ConceptComplete

Classification of Simple Lie Algebras - Examples and Constructions

Explicit constructions of simple Lie algebras demonstrate how abstract classification translates to concrete mathematical objects. Each type has characteristic realizations illuminating its structure.

Example

Type AnA_n - sln+1(C)\mathfrak{sl}_{n+1}(\mathbb{C}): Traceless complex (n+1)×(n+1)(n+1) \times (n+1) matrices with bracket [X,Y]=XYYX[X,Y] = XY - YX.

Cartan subalgebra: diagonal matrices diag(h1,,hn+1)\text{diag}(h_1, \ldots, h_{n+1}) with hi=0\sum h_i = 0

Root vectors: EijE_{ij} (matrix with 1 in position (i,j)(i,j), zero elsewhere) for iji \neq j

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

Example

Type BnB_n - so2n+1(C)\mathfrak{so}_{2n+1}(\mathbb{C}): Skew-symmetric (2n+1)×(2n+1)(2n+1) \times (2n+1) matrices preserving the standard bilinear form.

Can be realized as block matrices: (AuvTv0uTwTuAT)\begin{pmatrix} A & u & v^T \\ -v & 0 & u^T \\ w^T & -u & -A^T \end{pmatrix} where AA is n×nn \times n, u,v,wu, v, w are n×1n \times 1.

Root system has short roots {±ei}\{\pm e_i\} and long roots {±ei±ej}\{\pm e_i \pm e_j\}.

Example

Type CnC_n - sp2n(C)\mathfrak{sp}_{2n}(\mathbb{C}): Matrices preserving the symplectic form J=(0InIn0)J = \begin{pmatrix} 0 & I_n \\ -I_n & 0 \end{pmatrix}: sp2n={X:XTJ+JX=0}\mathfrak{sp}_{2n} = \{X : X^T J + JX = 0\}

Block form: (ABCAT)\begin{pmatrix} A & B \\ C & -A^T \end{pmatrix} where B,CB, C are symmetric n×nn \times n matrices.

Root system has long roots {±2ei}\{\pm 2e_i\} and short roots {±ei±ej}\{\pm e_i \pm e_j\}.

Example

Type DnD_n - so2n(C)\mathfrak{so}_{2n}(\mathbb{C}): Skew-symmetric 2n×2n2n \times 2n matrices. Root system {±ei±ej:ij}\{\pm e_i \pm e_j : i \neq j\} has all roots the same length.

The Dynkin diagram fork reflects the even-dimensional spinor representations' special properties (in D4D_4, this becomes triality).

Exceptional algebra constructions:

Example

Type G2G_2 - Octonion derivations: The automorphism algebra of the octonions O\mathbb{O} gives G2G_2. Alternatively, construct from sl3\mathfrak{sl}_3 by adding derivations of a cubic form, yielding 14-dimensional algebra.

Root system fits in a plane with 6 short and 6 long roots (length ratio 3\sqrt{3}).

Remark

Type F4F_4 arises as automorphisms of the Albert algebra (exceptional Jordan algebra of 3×33 \times 3 Hermitian matrices over octonions). It has dimension 52 and rank 4.

Example

Types E6,E7,E8E_6, E_7, E_8 - Chevalley construction: Start with the Cartan matrix, define generators {ei,fi,hi:i=1,,n}\{e_i, f_i, h_i : i = 1, \ldots, n\} satisfying Serre relations: [hi,ej]=aijej,[hi,fj]=aijfj[h_i, e_j] = a_{ij} e_j, \quad [h_i, f_j] = -a_{ij} f_j [ei,fj]=δijhi[e_i, f_j] = \delta_{ij} h_i (adei)1aij(ej)=0,(adfi)1aij(fj)=0(\text{ad}_{e_i})^{1-a_{ij}}(e_j) = 0, \quad (\text{ad}_{f_i})^{1-a_{ij}}(f_j) = 0

This presentation constructs the algebra purely from Dynkin diagram data.

Freudenthal magic square: The exceptional algebras fit into a 4×44 \times 4 table constructed from compositions of division algebras R,C,H,O\mathbb{R}, \mathbb{C}, \mathbb{H}, \mathbb{O}:

& \mathbb{R} & \mathbb{C} & \mathbb{H} & \mathbb{O} \\ \hline \mathbb{R} & A_1 & A_2 & C_3 & F_4 \\ \mathbb{C} & A_2 & A_2 \oplus A_2 & A_5 & E_6 \\ \mathbb{H} & C_3 & A_5 & D_6 & E_7 \\ \mathbb{O} & F_4 & E_6 & E_7 & E_8 \end{array}$$ This shows exceptional algebras arise naturally from extending classical constructions to octonions.