Densities against a common measure, and normalizing a density #
Let λ be a measure and let ν₁ i, ν₂ i be finitely many pairs of measures on a σ-compact
topological space, all finite on compact sets. The sum ρ = λ + ∑ i, (ν₁ i + ν₂ i) is finite on
compact sets and dominates all of them, so each signed difference ν₁ i - ν₂ i has a real density
dν₁ i/dρ - dν₂ i/dρ with respect to ρ, integrable on compact sets
(MeasureTheory.Measure.exists_common_density_sub).
This is how a vector-valued functional, given componentwise as differences of measures, is
represented by a single vector-valued density against one measure ρ which also dominates a
prescribed variation measure λ. Its pointwise norm is then compared with the density of λ
with respect to ρ, as in a polar decomposition.
The file also contains the normalization step of a polar decomposition
(MeasureTheory.Measure.exists_norm_le_one_toReal_rnDeriv_smul_eq): a measurable field g
dominated by the density dλ/dρ of λ ≪ ρ agrees ρ-almost everywhere with
(dλ/dρ).toReal • σ, where σ is a measurable field of norm at most one λ-almost everywhere.
This σ is the unit field of the polar decomposition.
References #
- L. C. Evans, R. F. Gariepy, Measure Theory and Fine Properties of Functions, revised edition, §1.8 (the Riesz representation theorem for vector-valued functionals).
Common densities. For a measure λ and finitely many pairs of measures ν₁ i, ν₂ i, all
finite on compact sets of a σ-compact space, there is a measure ρ, finite on compact sets and
dominating λ, with respect to which each signed difference ν₁ i - ν₂ i has a measurable density
f i, integrable on compact sets: ∫ ψ dν₁ i - ∫ ψ dν₂ i = ∫ f i ψ dρ for every ψ integrable
for ν₁ i and ν₂ i.
Normalizing a density. If a measurable field g has pointwise norm at most the density
dλ/dρ of a measure λ ≪ ρ (up to a ρ-null set), then g agrees ρ-almost everywhere with
(dλ/dρ).toReal • σ for a measurable field σ of norm at most one λ-almost everywhere.