Rate and null marks for first long excursions #
The lifetime intensity has no atoms. Localizing the mean measure to bounded label windows transfers this fact simultaneously to every passage jump of a stable path.
Reference: J. Bertoin, Lévy Processes, Cambridge University Press, 1996, Chapter IV.
The rate r_θ = 1/Γ(1-1/θ) = N(ζ > 1) = θ p₀.
Equations
- BGW.StableTrees.longRate θ = 1 / Real.Gamma (1 - 1 / θ)
Instances For
The exponential law of rate r_θ on ℝ≥0 (the law of the first long label).
Equations
Instances For
theorem
BGW.StableTrees.ae_jumpExcursion_not_mem_of_null
{θ : ℝ}
(hθ : 1 < θ ∧ θ ≤ 2)
{A : Set Excursion}
(hA : MeasurableSet A)
(hnull : (excursionMeasure θ) A = 0)
:
∀ᵐ (f : Skorokhod.DLoc) ∂↑(stableLocalLaw θ), ∀ x ∈ passageJumpSet f, jumpExcursion x f ∉ A
A measurable null mark set contains none of the passage-jump marks, almost surely.
theorem
BGW.StableTrees.ae_jump_lifetime_ne
{θ : ℝ}
(hθ : 1 < θ ∧ θ ≤ 2)
(a : NNReal)
:
∀ᵐ (f : Skorokhod.DLoc) ∂↑(stableLocalLaw θ), ∀ x ∈ passageJumpSet f, passageTime x f - passageTimeMinus x f ≠ a
A.s. no excursion mark has a prescribed lifetime a: the set of excursions of lifetime a
is N-null, and N-null mark sets carry no jump mark (ae_jumpExcursion_not_mem_of_null).
theorem
BGW.StableTrees.ae_continuousAt_tailExcursion_path
{θ : ℝ}
(hθ : 1 < θ ∧ θ ≤ 2)
(T : NNReal)
(hT : 0 < T)
:
∀ᵐ (e : Excursion) ∂↑(tailExcursionLaw θ), ContinuousAt (↑e.path) T
No fixed jump of the selected mark at a positive cutoff.