HepLean Documentation

Mathlib.MeasureTheory.Decomposition.Lebesgue

Lebesgue decomposition #

This file proves the Lebesgue decomposition theorem. The Lebesgue decomposition theorem states that, given two σ-finite measures μ and ν, there exists a σ-finite measure ξ and a measurable function f such that μ = ξ + fν and ξ is mutually singular with respect to ν.

The Lebesgue decomposition provides the Radon-Nikodym theorem readily.

Main definitions #

MeasureTheory.Measure.HaveLebesgueDecomposition : A pair of measures μ and ν is said to HaveLebesgueDecomposition if there exist a measure ξ and a measurable function f, such that ξ is mutually singular with respect to ν and μ = ξ + ν.withDensity f
MeasureTheory.Measure.singularPart : If a pair of measures HaveLebesgueDecomposition, then singularPart chooses the measure from HaveLebesgueDecomposition, otherwise it returns the zero measure.
MeasureTheory.Measure.rnDeriv: If a pair of measures HaveLebesgueDecomposition, then rnDeriv chooses the measurable function from HaveLebesgueDecomposition, otherwise it returns the zero function.

Main results #

MeasureTheory.Measure.haveLebesgueDecomposition_of_sigmaFinite : the Lebesgue decomposition theorem.
MeasureTheory.Measure.eq_singularPart : Given measures μ and ν, if s is a measure mutually singular to ν and f is a measurable function such that μ = s + fν, then s = μ.singularPart ν.
MeasureTheory.Measure.eq_rnDeriv : Given measures μ and ν, if s is a measure mutually singular to ν and f is a measurable function such that μ = s + fν, then f = μ.rnDeriv ν.

Tags #

Lebesgue decomposition theorem

class MeasureTheory.Measure.HaveLebesgueDecomposition {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

A pair of measures μ and ν is said to HaveLebesgueDecomposition if there exists a measure ξ and a measurable function f, such that ξ is mutually singular with respect to ν and μ = ξ + ν.withDensity f.

lebesgue_decomposition : ∃ (p : MeasureTheory.Measure α × (α → ENNReal)), Measurable p.2 ∧ p.1.MutuallySingular ν ∧ μ = p.1 + ν.withDensity p.2

Instances

theorem MeasureTheory.Measure.singularPart_def {α : Type u_2} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

μ.singularPart ν = if h : μ.HaveLebesgueDecomposition ν then (Classical.choose ⋯).1 else 0

@[irreducible]

noncomputable def MeasureTheory.Measure.singularPart {α : Type u_2} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

MeasureTheory.Measure α

If a pair of measures HaveLebesgueDecomposition, then singularPart chooses the measure from HaveLebesgueDecomposition, otherwise it returns the zero measure. For sigma-finite measures, μ = μ.singularPart ν + ν.withDensity (μ.rnDeriv ν).

Equations

@MeasureTheory.Measure.singularPart = MeasureTheory.Measure.wrapped✝.1

Instances For

@[irreducible]

noncomputable def MeasureTheory.Measure.rnDeriv {α : Type u_2} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

α → ENNReal

If a pair of measures HaveLebesgueDecomposition, then rnDeriv chooses the measurable function from HaveLebesgueDecomposition, otherwise it returns the zero function. For sigma-finite measures, μ = μ.singularPart ν + ν.withDensity (μ.rnDeriv ν).

Equations

@MeasureTheory.Measure.rnDeriv = MeasureTheory.Measure.wrapped✝.1

Instances For

theorem MeasureTheory.Measure.rnDeriv_def {α : Type u_2} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

μ.rnDeriv ν = if h : μ.HaveLebesgueDecomposition ν then (Classical.choose ⋯).2 else 0

theorem MeasureTheory.Measure.haveLebesgueDecomposition_spec {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [h : μ.HaveLebesgueDecomposition ν] :

