Bourbaki

Example

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

Integration, chapter V, § 5. Measures defined by numerical densities

— Lebesgue measure on R\mathbf{R} is diffuse (Ch. IV, §1, No. 3, Remark 1).

To say that θ\theta is a diffuse measure on TT amounts to saying that every set with finite complement carries ∣θ∣|\theta|, or again that ∣θ∣|\theta| is alien to every point measure. The diffuse measures therefore form a band in M(T)\mathscr{M}(T) (Ch. II, §1, No. 5, Th. 1).

Recall (Ch. III, §1, No. 3) that a complex measure ρ\rho on TT is said to be atomic if it is of the form ∑t∈Tα(t)εt\sum_{t \in T} \alpha(t) \varepsilon_t, where α\alpha is a complex function on TT such that ∑t∈K∣α(t)∣<+∞\sum_{t \in K} |\alpha(t)| < +\infty for every compact subset KK of TT, which expresses that the family (α(t)εt)t∈T(\alpha(t) \varepsilon_t)_{t \in T} is summable (§2, No. 1, Remark 2). It then follows from the remark following Cor. 3 of Th. 2 of No. 5 that ∣ρ∣=∑t∈T∣α(t)∣εt|\rho| = \sum_{t \in T} |\alpha(t)| \varepsilon_t. The function α\alpha that occurs in these formulas is uniquely determined, because α(t)=ρ({t})\alpha(t) = \rho(\{t\}). An atomic measure and a diffuse measure are alien to each other.

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

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Cites

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