Bourbaki

Proposition 13

Tag 093G, permanent. Cite it as [Bourbaki, Tag 093G].

Integration, V, p. 54, § 5. Measures defined by numerical densities

In order that two complex measures ρ\rho and σ\sigma on TT be alien to each other, it is necessary and sufficient that there exist in TT two disjoint sets RR and SS such that ρ\rho is concentrated on RR and σ\sigma on SS; RR and SS may be taken to be universally measurable.

Set μ=∣ρ∣\mu = |\rho|, ν=∣σ∣\nu = |\sigma|, λ=μ+ν\lambda = \mu + \nu; since μ\mu and ν\nu are bounded above by λ\lambda, there exist two locally λ\lambda-integrable functions uu and vv (which one can suppose to be universally measurable by §3, No. 4, Prop. 7) such that μ=u⋅λ\mu = u \cdot \lambda, ν=v⋅λ\nu = v \cdot \lambda. Then

inf⁡(∣ρ∣,∣σ∣)=inf⁡(μ,ν)=inf⁡(u,v)⋅λ \inf(|\rho|, |\sigma|) = \inf(\mu, \nu) = \inf(u, v) \cdot \lambda

(No. 2, Cor. of Prop. 2). Let AA (resp. BB) be the set of t∈Tt \in T such that u(t)>0u(t) > 0 and v(t)=0v(t) = 0 (resp. u(t)=0u(t) = 0 and v(t)>0v(t) > 0). If ρ\rho and σ\sigma are alien, then inf⁡(u,v)=0\inf(u, v) = 0 locally λ\lambda-almost everywhere (No. 3, Cor. 2 of Prop. 3), so that the disjoint universally measurable sets AA and BB carry μ\mu and ν\nu, respectively. Conversely, suppose that μ\mu and ν\nu are carried, respectively, by disjoint sets RR and SS; φR\varphi_R is measurable for the measure μ=u⋅λ\mu = u \cdot \lambda, and μ=φR⋅μ\mu = \varphi_R \cdot \mu. By Prop. 8 of No. 4, the function u′=uφRu' = u \varphi_R is λ\lambda-measurable, and μ=u′⋅λ\mu = u' \cdot \lambda. Similarly, if v′=vφSv' = v \varphi_S then ν=v′⋅λ\nu = v' \cdot \lambda; one concludes by remarking that inf⁡(u′,v′)=0\inf(u', v') = 0 (No. 2, Cor. of Prop. 2).

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.