Measurable (μ.rnDeriv ν) ∧ (μ.singularPart ν).MutuallySingular ν ∧ μ = μ.singularPart ν + ν.withDensity (μ.rnDeriv ν)

theorem MeasureTheory.Measure.rnDeriv_of_not_haveLebesgueDecomposition {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (h : ¬μ.HaveLebesgueDecomposition ν) :

μ.rnDeriv ν = 0

theorem MeasureTheory.Measure.singularPart_of_not_haveLebesgueDecomposition {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (h : ¬μ.HaveLebesgueDecomposition ν) :

μ.singularPart ν = 0

theorem MeasureTheory.Measure.measurable_rnDeriv {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

Measurable (μ.rnDeriv ν)

theorem MeasureTheory.Measure.mutuallySingular_singularPart {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

(μ.singularPart ν).MutuallySingular ν

theorem MeasureTheory.Measure.haveLebesgueDecomposition_add {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

μ = μ.singularPart ν + ν.withDensity (μ.rnDeriv ν)

theorem MeasureTheory.Measure.singularPart_add_rnDeriv {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

μ.singularPart ν + ν.withDensity (μ.rnDeriv ν) = μ

For the versions of this lemma where ν.withDensity (μ.rnDeriv ν) or μ.singularPart ν are isolated, see MeasureTheory.Measure.measure_sub_singularPart and MeasureTheory.Measure.measure_sub_rnDeriv.

theorem MeasureTheory.Measure.rnDeriv_add_singularPart {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

ν.withDensity (μ.rnDeriv ν) + μ.singularPart ν = μ

For the versions of this lemma where μ.singularPart ν or ν.withDensity (μ.rnDeriv ν) are isolated, see MeasureTheory.Measure.measure_sub_singularPart and MeasureTheory.Measure.measure_sub_rnDeriv.

instance MeasureTheory.Measure.instHaveLebesgueDecompositionZeroLeft {α : Type u_1} {m : MeasurableSpace α} {ν : MeasureTheory.Measure α} :

MeasureTheory.Measure.HaveLebesgueDecomposition 0 ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.instHaveLebesgueDecompositionZeroRight {α : Type u_1} {m : MeasurableSpace α} {μ : MeasureTheory.Measure α} :

μ.HaveLebesgueDecomposition 0

Equations

⋯ = ⋯

instance MeasureTheory.Measure.instHaveLebesgueDecompositionSelf {α : Type u_1} {m : MeasurableSpace α} {μ : MeasureTheory.Measure α} :

μ.HaveLebesgueDecomposition μ

Equations

⋯ = ⋯

instance MeasureTheory.Measure.HaveLebesgueDecomposition.sum_left {α : Type u_1} {m : MeasurableSpace α} {ν : MeasureTheory.Measure α} {ι : Type u_2} [Countable ι] (μ : ι → MeasureTheory.Measure α) [∀ (i : ι), (μ i).HaveLebesgueDecomposition ν] :

(MeasureTheory.Measure.sum μ).HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.HaveLebesgueDecomposition.add_left {α : Type u_1} {m : MeasurableSpace α} {μ ν μ' : MeasureTheory.Measure α} [μ.HaveLebesgueDecomposition ν] [μ'.HaveLebesgueDecomposition ν] :

(μ + μ').HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.haveLebesgueDecompositionSMul' {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] (r : ENNReal) :

(r • μ).HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.haveLebesgueDecompositionSMul {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] (r : NNReal) :

(r • μ).HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.haveLebesgueDecompositionSMulRight {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] (r : NNReal) :

μ.HaveLebesgueDecomposition (r • ν)

Equations

⋯ = ⋯

theorem MeasureTheory.Measure.haveLebesgueDecomposition_withDensity {α : Type u_1} {m : MeasurableSpace α} (μ : MeasureTheory.Measure α) {f : α → ENNReal} (hf : Measurable f) :

(μ.withDensity f).HaveLebesgueDecomposition μ

instance MeasureTheory.Measure.haveLebesgueDecompositionRnDeriv {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

(ν.withDensity (μ.rnDeriv ν)).HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

instance MeasureTheory.Measure.instHaveLebesgueDecompositionSingularPart {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} :

