Bourbaki

Lemma 6

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

Lie Groups and Lie Algebras, chapter III, § 4. Passage from Lie algebras to Lie groups

Let GG be a Lie group germ, ω\omega the canonical left differential form of GG (§ 3, no. 18.9), MM a manifold of class CrC^r (r≥2r \geq 2) and α\alpha a differential form of class Cr−1C^{r-1} and degree 1 on MM with values in L(G)L(G).

(i) The elements of T(M×G)T(M \times G) at which the differential form

θ=pr1∗α−pr2∗ω \theta = \mathrm{pr}_1^*\alpha - \mathrm{pr}_2^*\omega
is zero constitute a vector subbundle SS of T(M×G)T(M \times G) of class Cr−1C^{r-1}.

(ii) For all (x,g)∈M×G(x, g) \in M \times G, T(pr1)∣S(x,g)T(\mathrm{pr}_1)|S_{(x, g)} is an isomorphism of S(x,g)S_{(x, g)} onto Tx(M)T_x(M).

(iii) If dα+[α]2=0d\alpha + [\alpha]^2 = 0 (cf. § 3, no. 14) the vector subbundle SS is integrable.

If (x,g)∈M×G(x, g) \in M \times G and (u,v)∈Tx(M)×Tg(G)(u, v) \in T_x(M) \times T_g(G), then

θ(x,g)(u,v)=α(u)−g−1v. \theta_{(x, g)}(u, v) = \alpha(u) - g^{-1}v.
Hence the kernel of θ(x,g)\theta_{(x, g)} is the set S(x,g)S_{(x, g)} of (u,gα(u))(u, g\alpha(u)) for u∈Tx(M)u \in T_x(M), whence (ii). We consider T(M×G)T(M \times G) as the direct sum of two vector bundles FF and F′F' with F(x,g)=Tx(M)×{0}F_{(x, g)} = T_x(M) \times \{0\} and F(x,g)′={0}×Tg(G)F'_{(x, g)} = \{0\} \times T_g(G) for all
(x,g)∈M×G. (x, g) \in M \times G.
For u∈Tx(M)×{0}u \in T_x(M) \times \{0\}, we write ϕ(u)=(0,gα(u))\phi(u) = (0, g\alpha(u)). Using the left trivialization of T(G)T(G), it is seen that ϕ\phi is a morphism of FF into F′F', whence (i) (Lemma 5). Finally, if dα+[α]2=0d\alpha + [\alpha]^2 = 0, then
dθ=pr1∗(dα)−pr2∗(dω)=−12(pr1∗α∧pr1∗α−pr2∗ω∧pr2∗ω)=−12(pr1∗α−pr2∗ω)∧(pr1∗α+pr2∗ω)=−12θ∧(pr1∗α+pr2∗ω) \begin{align*} d\theta &= \mathrm{pr}_1^*(d\alpha) - \mathrm{pr}_2^*(d\omega) \\ &= -\frac{1}{2}(\mathrm{pr}_1^*\alpha \wedge \mathrm{pr}_1^*\alpha - \mathrm{pr}_2^*\omega \wedge \mathrm{pr}_2^*\omega) \\ &= -\frac{1}{2}(\mathrm{pr}_1^*\alpha - \mathrm{pr}_2^*\omega) \wedge (\mathrm{pr}_1^*\alpha + \mathrm{pr}_2^*\omega) \\ &= -\frac{1}{2}\theta \wedge (\mathrm{pr}_1^*\alpha + \mathrm{pr}_2^*\omega) \end{align*}
and hence SS is integrable (Differentiable and Analytic Manifolds, R, 9.3.6).

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

Cited by

Cites

Transcribed from the printed volume. Not translated.