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BGW.StableTrees.FirstLongMarkBasic

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.

noncomputable def BGW.StableTrees.longRate (θ : ℝ) :

The rate r_θ = 1/Γ(1-1/θ) = N(ζ > 1) = θ p₀.

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    The exponential law of rate r_θ on ℝ≥0 (the law of the first long label).

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      N(ζ > 1) = r_θ, from the sealed lifetime tail.

      No lifetime is charged by N (unified with lifetime 0, excluded by the carrier).

      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) :

      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) :

      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) :

      No fixed jump of the selected mark at a positive cutoff.