(μ.singularPart ν).HaveLebesgueDecomposition ν

Equations

⋯ = ⋯

theorem MeasureTheory.Measure.singularPart_le {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

μ.singularPart ν ≤ μ

theorem MeasureTheory.Measure.withDensity_rnDeriv_le {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

ν.withDensity (μ.rnDeriv ν) ≤ μ

theorem AEMeasurable.singularPart {α : Type u_1} {m : MeasurableSpace α} {μ : MeasureTheory.Measure α} {β : Type u_2} {x✝ : MeasurableSpace β} {f : α → β} (hf : AEMeasurable f μ) (ν : MeasureTheory.Measure α) :

AEMeasurable f (μ.singularPart ν)

theorem AEMeasurable.withDensity_rnDeriv {α : Type u_1} {m : MeasurableSpace α} {μ : MeasureTheory.Measure α} {β : Type u_2} {x✝ : MeasurableSpace β} {f : α → β} (hf : AEMeasurable f μ) (ν : MeasureTheory.Measure α) :

AEMeasurable f (ν.withDensity (μ.rnDeriv ν))

theorem MeasureTheory.Measure.MutuallySingular.singularPart {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (h : μ.MutuallySingular ν) (ν' : MeasureTheory.Measure α) :

(μ.singularPart ν').MutuallySingular ν

theorem MeasureTheory.Measure.absolutelyContinuous_withDensity_rnDeriv {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [ν.HaveLebesgueDecomposition μ] (hμν : μ.AbsolutelyContinuous ν) :

μ.AbsolutelyContinuous (μ.withDensity (ν.rnDeriv μ))

theorem MeasureTheory.Measure.singularPart_eq_zero_of_ac {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (h : μ.AbsolutelyContinuous ν) :

μ.singularPart ν = 0

@[simp]

theorem MeasureTheory.Measure.singularPart_zero {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) :

MeasureTheory.Measure.singularPart 0 ν = 0

@[simp]

theorem MeasureTheory.Measure.singularPart_zero_right {α : Type u_1} {m : MeasurableSpace α} (μ : MeasureTheory.Measure α) :

μ.singularPart 0 = μ

theorem MeasureTheory.Measure.singularPart_eq_zero {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

μ.singularPart ν = 0 ↔ μ.AbsolutelyContinuous ν

@[simp]

theorem MeasureTheory.Measure.withDensity_rnDeriv_eq_zero {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

ν.withDensity (μ.rnDeriv ν) = 0 ↔ μ.MutuallySingular ν

@[simp]

theorem MeasureTheory.Measure.rnDeriv_eq_zero {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] :

μ.rnDeriv ν =ᵐ[ν] 0 ↔ μ.MutuallySingular ν

theorem MeasureTheory.Measure.rnDeriv_zero {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) :

MeasureTheory.Measure.rnDeriv 0 ν =ᵐ[ν] 0

theorem MeasureTheory.Measure.MutuallySingular.rnDeriv_ae_eq_zero {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (hμν : μ.MutuallySingular ν) :

μ.rnDeriv ν =ᵐ[ν] 0

@[simp]

theorem MeasureTheory.Measure.singularPart_withDensity {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) (f : α → ENNReal) :

(ν.withDensity f).singularPart ν = 0

theorem MeasureTheory.Measure.rnDeriv_singularPart {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

(μ.singularPart ν).rnDeriv ν =ᵐ[ν] 0

@[simp]

theorem MeasureTheory.Measure.singularPart_self {α : Type u_1} {m : MeasurableSpace α} (μ : MeasureTheory.Measure α) :

μ.singularPart μ = 0

theorem MeasureTheory.Measure.rnDeriv_self {α : Type u_1} {m : MeasurableSpace α} (μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite μ] :

μ.rnDeriv μ =ᵐ[μ] fun (x : α) => 1

theorem MeasureTheory.Measure.singularPart_eq_self {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [μ.HaveLebesgueDecomposition ν] :

