Bourbaki

Lemma 3

Tag 08OQ, permanent. Cite it as [Bourbaki, Tag 08OQ].

Integration, chapter III, § 4. Products of measures

— Let F be the set of functions f∈C(X;C)f \in \mathscr{C}(X; \mathbf{C}) having the following property: there exist an α∈I\alpha \in I and a function fα∈C(Xα;C)f_\alpha \in \mathscr{C}(X_\alpha; \mathbf{C}) such that f=fα∘pαf = f_\alpha \circ p_\alpha. Then F is a dense linear subspace of C(X;C)\mathscr{C}(X; \mathbf{C}).

We note first of all that if g=gβ∘pβg = g_\beta \circ p_\beta and h=hγ∘pγh = h_\gamma \circ p_\gamma, where gβ∈C(Xβ;C)g_\beta \in \mathscr{C}(X_\beta; \mathbf{C}) and hγ∈C(Xγ;C)h_\gamma \in \mathscr{C}(X_\gamma; \mathbf{C}), then there exists an α∈I\alpha \in I such that α≥β\alpha \geq \beta and α≥γ\alpha \geq \gamma, and therefore pβ=pβα∘pαp_\beta = p_{\beta \alpha} \circ p_\alpha, pγ=pγα∘pαp_\gamma = p_{\gamma \alpha} \circ p_\alpha, which shows that

g+h=(gβ∘pβα+hγ∘pγα)∘pα g + h = (g_\beta \circ p_{\beta \alpha} + h_\gamma \circ p_{\gamma \alpha}) \circ p_\alpha
belongs to F; one sees similarly that gh∈Fgh \in F; F is thus a C-subalgebra of C(X;C)\mathscr{C}(X; \mathbf{C}), which contains the constants and is such that the relation f∈Ff \in F implies f‾∈F\overline{f} \in F. Finally, if x≠yx \neq y are two points of X, there exists an α∈I\alpha \in I such that pα(x)≠pα(y)p_\alpha(x) \neq p_\alpha(y), therefore there is a function fα∈C(Xα;C)f_\alpha \in \mathscr{C}(X_\alpha; \mathbf{C}) such that fα(pα(x))≠fα(pα(y))f_\alpha(p_\alpha(x)) \neq f_\alpha(p_\alpha(y)). The conclusion therefore follows from the Stone–Weierstrass theorem (GT, X, §4, No. 4, Prop. 7).

The lemma having been established, let μ,μ′\mu, \mu' be two measures on X such that (pα)∗(μ)=(pα)∗(μ′)(p_\alpha)_*(\mu) = (p_\alpha)_*(\mu') for all α∈I\alpha \in I; this means that, for every α∈I\alpha \in I and every function fα∈C(Xα;C)f_\alpha \in \mathscr{C}(X_\alpha; \mathbf{C}), we have

⟨fα,(pα)∗(μ)⟩=⟨fα,(pα)∗(μ′)⟩, \langle f_\alpha, (p_\alpha)_*(\mu) \rangle = \langle f_\alpha, (p_\alpha)_*(\mu') \rangle,
that is, ⟨fα∘pα,μ⟩=⟨fα∘pα,μ′⟩\langle f_\alpha \circ p_\alpha, \mu \rangle = \langle f_\alpha \circ p_\alpha, \mu' \rangle; in other words, μ\mu and μ′\mu' coincide on the subspace F of C(X;C)\mathscr{C}(X; \mathbf{C}), which is dense by Lemma 3, therefore μ=μ′\mu = \mu', which proves (i).

(ii) The relation (15) applied to pαp_\alpha shows that if μ\mu is the inverse limit of the inverse system (μα)(\mu_\alpha), necessarily

∥μ∥≥∥μα∥ \| \mu \| \geq \| \mu_\alpha \|
for all α∈I\alpha \in I.

