}\{\pm e_i\} and long roots {±ei±ej}\{\pm e_i \pm e_j\} with length ratio 2\sqrt{2}.

Example

Type CnC_n (sp2n\mathfrak{sp}_{2n}):

Root system: {±ei±ej:ij}{±2ei}\{\pm e_i \pm e_j : i \neq j\} \cup \{\pm 2e_i\} in Rn\mathbb{R}^n

Simple roots: αi=eiei+1\alpha_i = e_i - e_{i+1} (i<ni < n), αn=2en\alpha_n = 2e_n

Dynkin diagram: \circ - \circ - \cdots - \circ \Leftarrow \circ (arrow points from last node)

Here short roots are {±ei±ej}\{\pm e_i \pm e_j\} and long roots are {±2ei}\{\pm 2e_i\}.

Example

Type DnD_n (so2n\mathfrak{so}_{2n}):

Root system: {±ei±ej:ij}\{\pm e_i \pm e_j : i \neq j\} in Rn\mathbb{R}^n

Simple roots: αi=eiei+1\alpha_i = e_i - e_{i+1} (i<ni < n), αn=en1+en\alpha_n = e_{n-1} + e_n

Dynkin diagram: \circ - \circ - \cdots - \begin{matrix}\circ \\ \circ\end{matrix} (fork at end)

All roots have the same length. The Weyl group includes sign changes and even permutations.

Remark

The exceptional root systems G2,F4,E6,E7,E8G_2, F_4, E_6, E_7, E_8 require more sophisticated constructions. For instance, G2G_2 can be realized in the plane as the root system of a hexagonal lattice with two lengths, while E8E_8 naturally lives in 8-dimensional space and has 240 roots.

Construction from Dynkin diagram: Given a Dynkin diagram, one can reconstruct the Cartan matrix A=(aij)A = (a_{ij}) where:

  • aii=2a_{ii} = 2
  • aijaji=a_{ij} a_{ji} = (number of edges between nodes ii and jj)
  • aijaji|a_{ij}| \leq |a_{ji}| with equality iff roots have equal length

The Cartan matrix determines the root system up to isomorphism via the realization: αj=iaijλi\alpha_j = \sum_i a_{ij} \lambda_i where {λi}\{\lambda_i\} are fundamental weights (dual to simple coroots).

Example

Type G2G_2 Cartan matrix: A=(2132)A = \begin{pmatrix} 2 & -1 \\ -3 & 2 \end{pmatrix} The off-diagonal entries multiply to 3, indicating a triple bond in the Dynkin diagram. The asymmetry 1<3|-1| < |-3| indicates the arrow direction.

These constructions show that root systems, while abstractly defined, have concrete realizations as geometric configurations of vectors, making them amenable to both theoretical analysis and explicit computation.