μ.singularPart ν = μ ↔ μ.MutuallySingular ν

@[simp]

theorem MeasureTheory.Measure.singularPart_singularPart {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

(μ.singularPart ν).singularPart ν = μ.singularPart ν

instance MeasureTheory.Measure.singularPart.instIsFiniteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.IsFiniteMeasure μ] :

MeasureTheory.IsFiniteMeasure (μ.singularPart ν)

Equations

⋯ = ⋯

instance MeasureTheory.Measure.singularPart.instSigmaFinite {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.SigmaFinite μ] :

MeasureTheory.SigmaFinite (μ.singularPart ν)

Equations

⋯ = ⋯

instance MeasureTheory.Measure.singularPart.instIsLocallyFiniteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [TopologicalSpace α] [MeasureTheory.IsLocallyFiniteMeasure μ] :

MeasureTheory.IsLocallyFiniteMeasure (μ.singularPart ν)

Equations

⋯ = ⋯

instance MeasureTheory.Measure.withDensity.instIsFiniteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.IsFiniteMeasure μ] :

MeasureTheory.IsFiniteMeasure (ν.withDensity (μ.rnDeriv ν))

Equations

⋯ = ⋯

instance MeasureTheory.Measure.withDensity.instSigmaFinite {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.SigmaFinite μ] :

MeasureTheory.SigmaFinite (ν.withDensity (μ.rnDeriv ν))

Equations

⋯ = ⋯

instance MeasureTheory.Measure.withDensity.instIsLocallyFiniteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [TopologicalSpace α] [MeasureTheory.IsLocallyFiniteMeasure μ] :

MeasureTheory.IsLocallyFiniteMeasure (ν.withDensity (μ.rnDeriv ν))

Equations

⋯ = ⋯

theorem MeasureTheory.Measure.lintegral_rnDeriv_lt_top_of_measure_ne_top {α : Type u_1} {m : MeasurableSpace α} {μ : MeasureTheory.Measure α} (ν : MeasureTheory.Measure α) {s : Set α} (hs : μ s ≠ ⊤) :

∫⁻ (x : α) in s, μ.rnDeriv ν x ∂ν < ⊤

theorem MeasureTheory.Measure.lintegral_rnDeriv_lt_top {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure μ] :

∫⁻ (x : α), μ.rnDeriv ν x ∂ν < ⊤

theorem MeasureTheory.Measure.integrable_toReal_rnDeriv {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.IsFiniteMeasure μ] :

MeasureTheory.Integrable (fun (x : α) => (μ.rnDeriv ν x).toReal) ν

theorem MeasureTheory.Measure.rnDeriv_lt_top {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite μ] :

∀ᵐ (x : α) ∂ν, μ.rnDeriv ν x < ⊤

The Radon-Nikodym derivative of a sigma-finite measure μ with respect to another measure ν is ν-almost everywhere finite.

theorem MeasureTheory.Measure.rnDeriv_ne_top {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite μ] :

∀ᵐ (x : α) ∂ν, μ.rnDeriv ν x ≠ ⊤

theorem MeasureTheory.Measure.eq_singularPart {α : Type u_1} {m : MeasurableSpace α} {μ ν s : MeasureTheory.Measure α} {f : α → ENNReal} (hf : Measurable f) (hs : s.MutuallySingular ν) (hadd : μ = s + ν.withDensity f) :

s = μ.singularPart ν

Given measures μ and ν, if s is a measure mutually singular to ν and f is a measurable function such that μ = s + fν, then s = μ.singularPart μ.

