In fact, 𝔥=𝔤0 .
sl(2,C) subalgebras, 1
Review of SU(3)
When we studied the representation theory of G=SU(3) (or of its Lie algebra 𝔤=𝔰𝔩(3,𝐂) , one of the key pictures we studied was the root diagram: the weight diagram of its adjoint representation. This was a hexagonal configuration of roots at Li-Lj with i,j∈{1,2,3} , i≠j .

We'll write 𝔤Li-Lj=𝐂⋅Eij for the root space corresponding to the root Li-Lj and 𝔤0 for the weight space corresponding to 0 . Recall that 𝔤0=𝐂⋅H13⊕𝐂⋅H23={(θ1θ2-θ1-θ2):θ1,θ2∈𝐂}.
This Lie algebra has the nice property that if we pick one root Li-Lj and its opposite root Lj-Li ), and we pick generators Eij∈𝔤Li-Lj and Eji∈𝔤Lj-Li then the three elements Eij,Eji,Hij=[Eij,Eji] span a Lie subalgebra isomorphic to 𝔰𝔩(2,𝐂) . Our study of the structure of 𝔰𝔩(3,𝐂) representations used the three 𝔰𝔩(2,𝐂) subalgebras we obtained this way: for example, it gave us the Weyl symmetry group. This will generalise.
Roots in general
The setup
Suppose K is a compact matrix group with Lie algebra 𝔨 . Let's write 𝔤 for the complexification 𝔨⊗𝐂 . Inside K we have a maximal torus T with Lie algebra 𝔱 . Let's write 𝔥=𝔱⊗𝐂⊂𝔤 . The adjoint representation is a map Ad:K→GL(𝔨) , defined by g↦Adg,Adg(X)=gXg-1. The same formula defines a complex representation, also written Ad:K→GL(𝔤) , if we allow X to live in 𝔤 . By taking the derivative we get the Lie algebra representation ad:𝔨→𝔤𝔩(𝔤) and its complexification ad𝐂:𝔤→𝔤𝔩(𝔤).
The root diagram
Because we have a maximal torus, we get a weight space decomposition 𝔤=⊕𝔤α where 𝔤α={X∈𝔤:adHX=α(H)X∀H∈𝔥}. The direct sum is happening over a finite set of weights. Which weights occur in this direct sum?
-
α=0 occurs, in other words 𝔤0≠0 . This is because 𝔥 is an abelian Lie algebra, so adH(H′)=0 for all H,H′∈𝔥 . Therefore 𝔥⊂𝔤0 (just like in the SU(3) example).
Suppose Z∈𝔤0 , i.e. Z∈𝔤 and adHZ=0 for all H∈𝔥 . Then [H,Z]=0 for all H∈𝔥 . In particular, [H,Z]=0 for all H∈𝔱⊂𝔥 .
Let's write Z=X+iY where X,Y∈𝔨 (so they are the real and imaginary parts of Z ). Then 0=[H,Z]=[H,X]+i[H,Y] for all H∈𝔱 , therefore both real and imaginary parts must vanish, and [H,X]=[H,Y]=0 . This means that X,Y∈𝔨 commute with all elements in 𝔱 .
If either X or Y is not contained in 𝔱 then either 𝔱⊕𝐂⋅X or 𝔱⊕𝐂⋅Y will be an abelian subalgebra 𝔱′ strictly containing 𝔱 . Then ¯exp(𝔱′) is a torus strictly containing T , which contradicts the assumption that T is a maximal torus.
Which other weights occur?
Any nonzero weight of the adjoint representation is called a
Action of root vectors
-
If X∈𝔤α and Y∈𝔤β then [X,Y]∈𝔤α+β . (We won't prove this: it's an exercise, very similar to the corresponding results for 𝔰𝔩(2,𝐂) and 𝔰𝔩(3,𝐂) , like "X moves things to the right and Y moves things to the left".)
-
If X∈𝔤α and Y∈𝔤β then K(X,Y)=0 unless α+β=0 .
-
If 𝔤 is semisimple then α∈R if and only if .
(2). Pick a basis of consisting of root vectors. We'll compute the matrix of with respect to this basis and then take the trace to find . Suppose is one of our basis vectors. Where does go under ? By part (a), .
Let's write as a block matrix with respect to the splitting into weight spaces (i.e. the block in the matrix is the matrix of the map ).
The diagonal blocks encode the maps . But if then sends to , so there are no nonzero diagonal blocks if . Therefore the trace of this matrix vanishes and .
(3) If is semisimple then the Killing form is nondegenerate, so for all nonzero there exists such that . In particular, if then there exists such that .
Take the components of with respect to the weight space splitting. Then unless . Therefore, if , we must have , so and .
The trick for extracting the subalgebras will be the following theorem which we'll prove next time.
If , are nonzero then , and will span a subalgebra isomorphic to .
Pre-class exercise
True or false: If we use a sub-maximal torus, is it still true that ? If so, why? If not, what do we get instead?