Documentation

TauCeti.Probability.Renewal.Measure

The renewal measure and the renewal function #

For a measure F on an additive monoid, the renewal measure is the sum of its convolution powers,

U = ∑ n, F^{∗n} = δ₀ + F + F ∗ F + ⋯,

where F^{∗0} = δ₀ is Measure.convolutionPower F 0. It satisfies the renewal equation U = δ₀ + F ∗ U. When F is the law of the increments of a renewal process, F^{∗n} is the law of the n-th arrival time, so U s is the expected number of arrival times in s, counting the artificial arrival at time zero. This file proves that identity for the intervals [0, t].

On the half-line ℝ≥0, the renewal function is m t = (F ∗ U) [0, t] = ∑_{n ≥ 1} F^{∗n} [0, t]. For independent increments with law F, it is the expected count 𝔼[N t] of the renewal process, and U [0, t] = 1 + m t; this holds also when F has an atom at zero. If F is a probability measure with F {0} < 1, the finite moments of the renewal counts show that m t is finite. Hence U is finite on bounded intervals, and m is nondecreasing and right-continuous. The renewal measure and the renewal function are the objects of the renewal limit theorems and of the solution g = h ∗ U of the renewal equation g = h + g ∗ F.

Main definitions #

Main results #

References #

The renewal measure #

noncomputable def MeasureTheory.Measure.renewalMeasure {α : Type u_1} [MeasurableSpace α] [AddMonoid α] (μ : Measure α) :

The renewal measure ∑ n, μ^{∗n} of a measure μ: the sum of all its convolution powers, including the point mass μ^{∗0} = δ₀. For the law μ of the increments of a renewal process, its mass on [0, t] is one more than the expected number of arrivals in [0, t] (renewalMeasure_Iic and TauCeti.Probability.lintegral_renewalCount).

Instances For
    theorem MeasureTheory.Measure.map_renewalMeasure {α : Type u_1} [MeasurableSpace α] [AddMonoid α] {β : Type u_2} [MeasurableSpace β] [AddMonoid β] [MeasurableAdd₂ α] [MeasurableAdd₂ β] (μ : Measure α) [SFinite μ] (f : α →+ β) (hf : Measurable ⇑f) :
    map (⇑f) μ.renewalMeasure = (map (⇑f) μ).renewalMeasure

    A measurable additive homomorphism transports the renewal measure to the renewal measure of the transported increment law.

    Each convolution power is dominated by the renewal measure.

    An s-finite measure is dominated by its renewal measure, of which it is the term μ^{∗1}.

    An s-finite measure whose renewal measure is locally finite is itself locally finite.

    theorem MeasureTheory.Measure.summable_convolutionPower_real {α : Type u_1} [MeasurableSpace α] [AddMonoid α] {μ : Measure α} {s : Set α} (hU : μ.renewalMeasure s ≠ ⊤) :
    Summable fun (n : ℕ) => (μ.convolutionPower n).real s

    The masses of a set s under the convolution powers are summable when the renewal measure gives s finite mass. No measurability of s is needed.

    The renewal measure of an s-finite measure is s-finite.

    Convolving the renewal measure with μ removes the term μ^{∗0} = δ₀: μ ∗ U = ∑ n, μ^{∗(n + 1)}.

    The renewal equation U = δ₀ + μ ∗ U for the renewal measure U of μ.

    The renewal function on the half-line #

    The renewal function t ↦ (μ ∗ U) [0, t] of a measure μ on ℝ≥0, where U is the renewal measure of μ. It equals ∑_{n ≥ 1} μ^{∗n} [0, t] (renewalFunction_eq_tsum), and for independent increments with law μ it is the expected count of the renewal process (TauCeti.Probability.lintegral_renewalCount).

    Instances For

      The renewal function is the sum of the masses of [0, t] under the positive convolution powers.

      The renewal measure of [0, t] is one more than the renewal function at t: the extra unit is the point mass μ^{∗0} = δ₀.

      The renewal function is nondecreasing in time.

      theorem TauCeti.Probability.lintegral_renewalCount {Ω : Type u_1} [MeasurableSpace Ω] {P : MeasureTheory.Measure Ω} {T : ℕ → Ω → NNReal} (hindep : ProbabilityTheory.iIndepFun T P) (hid : ∀ (n : ℕ), ProbabilityTheory.IdentDistrib (T n) (T 0) P P) (t : NNReal) :

      The renewal function is the expected count. For independent, identically distributed increments, the expected number of arrivals in [0, t] is the renewal function of the common law of the increments. No assumption is made on the atom of the law at zero, and both sides may be infinite.

      theorem TauCeti.Probability.integral_renewalCountNat {Ω : Type u_1} [MeasurableSpace Ω] {P : MeasureTheory.Measure Ω} {T : ℕ → Ω → NNReal} (hT : ∀ (n : ℕ), Measurable (T n)) (hindep : ProbabilityTheory.iIndepFun T P) (hid : ∀ (n : ℕ), ProbabilityTheory.IdentDistrib (T n) (T 0) P P) (hzero : P {ω : Ω | T 0 ω = 0} < 1) (t : NNReal) :

      The real form of TauCeti.Probability.lintegral_renewalCount: for independent, identically distributed increments that are not almost surely zero, the mean of the natural-valued count at time t is the renewal function of the increment law.

      The renewal function is finite. For a probability measure μ on ℝ≥0 that is not the point mass at zero, the renewal function is finite at every time. No assumption is made on the mean of μ.

      The renewal measure of a probability measure on ℝ≥0 other than the point mass at zero is finite on every bounded interval [0, t].

      The renewal measure of a probability measure on ℝ≥0 other than the point mass at zero is locally finite.

      Right continuity of the renewal function of a probability measure on ℝ≥0. For the point mass at zero the renewal function is constantly infinite.