This theorem provides the uniqueness of the singularPart in the Lebesgue decomposition theorem, while MeasureTheory.Measure.eq_rnDeriv provides the uniqueness of the rnDeriv.

theorem MeasureTheory.Measure.singularPart_smul {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) (r : NNReal) :

(r • μ).singularPart ν = r • μ.singularPart ν

theorem MeasureTheory.Measure.singularPart_smul_right {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) (r : NNReal) (hr : r ≠ 0) :

μ.singularPart (r • ν) = μ.singularPart ν

theorem MeasureTheory.Measure.singularPart_add {α : Type u_1} {m : MeasurableSpace α} (μ₁ μ₂ ν : MeasureTheory.Measure α) [μ₁.HaveLebesgueDecomposition ν] [μ₂.HaveLebesgueDecomposition ν] :

(μ₁ + μ₂).singularPart ν = μ₁.singularPart ν + μ₂.singularPart ν

theorem MeasureTheory.Measure.singularPart_restrict {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] {s : Set α} (hs : MeasurableSet s) :

(μ.restrict s).singularPart ν = (μ.singularPart ν).restrict s

theorem MeasureTheory.Measure.measure_sub_singularPart {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] [MeasureTheory.IsFiniteMeasure μ] :

μ - μ.singularPart ν = ν.withDensity (μ.rnDeriv ν)

theorem MeasureTheory.Measure.measure_sub_rnDeriv {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] [MeasureTheory.IsFiniteMeasure μ] :

μ - ν.withDensity (μ.rnDeriv ν) = μ.singularPart ν

theorem MeasureTheory.Measure.eq_withDensity_rnDeriv {α : Type u_1} {m : MeasurableSpace α} {μ ν s : MeasureTheory.Measure α} {f : α → ENNReal} (hf : Measurable f) (hs : s.MutuallySingular ν) (hadd : μ = s + ν.withDensity f) :

ν.withDensity f = ν.withDensity (μ.rnDeriv ν)

Given measures μ and ν, if s is a measure mutually singular to ν and f is a measurable function such that μ = s + fν, then f = μ.rnDeriv ν.

This theorem provides the uniqueness of the rnDeriv in the Lebesgue decomposition theorem, while MeasureTheory.Measure.eq_singularPart provides the uniqueness of the singularPart. Here, the uniqueness is given in terms of the measures, while the uniqueness in terms of the functions is given in eq_rnDeriv.

theorem MeasureTheory.Measure.eq_withDensity_rnDeriv₀ {α : Type u_1} {m : MeasurableSpace α} {μ ν s : MeasureTheory.Measure α} {f : α → ENNReal} (hf : AEMeasurable f ν) (hs : s.MutuallySingular ν) (hadd : μ = s + ν.withDensity f) :

ν.withDensity f = ν.withDensity (μ.rnDeriv ν)

theorem MeasureTheory.Measure.eq_rnDeriv₀ {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.SigmaFinite ν] {s : MeasureTheory.Measure α} {f : α → ENNReal} (hf : AEMeasurable f ν) (hs : s.MutuallySingular ν) (hadd : μ = s + ν.withDensity f) :

f =ᵐ[ν] μ.rnDeriv ν

theorem MeasureTheory.Measure.eq_rnDeriv {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.SigmaFinite ν] {s : MeasureTheory.Measure α} {f : α → ENNReal} (hf : Measurable f) (hs : s.MutuallySingular ν) (hadd : μ = s + ν.withDensity f) :

f =ᵐ[ν] μ.rnDeriv ν

Given measures μ and ν, if s is a measure mutually singular to ν and f is a measurable function such that μ = s + fν, then f = μ.rnDeriv ν.

This theorem provides the uniqueness of the rnDeriv in the Lebesgue decomposition theorem, while MeasureTheory.Measure.eq_singularPart provides the uniqueness of the singularPart. Here, the uniqueness is given in terms of the functions, while the uniqueness in terms of the functions is given in eq_withDensity_rnDeriv.

theorem MeasureTheory.Measure.rnDeriv_withDensity₀ {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] {f : α → ENNReal} (hf : AEMeasurable f ν) :

(ν.withDensity f).rnDeriv ν =ᵐ[ν] f

The Radon-Nikodym derivative of f ν with respect to ν is f.

theorem MeasureTheory.Measure.rnDeriv_withDensity {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] {f : α → ENNReal} (hf : Measurable f) :

(ν.withDensity f).rnDeriv ν =ᵐ[ν] f

The Radon-Nikodym derivative of f ν with respect to ν is f.

