Bourbaki

Proposition 24

Tag 0AA9, permanent. Cite it as [Bourbaki, Tag 0AA9].

Lie Groups and Lie Algebras, chapter III, § 3. Passage from a Lie group to its Lie algebra

Let G be a Lie group and (U,ϕ,E)(U, \phi, E) a chart on G such that ϕ(e)=0\phi(e) = 0. Let V be an open neighbourhood of e such that V2⊂UV^2 \subset U. Let m be the analytic mapping (a,b)↦ϕ(ϕ−1(a)ϕ−1(b))(a, b) \mapsto \phi(\phi^{-1}(a)\phi^{-1}(b)) of ϕ(V)×ϕ(V)\phi(V) \times \phi(V) into E. Let

m=∑i,j≥0mi,j m = \sum_{i, j \geq 0} m_{i, j}

be the expansion of m as an integral series about (0, 0), where mi,jm_{i,j} is a bihomogeneous continuous-polynomial of bidegree (i,j)(i, j) on E×EE \times E with values in EE.

(i) mi,0=m0,j=0m_{i,0} = m_{0,j} = 0 for all i≠1i \neq 1 and j≠1j \neq 1. (ii) m1,0(a,b)=am_{1,0}(a, b) = a and m0,1(a,b)=bm_{0,1}(a, b) = b for all a∈E,b∈Ea \in E, b \in E. (iii) *Let ψ:Te(G)→E\psi : T_e(G) \to E be the differential of ϕ\phi at e. For all u,vu, v in Te(G)T_e(G),

ψ([u,v])=m1,1(ψ(u),ψ(v))−m1,1(ψ(v),ψ(u)). \psi([u, v]) = m_{1,1}(\psi(u), \psi(v)) - m_{1,1}(\psi(v), \psi(u)).

m(a,0)=a, m(0,b)=bm(a, 0) = a,\ m(0, b) = b for all a,ba, b in ϕ(V)\phi(V), which proves (i) and (ii). Let u,vu, v be in Te(G)T_e(G). Let T0(E)T_0(E) be identified with EE and hence ψ\psi with Te(ϕ)T_e(\phi): The images of uu and vv under Te(ϕ)T_e(\phi) are ψ(u)\psi(u) and ψ(v)\psi(v). The tensor product point distribution of these images is the symmetric product of (ψ(u),0)(\psi(u), 0) and (0,ψ(v))(0, \psi(v)) in TS(E×E)=TS(E)×TS(E)TS(E \times E) = TS(E) \times TS(E), that is

(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0). (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0).

Hence ϕ∗(u∗v)\phi * (u * v) is the image of the above element under the mapping mm of ϕ(V)×ϕ(V)\phi(V) \times \phi(V) into EE. Its component of degree 1 in TS(E)TS(E) is, by Lemma 1,

x=⟨m1,1,(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0)⟩. x = \langle m_{1,1}, (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0) \rangle.

We define a bilinear mapping n:(E×E)2→En : (E \times E)^2 \to E by

n((a,b),(a′,b′))=m1,1(a,b′). n((a, b), (a', b')) = m_{1,1}(a, b').

Then n((a,b),(a,b))=m1,1(a,b)n((a, b), (a, b)) = m_{1,1}(a, b) and hence

x=⟨n,(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0)⟩=m1,1(ψ(u),ψ(v))+m1,1(0,0)=m1,1(ψ(u),ψ(v)). x = \langle n, (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0) \rangle \\ = m_{1,1}(\psi(u), \psi(v)) + m_{1,1}(0, 0) = m_{1,1}(\psi(u), \psi(v)).

Similarly, ϕ∗(v∗u)\phi * (v * u) admits m1,1(ϕ(v),ϕ(u))m_{1,1}(\phi(v), \phi(u)) as component of degree 1 in TS(E)TS(E). As ϕ([u,v])\phi([u, v]) is of degree 1, this proves (iii).

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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