(iii) Suppose the pαβp_{\alpha \beta} are surjective; one knows that the same is then true of the pαp_\alpha (GT, I, §9, No. 6, Prop. 8). Consider an inverse system of measures (μα)(\mu_\alpha) and let us first show that there exists a linear form λ\lambda on F (in the notations of Lemma 3) such that, for every α∈I\alpha \in I and every fα∈C(Xα;C)f_\alpha \in \mathscr{C}(X_\alpha; \mathbf{C}), λ(fα∘pα)=μα(fα)\lambda(f_\alpha \circ p_\alpha) = \mu_\alpha(f_\alpha). To that end, let β,γ\beta, \gamma be two indices in I, and fβ∈C(Xβ;C)f_\beta \in \mathscr{C}(X_\beta; \mathbf{C}), fγ∈C(Xγ;C)f_\gamma \in \mathscr{C}(X_\gamma; \mathbf{C}) two functions such that fβ∘pβ=fγ∘pγf_\beta \circ p_\beta = f_\gamma \circ p_\gamma; then there exists an index α∈I\alpha \in I such that α≥β\alpha \geq \beta and α≥γ\alpha \geq \gamma, therefore

pβ=pβα∘pα, pγ=pγα∘pαand(fβ∘pβα)∘pα=(fγ∘pγα)∘pα; p_\beta = p_{\beta \alpha} \circ p_\alpha ,\ p_\gamma = p_{\gamma \alpha} \circ p_\alpha \quad \text{and} \quad (f_\beta \circ p_{\beta \alpha}) \circ p_\alpha = (f_\gamma \circ p_{\gamma \alpha}) \circ p_\alpha ;

since pαp_\alpha is surjective, this implies fβ∘pβα=fγ∘pγαf_\beta \circ p_{\beta \alpha} = f_\gamma \circ p_{\gamma \alpha}, therefore

μα(fβ∘pβα)=μα(fγ∘pγα); \mu_\alpha(f_\beta \circ p_{\beta \alpha}) = \mu_\alpha(f_\gamma \circ p_{\gamma \alpha});

but by definition the last relation may also be written μβ(fβ)=μγ(fγ)\mu_\beta(f_\beta) = \mu_\gamma(f_\gamma), whence our assertion.

This being so, suppose that there exists a finite number a>0a > 0 such that ∥μα∥≤a\| \mu_\alpha \| \leq a for all α∈I\alpha \in I; then, for every function fα∈C(Xα;C)f_\alpha \in \mathscr{C}(X_\alpha; \mathbf{C}),

∣λ(fα∘pα)∣=∣μα(fα)∣≤a∥fα∥=a∥fα∘pα∥ |\lambda(f_\alpha \circ p_\alpha)| = |\mu_\alpha(f_\alpha)| \leq a \| f_\alpha \| = a \| f_\alpha \circ p_\alpha \|

since pαp_\alpha is surjective. This shows that the linear form λ\lambda is continuous on FF, and it follows from Lemma 3 that λ\lambda may be extended to a measure μ\mu on XX such that (pα)∗(μ)=μα(p_\alpha)_*(\mu) = \mu_\alpha for all α∈I\alpha \in I, which proves (iii).

(iv) To prove the existence of μ\mu it suffices, by (iii), to verify that the family of norms (∥μα∥)(\| \mu_\alpha \|) is bounded. But ∥μα∥=μα(1)\| \mu_\alpha \| = \mu_\alpha(1) and, when α≤β\alpha \leq \beta, the relation μα=(pαβ)∗(μβ)\mu_\alpha = (p_{\alpha \beta})_*(\mu_\beta) implies that μα(1)=μβ(1)\mu_\alpha(1) = \mu_\beta(1); since II is directed, the total masses of all the measures μα\mu_\alpha are therefore equal, whence our assertion. Moreover, the subspace FF obviously satisfies the property (P) of §1, No. 7, Prop. 9, therefore the inverse limit measure μ\mu of (μα)(\mu_\alpha) is positive. Finally, the relation μα=(pα)∗(μ)\mu_\alpha = (p_\alpha)_*(\mu) shows as above that μ(1)=μα(1)\mu(1) = \mu_\alpha(1).

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

Cited by

Cites

  • I, §9, No. 6, Prop. 8 not yet on this site
  • X, §4, No. 4, Prop. 7 not yet on this site
  • §1, No. 7, Prop. 9
Transcribed from the printed volume. Not translated.