theorem MeasureTheory.Measure.rnDeriv_restrict {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [μ.HaveLebesgueDecomposition ν] [MeasureTheory.SigmaFinite ν] {s : Set α} (hs : MeasurableSet s) :

(μ.restrict s).rnDeriv ν =ᵐ[ν] s.indicator (μ.rnDeriv ν)

theorem MeasureTheory.Measure.rnDeriv_restrict_self {α : Type u_1} {m : MeasurableSpace α} (ν : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] {s : Set α} (hs : MeasurableSet s) :

(ν.restrict s).rnDeriv ν =ᵐ[ν] s.indicator 1

The Radon-Nikodym derivative of the restriction of a measure to a measurable set is the indicator function of this set.

theorem MeasureTheory.Measure.rnDeriv_smul_left {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure ν] [ν.HaveLebesgueDecomposition μ] (r : NNReal) :

(r • ν).rnDeriv μ =ᵐ[μ] r • ν.rnDeriv μ

Radon-Nikodym derivative of the scalar multiple of a measure. See also rnDeriv_smul_left', which requires sigma-finite ν and μ.

theorem MeasureTheory.Measure.rnDeriv_smul_left_of_ne_top {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure ν] [ν.HaveLebesgueDecomposition μ] {r : ENNReal} (hr : r ≠ ⊤) :

(r • ν).rnDeriv μ =ᵐ[μ] r • ν.rnDeriv μ

Radon-Nikodym derivative of the scalar multiple of a measure. See also rnDeriv_smul_left_of_ne_top', which requires sigma-finite ν and μ.

theorem MeasureTheory.Measure.rnDeriv_smul_right {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure ν] [ν.HaveLebesgueDecomposition μ] {r : NNReal} (hr : r ≠ 0) :

ν.rnDeriv (r • μ) =ᵐ[μ] r⁻¹ • ν.rnDeriv μ

Radon-Nikodym derivative with respect to the scalar multiple of a measure. See also rnDeriv_smul_right', which requires sigma-finite ν and μ.

theorem MeasureTheory.Measure.rnDeriv_smul_right_of_ne_top {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure ν] [ν.HaveLebesgueDecomposition μ] {r : ENNReal} (hr : r ≠ 0) (hr_ne_top : r ≠ ⊤) :

ν.rnDeriv (r • μ) =ᵐ[μ] r⁻¹ • ν.rnDeriv μ

Radon-Nikodym derivative with respect to the scalar multiple of a measure. See also rnDeriv_smul_right_of_ne_top', which requires sigma-finite ν and μ.

theorem MeasureTheory.Measure.rnDeriv_add {α : Type u_1} {m : MeasurableSpace α} (ν₁ ν₂ μ : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure ν₁] [MeasureTheory.IsFiniteMeasure ν₂] [ν₁.HaveLebesgueDecomposition μ] [ν₂.HaveLebesgueDecomposition μ] [(ν₁ + ν₂).HaveLebesgueDecomposition μ] :

(ν₁ + ν₂).rnDeriv μ =ᵐ[μ] ν₁.rnDeriv μ + ν₂.rnDeriv μ

Radon-Nikodym derivative of a sum of two measures. See also rnDeriv_add', which requires sigma-finite ν₁, ν₂ and μ.

theorem MeasureTheory.Measure.exists_positive_of_not_mutuallySingular {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [MeasureTheory.IsFiniteMeasure μ] [MeasureTheory.IsFiniteMeasure ν] (h : ¬μ.MutuallySingular ν) :

∃ (ε : NNReal), 0 < ε ∧ ∃ (E : Set α), MeasurableSet E ∧ 0 < ν E ∧ MeasureTheory.VectorMeasure.restrict 0 E ≤ MeasureTheory.VectorMeasure.restrict (μ.toSignedMeasure - (ε • ν).toSignedMeasure) E

If two finite measures μ and ν are not mutually singular, there exists some ε > 0 and a measurable set E, such that ν(E) > 0 and E is positive with respect to μ - εν.

