Bourbaki

Exercise 7, § 4

Lie Groups and Lie Algebras, III, 378

Bourbaki marks this one as harder than the rest.

(a) Let (λ,x)↦λ.x(\lambda, x) \mapsto \lambda.x be a law of continuous left operation of R\mathbf{R} on T\mathbf{T}. Then one of the two following holds: (1) either there exists a fixed point and the stabilizer of every point is either R\mathbf{R} or {0}\{0\}; (2) or there exists a point whose stabilizer is an infinite discrete subgroup of R\mathbf{R} and R\mathbf{R} operates transitively on T\mathbf{T}. (If {λ∈R∣λ.x=x}={0}\{\lambda \in \mathbf{R} | \lambda.x = x\} = \{0\}, the orbit of xx is homeomorphic to R\mathbf{R} and has frontier points lim⁡λ→+∞λ.x\lim_{\lambda \to +\infty} \lambda.x which are fixed. If {λ∈R∣λ.x=x}=Za\{\lambda \in \mathbf{R} | \lambda.x = x\} = \mathbf{Z}a with a≠0a \neq 0, the orbit of xx is homeomorphic to T\mathbf{T} and R\mathbf{R} is transitive.)

(b) If ff is a homeomorphism of T\mathbf{T} onto itself and kk an integer ⩾1\geqslant 1, a point x∈Tx \in \mathbf{T} is called periodic of period kk for ff if fk(x)=xf^k(x) = x and fh(x)≠xf^h(x) \neq x for 1⩽h<k1 \leqslant h < k. In the notation of (a), let fλf_\lambda be the homeomorphism x↦λ.xx \mapsto \lambda.x. Then the set of periodic points of period k>1k > 1 for fλf_\lambda is empty or equal to T\mathbf{T}. (If there exists a periodic point of period k>1k > 1 for fλf_\lambda, its stabilizer is distinct from {0}\{0\} and R\mathbf{R}, hence R\mathbf{R} operates transitively on T\mathbf{T} and all the points of T\mathbf{T} are periodic of period kk for fλf_\lambda.)

(c) Let Ω\Omega be a neighbourhood of ee in Diff∞(T)\mathrm{Diff}^\infty(\mathbf{T}) (Differentiable and Analytic Manifolds, R, 15.3.8, Note (1)). There exist an integer k>1k > 1 and f∈Ωf \in \Omega without fixed point such that the set of periodic points of period kk for ff is neither empty nor equal to T\mathbf{T}. (Let p:R→Tp : \mathbf{R} \to \mathbf{T} be the canonical mapping. Let ρ\rho be the mapping p(x)↦p(x+2πk)p(x) \mapsto p\left(x + \frac{2\pi}{k}\right) of T\mathbf{T} into T\mathbf{T}. Let Ω′\Omega' be a neighbourhood of ee in Diff∞(T)\mathrm{Diff}^\infty(\mathbf{T}) such that Ω′2⊂Ω{\Omega'}^2 \subset \Omega. For sufficiently large kk, ρ∈Ω′\rho \in \Omega'. On the other hand, let σ\sigma be a mapping of T\mathbf{T} into T\mathbf{T} such that σ(y)=y\sigma(y) = y for

y∉p(]0,2πk[) y \notin p\left(]0, \frac{2\pi}{k}[\right)
and σ(p(x))=p(x+λ(x))\sigma(p(x)) = p(x + \lambda(x)) for x∈]0,2πk[x \in ]0, \frac{2\pi}{k}[, where
0<λ(x)<2πk−x; 0 < \lambda(x) < \frac{2\pi}{k} - x;
can be chosen such that σ∈Ω′\sigma \in \Omega'. Then f=ρ∘σf = \rho \circ \sigma has the required properties.)

Such an ff cannot, by (b), be in the image of a continuous morphism of R\mathbf{R} into Diff∞(T)\mathrm{Diff}^\infty(\mathbf{T}).

(d) Let YY be a compact differentiable manifold of dimension ⩾1\geqslant 1. Every neighbourhood of ee in Diff∞(Y)\mathrm{Diff}^\infty(Y) contains an element hh with the following property: hh belongs to the image of no continuous morphism of R\mathbf{R} into Diff0(Y)\mathrm{Diff}^0(Y). (The manifold YY contains an open submanifold of the form T×D\mathbf{T} \times D, where DD is the open Euclidean ball of radius 1 and centre 0 in Rn\mathbf{R}^n (n=dim⁡Y−1n = \dim Y - 1). Let g∈Diff∞(D)g \in \mathrm{Diff}^\infty(D) be such that g(0)=0g(0) = 0, ∥g(x)∥>∥x∥\|g(x)\| > \|x\| for 0<∥x∥<120 < \|x\| < \frac{1}{2} and g(x)=xg(x) = x for ∥x∥⩾12\|x\| \geqslant \frac{1}{2} and gg very close to ee in Diff∞(D)\mathrm{Diff}^\infty(D). Let ff be as in (c), and, for 0<t<10 < t < 1, let ft:T→Tf_t : \mathbf{T} \to \mathbf{T} be defined as follows: for x∈Tx \in \mathbf{T}, y∈p−1(x)y \in p^{-1}(x), z∈p−1(f(x))z \in p^{-1}(f(x)) and ∣z−y∣<π|z - y| < \pi, we write ft(x)=p(ty+(1−t)z)f_t(x) = p(ty + (1 - t)z). Then there exists h∈Diff∞(Y)h \in \mathrm{Diff}^\infty(Y) such that h(x,y)=(f2∥y∥(x),g(y))h(x, y) = (f_{2\|y\|}(x), g(y)) for x∈Tx \in \mathbf{T}, y∈Dy \in D and h(u)=uh(u) = u for u∈Y−(T×D)u \in Y - (\mathbf{T} \times D); moreover, we can choose ff and gg such that hh is arbitrarily close to ee in Diff∞(Y)\mathrm{Diff}^\infty(Y). The points of T×{0}\mathbf{T} \times \{0\} are the y∈Yy \in Y such that when nn tends to +∞+\infty, hkn(x)h^{kn}(x) tends to a point not fixed under hh (in fact it is periodic of period kk). Therefore, every homeomorphism of YY onto YY which commutes with hh leaves T×{0}\mathbf{T} \times \{0\} invariant. Then apply (c).)

(e) Let YY be a compact differentiable manifold of dimension ⩾1\geqslant 1. There do not exist a Lie group GG and continuous morphisms Diff∞(Y)→G\mathrm{Diff}^\infty(Y) \to G, G→Diff0(Y)G \to \mathrm{Diff}^0(Y) whose composition is the canonical injection of Diff∞(Y)\mathrm{Diff}^\infty(Y) into Diff0(Y)\mathrm{Diff}^0(Y). (Use (d).)

Solution

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