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The Lie algebra of a semisimple group in characteristic zero is semisimple

Statement

Assume the Axiom of Choice inherited from the named suppliers. Let G be a semisimple algebraic group over a field k of characteristic 0 (Split reductive groups, Radical, unipotent radical, semisimple and reductive algebraic groups). Then its Lie algebra g=Lie⁡(G) is semisimple: it has no nonzero solvable ideal.

Facts & Assumptions

Given: A semisimple algebraic group G over a characteristic-zero field k, with g=Lie⁡(G) and the adjoint representation Ad⁡:G→GL⁡g (The adjoint representation of an affine group scheme).

[F1]

The derived series of a Lie algebra is defined by successive brackets; Jacobi makes the successive derived terms of an ideal ideals in the ambient algebra. (Derived series and solvable Lie algebras)

[F2]

Stabilizers and their Lie algebras. For a finite-dimensional rational representation (V,r) and a k-point w∈V(k), the stabilizer of the point w is a closed subgroup scheme of G with Lie⁡(Stab⁡G(w))={x∈g:xw=0}; for the adjoint representation this is the computation Ad⁡(eεx)=id⁡+εad⁡(x) (Algebraic group actions, orbit maps, orbit subschemes and scheme-theoretic stabilizers, Fibres of the orbit map and the scheme-theoretic stabilizer as a closed subgroup scheme, The adjoint representation of an affine group scheme).

[F3]

Normal subgroups and ideals. For a smooth closed subgroup scheme H⊆G, the identity component H∘ is normal in G if and only if Lie⁡(H) is an ideal of g (Lie ideals and normal connected subgroups in characteristic zero).

[F4]

Cartier's theorem makes every affine finite-type group scheme in characteristic 0 smooth. The Lie algebra of a scheme-theoretic centralizer is the fixed subspace under the adjoint action; the differential of the adjoint action is the bracket. (The Lie functor: exactness, fixed points and generation, The adjoint representation of an affine group scheme, Cartier's theorem: affine group schemes in characteristic zero are smooth)

[F5]

The radical of a semisimple group. G is semisimple exactly when R(G)=1, and a semisimple group is reductive; the radical R(G) is the largest smooth connected normal solvable subgroup (Centre, radical and semisimple quotient of a reductive group, Radical, unipotent radical, semisimple and reductive algebraic groups).

Proof

Given: A semisimple algebraic group G over a characteristic-zero field k, with g=Lie⁡(G) and the adjoint representation Ad⁡:G→GL⁡g (The adjoint representation of an affine group scheme).

Proof technique: direct.

1.1F1givenalgebra

If a nonzero solvable ideal r exists, take its last nonzero derived term. Jacobi gives [g,[I,I]]⊆[I,I] for each ambient ideal I, so this term is an ambient ideal, and its next derived term being zero makes it commutative. Thus it suffices to exclude nonzero commutative ideals.

1.2givenalgebra

Let n⊆g be a commutative ideal and put h={x∈g:[x,n]=0}. Then n⊆h because n is commutative, and h is an ideal of g: for y∈g, x∈h and n∈n one has [[y,x],n]=[y,[x,n]]−[x,[y,n]]=0 because [x,n]=0 and [y,n]∈n is killed by x.

2.1F2step 1.2

Choose a k-basis y1,…,ym of n and let H be the stabilizer of the point (y1,…,ym) of the rational representation g⊕m; this is a closed subgroup scheme of G, and Lie⁡(H)=h: a dual-number point eεx lies in H exactly when Ad⁡(eεx)yi=yi for all i, that is, by [F2], exactly when [x,yi]=0 for all i.

3.1F3F4step 1.2step 2.1

Cartier's theorem [F4] makes the closed affine group H smooth. Since h=Lie⁡(H) is an ideal of g by step 1.2, [F3] shows that H∘ is normal in G.

4.1F4step 3.1algebra

For any smooth connected affine H0 in characteristic 0, Z(H0)=ker⁡Ad⁡H0. Indeed, over an algebraic closure a point of the latter has centralizer with full Lie algebra by [F4]. Cartier makes that centralizer smooth, so it has full dimension and equals connected H0. Hence the geometric points of the adjoint kernel and centre agree; Cartier makes both subgroup schemes smooth and reduced, so they agree as schemes, and the equality descends to k. Differentiating the adjoint kernel now gives Lie⁡Z(H0)=ker⁡ad⁡=Z(Lie⁡H0). Apply this to H0=H∘: its centre is characteristic in H∘, hence normal in G by step 3.1, and its Lie algebra is Z(h).

5.1F4F5step 4.1

Z(H∘) is finite: its identity component is a connected commutative, hence solvable, normal subgroup of G, so it is contained in R(G)=1 by [F5]; since Z(H∘) is smooth of dimension 0 in characteristic 0, its Lie algebra is zero.

6.1step 1.1step 1.2step 4.1step 5.1∎

Finally n⊆Z(h): for n∈n⊆h and x∈h one has [x,n]=0 by the definition of h. Hence n⊆Z(h)=Lie⁡(Z(H∘))=0, so n=0, and by step 1.1 the algebra g has no nonzero solvable ideal.

Remarks

  • The proof is Milne's argument in the paragraph before Lemma 22.39: a commutative ideal n has a centralizer h that is again an ideal. The identity component of Z(H∘) is a normal connected commutative subgroup of G, hence trivial; the full centre is finite, so its Lie algebra is zero in characteristic 0.
  • Characteristic 0 is used twice: Cartier's theorem for smoothness of H∘, Z(H∘) and G, and the Lie-normal-subgroup correspondence.

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