Bourbaki

Theorem 1

Tag 092P, permanent. Cite it as [Bourbaki, Tag 092P].

Integration, V, p. 43, § 5. Measures defined by numerical densities

Let f\mathbf{f} be a function defined on TT, with values in a Banach space FF or in R‾\overline{\mathbf{R}}. In order that f\mathbf{f} be essentially integrable for the measure η=u⋅θ\eta = u \cdot \theta, it is necessary and sufficient that ufuf be essentially θ\theta-integrable, in which case

∫f dη=∫(uf) dθ. \int f \, d\eta = \int (uf) \, d\theta .

Suppose moreover that uu is continuous and that u(t)≠0u(t) \neq 0 for all t∈Tt \in T; then ff is integrable for the measure η\eta if and only if ufuf is integrable for θ\theta.

The case that uu and θ\theta are positive follows at once from Th. 2 of §4, No. 4. The first and the last assertion of the statement then follow immediately, because ff is essentially integrable (resp. integrable) with respect to η=u⋅θ\eta = u \cdot \theta if and only if it is essentially integrable (resp. integrable) for ∣η∣=∣u∣⋅∣θ∣|\eta| = |u| \cdot |\theta|. Finally, suppose that ff is essentially integrable for η\eta (hence for ∣η∣|\eta|); we make use of the decomposition (2): ff is essentially integrable for each of the measures ηij=gi⋅μj\eta_{ij} = g_i \cdot \mu_j (i=1,2,3,4, j=1,2,3,4i = 1, 2, 3, 4,\ j = 1, 2, 3, 4), because these measures are ≤∣η∣\leq |\eta|. We have

∫f dηij=∫gif dμj. \int f \, d\eta_{ij} = \int g_i f \, d\mu_j .

The formula (6) follows immediately from this.

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.