Bourbaki

Theorem 2

Tag 0AI8, permanent. Cite it as [Bourbaki, Tag 0AI8].

Lie Groups and Lie Algebras, chapter III, § 8. Lie groups over R or Qp

Let GG be a finite-dimensional Lie group over R\mathbf{R} or Qp\mathbf{Q}_p. Every closed subgroup of GG is a Lie subgroup of GG. More generally, let UU be a symmetric open neighbourhood of ee in GG and HH a non-empty closed subspace of UU such that the conditions x∈Hx \in H, y∈Hy \in H and xy−1∈Uxy^{-1} \in U imply xy−1∈Hxy^{-1} \in H. Then HH is a Lie subgroup germ of GG.

Let h\mathfrak{h} be the Lie subalgebra tangent to HH at ee (§ 4, no. 5, Definition 2). There exists a Lie subgroup germ H0H_0 of GG with Lie algebra h\mathfrak{h} and contained in HH. We prove that H0H_0 is open in HH with the topology induced by that on GG. This will prove that HH is an analytic submanifold of GG and will establish the theorem.

There exist a vector subspace k\mathfrak{k} supplementary to h\mathfrak{h} in L(G)L(G), symmetric open neighbourhoods V1,V2V_1, V_2 of zero in h\mathfrak{h} and k\mathfrak{k} respectively and an exponential mapping ϕ\phi of GG defined on V1+V2V_1 + V_2 and possessing the following properties:

(a) the mapping (a1,a2)↦ϕ(a1)ϕ(a2)(a_1, a_2) \mapsto \phi(a_1)\phi(a_2) is an analytic isomorphism of V1×V2V_1 \times V_2 onto an open subset VV of GG; (b) ϕ(V1)⊂H0\phi(V_1) \subset H_0; (c) V2⊂UV^2 \subset U.

We shall prove (and this will achieve the proof) that there exists an open neighbourhood V2′V'_2 of 0 in V2V_2 such that H∩(ϕ(V1)ϕ(V2′))=ϕ(V1)H \cap (\phi(V_1)\phi(V'_2)) = \phi(V_1).

Suppose that the assertion is false. Then we can find a sequence (xn)(x_n) in V1V_1 and a sequence (yn)(y_n) in V2−{0}V_2 - \{0\} tending to 0, such that ϕ(xn)ϕ(yn)∈H\phi(x_n)\phi(y_n) \in H for all nn. Then ϕ(yn)∈H\phi(y_n) \in H by (c).

If K=QpK = \mathbf{Q}_p, it can be assumed that V2V_2 is an additive subgroup of k\mathfrak{k} and that ϕ(pa)=ϕ(a)p\phi(pa) = \phi(a)^p for all a∈V2a \in V_2 and all p∈Zp \in \mathbf{Z}. Then ϕ(λy1)∈H\phi(\lambda y_1) \in H for all λ∈Z\lambda \in \mathbf{Z} and hence by continuity for all λ∈Zp\lambda \in \mathbf{Z}_p. The mapping f:λ↦ϕ(λy1)f : \lambda \mapsto \phi(\lambda y_1) of Zp\mathbf{Z}_p into GG is analytic and takes its values in HH and (T0f)(1)=y1(T_0f)(1) = y_1. Hence y1∈hy_1 \in \mathfrak{h}, which is absurd. The theorem is therefore established in the case of Qp\mathbf{Q}_p.

If K=RK = \mathbf{R}, it can be assumed that V2V_2 is connected and that yny_n belongs to 12V2−{0}\frac{1}{2}V_2 - \{0\}. By taking a subsequence of (yn)(y_n) if necessary, we can find a sequence (λn)(\lambda_n) of non-zero scalars such that λn−1yn\lambda_n^{-1}y_n tends to an element yy of V2−{0}V_2 - \{0\}. The sequence (λn)(\lambda_n) tends to 0. Let λ∈R\lambda \in \mathbf{R} be such that λy∈12V2\lambda y \in \frac{1}{2}V_2; we prove that exp⁡(λy)∈H\exp(\lambda y) \in H. It can be assumed that λλn−1yn∈12V2\lambda \lambda_n^{-1}y_n \in \frac{1}{2}V_2 for all nn. Let kn∈Zk_n \in \mathbf{Z} be such that ∣λ−knλn∣|\lambda - k_n \lambda_n| tends to 0. For nn sufficiently large, (λ−knλn)λn−1yn∈12V2(\lambda - k_n \lambda_n)\lambda_n^{-1}y_n \in \frac{1}{2}V_2 and hence knyn∈12V2k_n y_n \in \frac{1}{2}V_2. Hence exp⁡(hyn)∈H\exp(h y_n) \in H for hh an integer and 0≤∣h∣≤∣kn∣0 \leq |h| \leq |k_n| (as is seen by induction on ∣h∣|h|). Then

exp⁡(λy)=lim⁡n→∞exp⁡(λλn−1yn)=lim⁡n→∞(exp⁡((λ−knλn)λn−1yn)exp⁡(knyn))=lim⁡n→∞exp⁡knyn∈H. \exp(\lambda y) = \lim_{n \to \infty} \exp(\lambda \lambda_n^{-1}y_n) = \lim_{n \to \infty} (\exp((\lambda - k_n \lambda_n)\lambda_n^{-1}y_n) \exp(k_n y_n)) = \lim_{n \to \infty} \exp k_n y_n \in H.

Hence the mapping f:λ↦exp⁡λyf : \lambda \mapsto \exp \lambda y, where λy∈14V2\lambda y \in \frac{1}{4}V_2, takes its values in HH and (T0f)(1)=y(T_0f)(1) = y. Hence y∈hy \in \mathfrak{h}, which is absurd. The theorem is thus established in the case of R\mathbf{R}.

Theorem 2 is no longer true if GG is not assumed to be finite-dimensional (Exercise 12).

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

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Transcribed from the printed volume. Not translated.