Bourbaki

Proposition 6

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

Integration, VIII, p. 32, § 4. Convolution of measures and functions

*Assume χ\chi a continuous multiplier and each function χ(s,⋅)\chi(s, \cdot) bounded. Let ρ(s)=sup⁡x∈Xχ(s−1,x)\rho(s) = \sup_{x \in X} \chi(s^{-1}, x). Let pp and qq be two conjugate exponents (1≤p<+∞1 \leq p < +\infty). Let μ∈Mρ1/q(G)\mu \in \mathscr{M}^{\rho^{1/q}}(G) and f∈Lp(X,β)2f \in L^p(X, \beta)^2 Then: (i) μ\mu and ff are convolvable; (ii) the convolution product μ∗βf\mu *^\beta f is given locally β\beta-almost everywhere by the formula (3), and is equal locally β\beta-almost everywhere to a function g∈Lp(X,β)g \in L^p(X, \beta) such that ∥g∥p≤∥μ∥ρ1/q∥f∥p\|g\|_p \leq \|\mu\|_{\rho^{1/q}} \|f\|_p; (iii) gg is equal to the element γχ(μ)f\gamma_\chi(\mu)f defined by the continuous representation γχ\gamma_\chi of GG in Lp(X,β)L^p(X, \beta).

We have

∫∗∥γχ(s)f∥pd∣μ∣(s)≤(∫∗ρ(s)1/qd∣μ∣(s))∥f∥p<+∞ \int^* \|\gamma_\chi(s)f\|_p d|\mu|(s) \leq \left( \int^* \rho(s)^{1/q} d|\mu|(s) \right) \|f\|_p < +\infty
by §2, No. 5, formula (5). On the other hand, the mapping s↦γχ(s)fs \mapsto \gamma_\chi(s)f of GG into Lp(X,β)L^p(X, \beta) is continuous (§2, No. 5, Prop. 9). Therefore this mapping is μ\mu-integrable. Let
g=∫G(γχ(s)f)dμ(s)∈Lp(X,β). g = \int_G (\gamma_\chi(s)f) d\mu(s) \in L^p(X, \beta).
We have ∥g∥p≤(∫ρ1/q(s)d∣μ∣(s))∥f∥p\|g\|_p \leq (\int \rho^{1/q}(s) d|\mu|(s)) \|f\|_p. Applying the preceding remarks to ∣f∣|f|, one sees that the mapping s↦εs∗∣f∣s \mapsto \varepsilon_s * |f| of GG into Lp(X,β)L^p(X, \beta) is μ\mu-integrable, therefore that, for every h∈H(X)h \in \mathscr{H}(X), the mapping s↦⟨h,εs∗(∣f∣⋅β)⟩s \mapsto \langle h, \varepsilon_s * (|f| \cdot \beta) \rangle is μ\mu-integrable. Prop. 7 of §1, No. 5 then proves that μ\mu and f⋅βf \cdot \beta are convolvable. Moreover,
∫Xg(x)h(x)dβ(x)=∫Gdμ(s)∫X(γχ(s)f)(x)h(x)dβ(x)=∫G⟨h,εs∗(f⋅β)⟩dμ(s), \int_X g(x)h(x) d\beta(x) = \int_G d\mu(s) \int_X (\gamma_\chi(s)f)(x)h(x) d\beta(x) = \int_G \langle h, \varepsilon_s * (f \cdot \beta) \rangle d\mu(s),
and this last integral is equal to ⟨h,μ∗(f⋅β)⟩\langle h, \mu * (f \cdot \beta) \rangle by Prop. 7 of §1, No. 5. One therefore sees that gg is a convolution product of μ\mu and ff. This convolution product is given locally β\beta-almost everywhere by (3), by Prop. 2 and the Remark that follows it.

2For a function ff, the expression " f∈Lp(X,β)f \in L^p(X, \beta) " is an abuse of notation signifying that, depending on the context, the symbol ff is to be interpreted either as a function defined β\beta-almost everywhere, or as the equivalence class of such a function for the relation of equality β\beta-almost everywhere. Thus f∈Lpf \in L^p can symbolize either f∈Lpf \in \mathscr{L}^p or f˙∈Lp\dot{f} \in L^p.

By an abuse of notation, it is often one of the functions gg of the statement that is denoted μ∗βf\mu *^\beta f, which permits writing

∥μ∗βf∥p≤∥μ∥ρ1/q∥f∥p. \| \mu *^\beta f \|_p \leq \| \mu \|_{\rho^{1/q}} \| f \|_p .

If XX is countable at infinity, this style of notation is, moreover, entirely justified.

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

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