For any class γ of finite dimensional simple g-modules, let Uγ be the isotypical component of type γ of the g-module U (for the adjoint representation of g on U). Let γ0 be the class of the trivial g-module of dimension 1. Let [U,U] be the vector subspace of U generated by the brackets of pairs of elements of U.
(i) U is the direct sum of the Uγ.
(ii) Uγ0=Z, and ∑γ=γ0Uγ=[U,U].
(iii) Let u→u♮ be the projection of U onto Z defined by the decomposition U=Z⊕[U,U]. If u∈U and v∈U, we have (uv)♮=(vu)♮. If u∈U and z∈Z, we have (uz)♮=u♮z.
(iv) Let φ be the Harish-Chandra homomorphism. Let λ∈P++, and let E be a finite dimensional simple g-module of highest weight λ. For all u∈U, we have
dim E1 Tr(uE) =(φ(u♮))(λ).
The g-module U is a direct sum of finite dimensional submodules. This implies (i).
It is clear that Uγ0=Z. Let U′ be a vector subspace of U defining a subrepresentation of class γ of the adjoint representation. Then either [g,U′]=U′ or [g,U′]=0. Thus, if γ=γ0 then [g,U′]=U′, so ∑γ=γ0Uγ⊂[U,U]. On the other hand, if u∈U and x1,...,xn∈g, then
[x1...xn,u]=(x1...xnu−x2...xnux1)+(x2...xnux1−x3...xnux1x2)
+⋯+(xnux1...xn−1−ux1...xn)∈[g,U]
Hence [U,U]⊂[g,∑γUγ]=[g,∑γ=γ0Uγ]⊂∑γ=γ0Uγ. This proves (ii). Under these conditions, (iii) follows from Chap. I, §6, no. 9, Lemma 5.
Finally, let E,λ be as in (iv). Then
Tr(uE) = Tr((u♮)E) since u−u♮∈[U,U]
= Tr(φ(u♮)(λ).1) (§6, no.4, Prop.7)
= (dim E).φ(u♮)(λ).
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.
Nothing.