Bourbaki

Lemma 3

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

Integration, IX, p. 87, § 6. Promeasures and measures on a locally convex space

*For any t,t′t, t' in D,

∫Ω∣X(t+t′2)−X(t)+X(t′)2∣3dm=1(8π)1/2∣t−t′∣3/2. \int_\Omega \left| X\left( \frac{t + t'}{2} \right) - \frac{X(t) + X(t')}{2} \right|^3 dm = \frac{1}{(8\pi)^{1/2}} |t - t'|^{3/2}.
Note that t+t′2\frac{t + t'}{2} belongs to D. One knows (No. 6, Example 2) that the family (X(t))t∈D(X(t))_{t \in D} is a basis of the topological dual Ω′\Omega' of Ω\Omega; therefore there exists a symmetric bilinear form M^\widehat{M} on Ω′×Ω′\Omega' \times \Omega' characterized by M^(X(t),X(t′))=inf⁡(t,t′)\widehat{M}(X(t), X(t')) = \inf(t, t'). By construction, the variance of the Gaussian measure m on Ω\Omega is the quadratic form ξ↦M^(ξ,ξ)\xi \mapsto \widehat{M}(\xi, \xi) on Ω′\Omega'. Set, in particular,
ξ=X(t+t′2)−X(t)+X(t′)2; \xi = X\left( \frac{t + t'}{2} \right) - \frac{X(t) + X(t')}{2};
an easy calculation yields
M^(ξ,ξ)=∣t−t′∣4. \widehat{M}(\xi, \xi) = \frac{|t - t'|}{4}.

(2) Espace mesuré: a locally compact space equipped with a measure (Ch. III, 1st edn., §2, No. 2, p. 52).

By Prop. 6 of No. 5 (formula (16)),

∫Ω∣ξ∣3 dm=π−1/223/2Γ(2)M^(ξ,ξ)3/2; \int_{\Omega} |\xi|^3 \, dm = \pi^{-1/2} 2^{3/2} \Gamma(2) \widehat{M}(\xi, \xi)^{3/2};

the lemma follows immediately from formulas (40) and (41).

B) Construction of a mapping u of Ω\Omega into C\mathscr{C}: For every integer n⩾0n \geqslant 0, denote by EnE_n the subspace of C\mathscr{C} formed by the functions that are affine on each of the intervals [k−12n,k2n]\left[ \frac{k-1}{2^n}, \frac{k}{2^n} \right] for 1⩽k⩽2n1 \leqslant k \leqslant 2^n. An affine function on a compact interval I of R\mathbf{R} attains its bounds at the endpoints of I; consequently,

∥f∥=sup⁡1⩽k⩽2n∣f(k2n)∣ \|f\| = \sup_{1 \leqslant k \leqslant 2^n} \left| f\left( \frac{k}{2^n} \right) \right|

for f∈Enf \in E_n.

For every function g∈Ωg \in \Omega and every integer n⩾0n \geqslant 0, there exists one and only one function un(g)u_n(g) that belongs to EnE_n and coincides with gg at every point of DnD_n; we shall write Tng=un+1(g)−un(g)T_n g = u_{n+1}(g) - u_n(g). Since DnD_n is finite, the mapping TnT_n of Ω\Omega into C\mathscr{C} is continuous, hence mm-measurable.

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.