Serre's theorem on a semisimple Lie algebra

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In abstract algebra, specifically the theory of Lie algebras, Serre's theorem states: given a (finite reduced) root system Φ, there exists a finite-dimensional semisimple Lie algebra whose root system is the given Φ.

Statement

The theorem states that: given a root system Φ in a Euclidean space with an inner product (,), ⟨β,α⟩=2(α,β)/(α,α),β,α∈E and a base {α1,…,αn} of Φ, the Lie algebra 𝔤 defined by (1) 3n generators ei,fi,hi and (2) the relations

[hi,hj]=0,
[ei,fi]=hi,[ei,fj]=0,i≠j,
[hi,ej]=⟨αi,αj⟩ej,[hi,fj]=−⟨αi,αj⟩fj,
ad⁡(ei)−⟨αi,αj⟩+1(ej)=0,i≠j,
ad⁡(fi)−⟨αi,αj⟩+1(fj)=0,i≠j.

is a finite-dimensional semisimple Lie algebra with the Cartan subalgebra generated by hi's and with the root system Φ.

The square matrix [⟨αi,αj⟩]1≤i,j≤n is called the Cartan matrix. Thus, with this notion, the theorem states that, give a Cartan matrix A, there exists a unique (up to an isomorphism) finite-dimensional semisimple Lie algebra 𝔤(A) associated to A. The construction of a semisimple Lie algebra from a Cartan matrix can be generalized by weakening the definition of a Cartan matrix. The (generally infinite-dimensional) Lie algebra associated to a generalized Cartan matrix is called a Kac–Moody algebra.

Sketch of proof

The proof here is taken from (Serre 1966) and (Kac 1990). Let aij=⟨αi,αj⟩ and then let 𝔤~ be the Lie algebra generated by (1) the generators ei,fi,hi and (2) the relations:

  • [hi,hj]=0,
  • [ei,fi]=hi, [ei,fj]=0,i≠j,
  • [hi,ej]=aijej,[hi,fj]=−aijfj.

Let 𝔥 be the free vector space spanned by hi, V the free vector space with a basis v1,…,vn and T=⨁l=0∞V⊗l the tensor algebra over it. Consider the following representation of a Lie algebra:

π:𝔤~→𝔤𝔩(T)

given by: for a∈T,h∈𝔥,λ∈𝔥*,

  • π(fi)a=vi⊗a,
  • π(h)1=⟨λ,h⟩1,π(h)(vj⊗a)=−⟨αj,h⟩vj⊗a+vj⊗π(h)a, inductively,
  • π(ei)1=0,π(ei)(vj⊗a)=δijαi(a)+vj⊗π(ei)a, inductively.

It is not trivial that this is indeed a well-defined representation and that has to be checked by hand. From this representation, one deduces the following properties: let 𝔫~+ (resp. 𝔫~−) the subalgebras of 𝔤~ generated by the ei's (resp. the fi's).

  • 𝔫~+ (resp. 𝔫~−) is a free Lie algebra generated by the ei's (resp. the fi's).
  • As a vector space, 𝔤~=𝔫~+⨁𝔥⨁𝔫~−.
  • 𝔫~+=⨁0≠α∈Q+𝔤~α where 𝔤~α={x∈𝔤~|[h,x]=α(h)x,h∈𝔥} and, similarly, 𝔫~−=⨁0≠α∈Q+𝔤~−α.
  • (root space decomposition) 𝔤~=(⨁0≠α∈Q+𝔤~−α)⨁𝔥⨁(⨁0≠α∈Q+𝔤~α).

For each ideal 𝔦 of 𝔤~, one can easily show that 𝔦 is homogeneous with respect to the grading given by the root space decomposition; i.e., 𝔦=⨁α(𝔤~α∩𝔦). It follows that the sum of ideals intersecting 𝔥 trivially, it itself intersects 𝔥 trivially. Let 𝔯 be the sum of all ideals intersecting 𝔥 trivially. Then there is a vector space decomposition: 𝔯=(𝔯∩𝔫~−)⊕(𝔯∩𝔫~+). In fact, it is a 𝔤~-module decomposition. Let

𝔤=𝔤~/𝔯.

Then it contains a copy of 𝔥, which is identified with 𝔥 and

𝔤=𝔫+⨁𝔥⨁𝔫−

where 𝔫+ (resp. 𝔫−) are the subalgebras generated by the images of ei's (resp. the images of fi's).

One then shows: (1) the derived algebra [𝔤,𝔤] here is the same as 𝔤 in the lead, (2) it is finite-dimensional and semisimple and (3) [𝔤,𝔤]=𝔤.

References