Bourbaki

Exercise 13, § 5

Integration, IX, p. 116

Bourbaki marks this one as harder than the rest.

*Let G be a locally compact abelian group. One denotes by G^\widehat{G} the dual group of G and by α\alpha a Haar measure on G^\widehat{G}. For every bounded measure μ\mu on G, one denotes by Fμ\mathscr{F} \mu the Fourier transform of μ\mu, which is a function on the group G^\widehat{G} (cf. Théor. spec., Ch. II, §1, No. 2).

a) The Fourier transformation F\mathscr{F} is a continuous mapping of M+b(G)\mathscr{M}_+^b(G) equipped with the tight topology into Cb(G^)\mathscr{C}^b(\widehat{G}) equipped with the topology of compact convergence. (Make use of the Cor. of Prop. 13 of No. 6.)

b) Let F\mathscr{F} be a filter on M+b(G)\mathscr{M}_+^b(G) and Φ\Phi a bounded continuous function on G^\widehat{G}; assume that lim⁡λ,F(Fλ)⋅α=Φ⋅α\lim_{\lambda, \mathscr{F}} (\mathscr{F} \lambda) \cdot \alpha = \Phi \cdot \alpha (vague convergence) and lim⁡λ,F(Fλ)(0)=Φ(0)\lim_{\lambda, \mathscr{F}} (\mathscr{F} \lambda)(0) = \Phi(0). Show that the filter F\mathscr{F} converges tightly to a measure μ\mu such that Fμ=Φ\mathscr{F} \mu = \Phi (show by application of the Stone–Weierstrass theorem that the set of Fourier transforms of continuous functions on GG with compact support is a dense linear subspace of C0(G^)C^0(\widehat{G}) for uniform convergence; next observe that lim⁡λ,F∫(Fλ)⋅udα=∫Φudα\lim_{\lambda, \mathscr{F}} \int (\mathscr{F} \lambda) \cdot u d\alpha = \int \Phi u d\alpha for every u∈Eu \in E and that the filter F\mathscr{F} contains a vaguely compact set of bounded measures; deduce from this that the filter F\mathscr{F} has at most one cluster point, then that it converges tightly).

c) Let F\mathscr{F} be a filter on M+b(G)\mathscr{M}_+^b(G) having a countable base. In order that F\mathscr{F} converge tightly to a bounded positive measure μ\mu, it is necessary and sufficient that there exist a continuous function Φ\Phi on G^\widehat{G} such that Fλ\mathscr{F} \lambda converges pointwise to Φ\Phi with respect to F\mathscr{F}, in which case Fμ=Φ\mathscr{F} \mu = \Phi (P. Lévy’s theorem).

Solution

No solution has been written yet.

Transcribed from the printed volume. Not translated.