Bourbaki

Lemma 6

Tag 03EZ, permanent. Cite it as [Bourbaki, Tag 03EZ].

Théories spectrales, chapter V, § 4. Représentations des groupes compacts

Let qq be a non-degenerate bilinear form on a finite-dimensional complex vector space E of dimension ⩾3\geqslant 3.

a) If qq is symmetric, then the adjoint representation of the orthogonal Lie algebra so(q)\mathfrak{s}\mathfrak{o}(q) is isomorphic to the exterior square ∧2E\wedge^2E of the natural representation so(q)→gl(E)\mathfrak{s}\mathfrak{o}(q)\rightarrow \mathfrak{g}\mathfrak{l}(E);

b) If qq is alternating, then the adjoint representation of the symplectic Lie algebra sp(q)\mathfrak{s}\mathfrak{p}(q) is isomorphic to the symmetric square S2(E)\mathsf{S}^2(E) of the natural representation sp(q)→gl(E)\mathfrak{s}\mathfrak{p}(q)\rightarrow \mathfrak{g}\mathfrak{l}(E).

Let C\mathbf{C} be provided with the identical involutive automorphism. The bilinear form qq is then ε\varepsilon-Hermitian (A, IX, § 3, no1^o1, Def. 1) with ε=1\varepsilon = 1 in case a) and ε=−1\varepsilon =-1 in case b). For every u∈u\in End(E), let tu^tu denote the adjoint of uu with respect to qq. Thus one has q(x,u(y))=q(tu(x),y)q(x, u(y)) =q(^tu(x), y) for every (x,y)∈E×E(x, y)\in E\times E. Let vv denote the unique automorphism of E⊗EE\otimes E such that v(x⊗y)=y⊗xv(x\otimes y) =y\otimes x for every (x,y)∈E2(x, y)\in E^2.

There exists a unique linear mapping ww of E⊗EE\otimes E into End(E) such that w(a⊗b)w(a\otimes b) is the linear mapping defined by x↦q(a,x)bx\mapsto q(a, x)b for every (a,b,x)∈E3(a, b, x)\in E^3. The mapping ww is an isomorphism. For every s∈E⊗Es\in E\otimes E, one has

t(w(s))=εw(v(s))(3) t(w(s)) =\varepsilon w(v(s)) \tag{3}

In fact, for all (x,y)(x, y) and (a,b)(a, b) in E×EE\times E, there follows

q(x,w(a⊗b)y)=q(a,y)q(x,b)=εq(b,x)q(a,y)=q(εw(b⊗a)x,y) q(x, w(a\otimes b)y) =q(a, y)q(x, b) =\varepsilon q(b, x)q(a, y) =q(\varepsilon w(b\otimes a)x, y)

Finally, denote by x↦x∗x\mapsto x^* the isomorphism of E onto E′E' deduced from qq, that is to say such that ⟨x∗,y⟩=q(x,y)\langle x^*, y\rangle =q(x, y) for every (x,y)∈E2(x, y)\in E^2.

With these notations established, let H be the orthogonal group (resp. symplectic) of qq. It is a Lie subgroup of GL(E)\mathbf{G}\mathbf{L}(E) whose Lie algebra h\mathfrak{h} is the subspace of End(E) consisting of the u∈u\in End(E) such that tu=−u^tu=-u (LIE, III, p. 146, cor. 1). Since the form qq is H-invariant, we have

⟨(ga)∗,b⟩=q(ga,b)=⟨a,g−1b⟩ \langle (ga)^*, b\rangle =q(ga, b) =\langle a, g^{-1}b\rangle

for every g∈Hg\in H and every (a,b)∈E×E(a, b)\in E\times E.

Equip End(E) with the adjoint representation Ad of H. The linear mapping ww is a morphism of representations of H: in fact, for every g∈Hg\in H and every (a,b,x)∈E3(a, b, x)\in E^3, we have

w(g(a⊗b))(x)=⟨(ga)∗,x⟩gb=⟨a,g−1x⟩gb w(g(a\otimes b))(x) =\langle (ga)^*, x\rangle gb=\langle a, g^{-1}x\rangle gb

=g(⟨a,g−1x⟩b)==g(\langle a, g^{-1}x\rangle b) = Ad(gg)(w(a⊗b))x(w(a\otimes b))x,

whence the conclusion by linearity.

Since vv is likewise a morphism of representations of H, the same is true of the linear mapping θ=w−εw∘v\theta =w-\varepsilon w\circ v; the latter is therefore a morphism of h\mathfrak{h}-modules.

Let F ⊂E⊗E\subset E\otimes E be the subspace of elements s∈E⊗Es\in E\otimes E such that v(s)=−εsv(s) =-\varepsilon s. If ε=−1\varepsilon =-1, the restriction to F of the canonical mapping of E⊗EE\otimes E into the symmetric square of E is an isomorphism of C\mathbf{C}-vector spaces (A, III, p. 72); if ε=1\varepsilon = 1, the restriction to F of the canonical mapping of E⊗EE\otimes E into the exterior square of E is an isomorphism of C\mathbf{C}-vector spaces (loc. cit., p. 82).

The image of F under θ\theta is contained in h:\mathfrak{h}: in fact, for every s∈Fs\in F, formula (3) implies

tθ(s)=tw(s)−εtw(v(s))=εw(v(s))−w(s)=−θ(s) ^t\theta (s) =^tw(s)-\varepsilon^tw(v(s)) =\varepsilon w(v(s))-w(s) =-\theta (s)

By definition of F, the restriction of the mapping θ\theta to F coincides with that of 2w2w and the linear mapping θ\theta is therefore injective on F. Since dim(F) = dim(h\mathfrak{h}) (A, III, p. 75, th. 1 and p. 87, cor. 1 and LIE, VIII, p. 192 and p. 201), one concludes that θ\theta induces by passing to the subspaces an isomorphism of h\mathfrak{h}-modules of F onto h\mathfrak{h}, whence the lemma.

Bourbaki sets the proof directly after the statement, and the corpus does not separate them, so what is above is the statement and its proof together.

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Machine translation of the English, by gpt-5.4, against glossary version 34. Not checked by a person.