Bourbaki

Lemma 2

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

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

Let G be a Lie group, U a symmetric open neighbourhood of e in G, E a complete normable space and ϕ:U2→E\phi : U^2 \to E an analytic mapping. For all g∈Ug \in U, let ωg\omega_g be the differential at the point g of the mapping h↦ϕ(g−1h)h \mapsto \phi(g^{-1}h). Then ω\omega is the restriction to U of the left invariant differential form on G whose value at e is deϕd_e \phi.

Clearly ωe=deϕ\omega_e = d_e \phi. For all g∈Ug \in U and all t∈Te(G)t \in T_e(G),

⟨ωg,Te(γ(g))t⟩=⟨dg(ϕ∘γ(g)−1),Te(γ(g))t⟩=⟨deϕ∘Tg(γ(g)−1),Te(γ(g))t⟩=⟨deϕ,t⟩ \langle \omega_g, T_e(\gamma(g))t \rangle = \langle d_g(\phi \circ \gamma(g)^{-1}), T_e(\gamma(g))t \rangle \\ = \langle d_e \phi \circ T_g(\gamma(g)^{-1}), T_e(\gamma(g))t \rangle = \langle d_e \phi, t \rangle

and hence ωg\omega_g is derived from deϕd_e \phi by Te(γ(g))T_e(\gamma(g)).

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

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Cites

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Transcribed from the printed volume. Not translated.