This lemma is useful for the Lebesgue decomposition theorem.

def MeasureTheory.Measure.LebesgueDecomposition.measurableLE {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

Set (α → ENNReal)

Given two measures μ and ν, measurableLE μ ν is the set of measurable functions f, such that, for all measurable sets A, ∫⁻ x in A, f x ∂μ ≤ ν A.

This is useful for the Lebesgue decomposition theorem.

Equations

MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν = {f : α → ENNReal | Measurable f ∧ ∀ (A : Set α), MeasurableSet A → ∫⁻ (x : α) in A, f x ∂μ ≤ ν A}

Instances For

theorem MeasureTheory.Measure.LebesgueDecomposition.zero_mem_measurableLE {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} :

0 ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν

theorem MeasureTheory.Measure.LebesgueDecomposition.sup_mem_measurableLE {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} {f g : α → ENNReal} (hf : f ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν) (hg : g ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν) :

(fun (a : α) => f a ⊔ g a) ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_succ_eq_sup {α : Sort u_2} (f : ℕ → α → ENNReal) (m : ℕ) (a : α) :

⨆ (k : ℕ), ⨆ (_ : k ≤ m + 1), f k a = f m.succ a ⊔ ⨆ (k : ℕ), ⨆ (_ : k ≤ m), f k a

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_mem_measurableLE {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (f : ℕ → α → ENNReal) (hf : ∀ (n : ℕ), f n ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν) (n : ℕ) :

(fun (x : α) => ⨆ (k : ℕ), ⨆ (_ : k ≤ n), f k x) ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_mem_measurableLE' {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} (f : ℕ → α → ENNReal) (hf : ∀ (n : ℕ), f n ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν) (n : ℕ) :

⨆ (k : ℕ), ⨆ (_ : k ≤ n), f k ∈ MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_monotone {α : Type u_2} (f : ℕ → α → ENNReal) :

Monotone fun (n : ℕ) (x : α) => ⨆ (k : ℕ), ⨆ (_ : k ≤ n), f k x

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_monotone' {α : Type u_2} (f : ℕ → α → ENNReal) (x : α) :

Monotone fun (n : ℕ) => ⨆ (k : ℕ), ⨆ (_ : k ≤ n), f k x

theorem MeasureTheory.Measure.LebesgueDecomposition.iSup_le_le {α : Type u_2} (f : ℕ → α → ENNReal) (n k : ℕ) (hk : k ≤ n) :

f k ≤ fun (x : α) => ⨆ (k : ℕ), ⨆ (_ : k ≤ n), f k x

def MeasureTheory.Measure.LebesgueDecomposition.measurableLEEval {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) :

measurableLEEval μ ν is the set of ∫⁻ x, f x ∂μ for all f ∈ measurableLE μ ν.

Equations

MeasureTheory.Measure.LebesgueDecomposition.measurableLEEval μ ν = (fun (f : α → ENNReal) => ∫⁻ (x : α), f x ∂μ) '' MeasureTheory.Measure.LebesgueDecomposition.measurableLE μ ν

Instances For

theorem MeasureTheory.Measure.haveLebesgueDecomposition_of_finiteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.IsFiniteMeasure μ] [MeasureTheory.IsFiniteMeasure ν] :

μ.HaveLebesgueDecomposition ν

Any pair of finite measures μ and ν, HaveLebesgueDecomposition. That is to say, there exist a measure ξ and a measurable function f, such that ξ is mutually singular with respect to ν and μ = ξ + ν.withDensity f.

This is not an instance since this is also shown for the more general σ-finite measures with MeasureTheory.Measure.haveLebesgueDecomposition_of_sigmaFinite.

theorem MeasureTheory.Measure.HaveLebesgueDecomposition.sfinite_of_isFiniteMeasure {α : Type u_1} {m : MeasurableSpace α} {μ ν : MeasureTheory.Measure α} [MeasureTheory.SFinite μ] (_h : ∀ (μ : MeasureTheory.Measure α) [inst : MeasureTheory.IsFiniteMeasure μ], μ.HaveLebesgueDecomposition ν) :

μ.HaveLebesgueDecomposition ν

If any finite measure has a Lebesgue decomposition with respect to ν, then the same is true for any s-finite measure.

