Bourbaki

Theorem 4

Tag 09T2, permanent. Cite it as [Bourbaki, Tag 09T2].

Integration, chapter IX, § 6. Promeasures and measures on a locally convex space

— Let E be a locally convex space. The Fourier transformation is a bijection of the set of promeasures on E onto the set of functions of positive type on E′E' whose restriction to every finite-dimensional subspace is continuous.

We know (No. 3, Prop. 3) that the Fourier transformation is injective. Let μ=(μV)V∈F(E)\mu = (\mu_V)_{V \in \mathscr{F}(E)} be a promeasure on E and Φ\Phi its Fourier transform. Let T be a finite-dimensional subspace of E′E' and let V be the orthogonal of T in E. One can identify T with the dual of E/VE/V; the restriction ΦT\Phi_T of Φ\Phi to T is the Fourier transform of the bounded measure μV\mu_V on E/VE/V. By Prop. 11, ΦT\Phi_T is continuous and of positive type on T. Since T is arbitrary, it is clear that Φ\Phi is of positive type on E′E'.

Conversely, let Φ\Phi be a function of positive type on E′E' whose restriction to every finite-dimensional subspace of E′E' is continuous. For every V∈F(E)V \in \mathscr{F}(E), we identify the dual of E/VE/V with the orthogonal V∘V^\circ of V in E′E'; the restriction ΦV\Phi_V of Φ\Phi to V∘V^\circ is continuous and of positive type and so, by Bochner's theorem, there exists a bounded (positive) measure μV\mu_V on E/VE/V whose Fourier transform is ΦV\Phi_V. Let V and W in F(E)\mathscr{F}(E) be such that W⊂VW \subset V, and let pVWp_{VW} be the canonical mapping of E/WE/W onto E/VE/V; with the identifications made, tpVW{}^t p_{VW} is the injection of V∘V^\circ into W∘W^\circ. By formula (4) of No. 3, we then have

F(pVW(μW))=(FμW)∘tpVW=ΦW∘tpVW=ΦV=FμV, \mathscr{F}(p_{VW}(\mu_W)) = (\mathscr{F}\mu_W) \circ {}^t p_{VW} = \Phi_W \circ {}^t p_{VW} = \Phi_V = \mathscr{F}\mu_V,

(*) This question will be studied in a forthcoming chapter of the Book Théories spectrales. The reader may consult for this subject the book of L.H. LOOMIS, Abstract harmonic analysis, Van Nostrand, New York, 1953.

whence pvw(μw)=μvpvw(\mu_w) = \mu_v by Prop. 3 of No. 3. Consequently, the family μ=(μv)v∈F(E)\mu = (\mu_v)_{v \in \mathscr{F}(E)} is a promeasure on EE; it is clear that Φ\Phi is the Fourier transform of μ\mu.

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.