@[instance 100]

instance MeasureTheory.Measure.haveLebesgueDecomposition_of_sigmaFinite {α : Type u_1} {m : MeasurableSpace α} (μ ν : MeasureTheory.Measure α) [MeasureTheory.SFinite μ] [MeasureTheory.SigmaFinite ν] :

μ.HaveLebesgueDecomposition ν

The Lebesgue decomposition theorem: Any s-finite measure μ has Lebesgue decomposition with respect to any σ-finite measure ν. That is to say, there exist a measure ξ and a measurable function f, such that ξ is mutually singular with respect to ν and μ = ξ + ν.withDensity f

Equations

⋯ = ⋯

theorem MeasureTheory.Measure.rnDeriv_smul_left' {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] [MeasureTheory.SigmaFinite μ] (r : NNReal) :

(r • ν).rnDeriv μ =ᵐ[μ] r • ν.rnDeriv μ

Radon-Nikodym derivative of the scalar multiple of a measure. See also rnDeriv_smul_left, which has no hypothesis on μ but requires finite ν.

theorem MeasureTheory.Measure.rnDeriv_smul_left_of_ne_top' {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] [MeasureTheory.SigmaFinite μ] {r : ENNReal} (hr : r ≠ ⊤) :

(r • ν).rnDeriv μ =ᵐ[μ] r • ν.rnDeriv μ

Radon-Nikodym derivative of the scalar multiple of a measure. See also rnDeriv_smul_left_of_ne_top, which has no hypothesis on μ but requires finite ν.

theorem MeasureTheory.Measure.rnDeriv_smul_right' {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] [MeasureTheory.SigmaFinite μ] {r : NNReal} (hr : r ≠ 0) :

ν.rnDeriv (r • μ) =ᵐ[μ] r⁻¹ • ν.rnDeriv μ

Radon-Nikodym derivative with respect to the scalar multiple of a measure. See also rnDeriv_smul_right, which has no hypothesis on μ but requires finite ν.

theorem MeasureTheory.Measure.rnDeriv_smul_right_of_ne_top' {α : Type u_1} {m : MeasurableSpace α} (ν μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν] [MeasureTheory.SigmaFinite μ] {r : ENNReal} (hr : r ≠ 0) (hr_ne_top : r ≠ ⊤) :

ν.rnDeriv (r • μ) =ᵐ[μ] r⁻¹ • ν.rnDeriv μ

Radon-Nikodym derivative with respect to the scalar multiple of a measure. See also rnDeriv_smul_right_of_ne_top, which has no hypothesis on μ but requires finite ν.

theorem MeasureTheory.Measure.rnDeriv_add' {α : Type u_1} {m : MeasurableSpace α} (ν₁ ν₂ μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν₁] [MeasureTheory.SigmaFinite ν₂] [MeasureTheory.SigmaFinite μ] :

(ν₁ + ν₂).rnDeriv μ =ᵐ[μ] ν₁.rnDeriv μ + ν₂.rnDeriv μ

Radon-Nikodym derivative of a sum of two measures. See also rnDeriv_add, which has no hypothesis on μ but requires finite ν₁ and ν₂.

theorem MeasureTheory.Measure.rnDeriv_add_of_mutuallySingular {α : Type u_1} {m : MeasurableSpace α} (ν₁ ν₂ μ : MeasureTheory.Measure α) [MeasureTheory.SigmaFinite ν₁] [MeasureTheory.SigmaFinite ν₂] [MeasureTheory.SigmaFinite μ] (h : ν₂.MutuallySingular μ) :

(ν₁ + ν₂).rnDeriv μ =ᵐ[μ] ν₁.rnDeriv μ