Documentation

BGW.StableTrees.SupremumPotentialBasic

Supremum potentials and reflected occupation resolvents #

Analytic functions for the scale series, exponential-clock supremum tail, and occupation resolvents of the reflected stable family.

Reference: A. E. Kyprianou, Fluctuations of Lévy Processes with Applications, 2nd ed., Springer, 2014, Chapter 8.

noncomputable def BGW.StableTrees.stableScale (θ x : ℝ) :

W(x) = x^{θ-1}/Γ(θ) for x ≥ 0, 0 for x < 0.

Equations
Instances For
    noncomputable def BGW.StableTrees.stableSeriesTerm (θ q : ℝ) (n : ℕ) (x : ℝ) :

    Term q^n x^{θ(n+1)-1}/Γ(θ(n+1)) of W_q.

    Equations
    Instances For
      noncomputable def BGW.StableTrees.stableSeriesDerivTerm (θ q : ℝ) (n : ℕ) (x : ℝ) :

      Term q^n x^{θ(n+1)-2}/Γ(θ(n+1)-1) of W_q'.

      Equations
      Instances For
        noncomputable def BGW.StableTrees.stableSeries (θ q x : ℝ) :

        W_q(x) for x ≥ 0, 0 for x < 0.

        Equations
        Instances For
          noncomputable def BGW.StableTrees.stableSeriesDeriv (θ q x : ℝ) :

          Termwise derivative of W_q on (0,∞), 0 elsewhere.

          Equations
          Instances For
            noncomputable def BGW.StableTrees.supExpTail (θ q x : ℝ) :

            H_q(x) = P(S_{e_q} ≥ x) for x ≥ 0, extended by 1 for x < 0.

            Equations
            Instances For
              noncomputable def BGW.StableTrees.supPotential (θ q x : ℝ) :

              h_q = (Φ/q) H_q, Φ = q^{1/θ}.

              Equations
              Instances For
                noncomputable def BGW.StableTrees.supOccKernel (ε r : ℝ) :

                The occupation kernel g_ε(r) = ε⁻¹ 1{r < ε}.

                Equations
                Instances For
                  noncomputable def BGW.StableTrees.reflectedResolvent (θ q : ℝ) (k : ℝ → ℝ) (y : ℝ) :

                  q-resolvent of the reflected family on a bounded Borel k: y ↦ E ∫_0^∞ e^{-qt} k(R^y_t) dt (start y.toNNReal).

                  Equations
                  • One or more equations did not get rendered due to their size.
                  Instances For
                    noncomputable def BGW.StableTrees.supCorrection (θ ε x : ℝ) :

                    The zero-resolvent correction v_ε.

                    Equations
                    Instances For
                      theorem BGW.StableTrees.stableScale_eq_zero {θ x : ℝ} (hθ : 1 < θ) (hx : x ≤ 0) :
                      stableScale θ x = 0

                      The scale vanishes on the nonpositive half-line for a stable index.

                      theorem BGW.StableTrees.stableSeries_zero {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) (q : ℝ) :
                      stableSeries θ q 0 = 0

                      The scale series vanishes at its left endpoint.

                      theorem BGW.StableTrees.supExpTail_zero {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) :
                      supExpTail θ q 0 = 1

                      The exponential-clock supremum tail equals one at zero.

                      theorem BGW.StableTrees.supExpTail_mem_Icc {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) (x : ℝ) :

                      The exponential-clock tail takes values in the unit interval.

                      theorem BGW.StableTrees.antitone_supExpTail {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) :

                      The exponential-clock supremum tail is nonincreasing.

                      theorem BGW.StableTrees.supPotential_zero {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) :
                      supPotential θ q 0 = q ^ (1 / θ) / q

                      The boundary potential has the required normalization.

                      theorem BGW.StableTrees.supPotential_mem_Icc {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) (x : ℝ) :
                      supPotential θ q x ∈ Set.Icc 0 (q ^ (1 / θ) / q)

                      The potential lies between zero and its boundary value.

                      The occupation cutoff is a Borel function.

                      theorem BGW.StableTrees.supOccKernel_mem_Icc {ε : ℝ} (hε : 0 < ε) (r : ℝ) :

                      The positive occupation kernel lies in its sharp constant interval.

                      theorem BGW.StableTrees.supCorrection_zero {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {ε : ℝ} (hε : 0 < ε) :
                      supCorrection θ ε 0 = -if θ = 2 then ε / 2 else 0

                      The correction at the reflecting boundary.

                      theorem BGW.StableTrees.supPotential_zero_mul {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) {q : ℝ} (hq : 0 < q) :
                      q ^ (1 / θ) * supPotential θ q 0 = q ^ (2 / θ - 1)

                      The boundary potential gives the Brownian correction exponent.

                      theorem BGW.StableTrees.tendsto_rpow_two_div_sub_one {θ : ℝ} (hθ : 1 < θ ∧ θ ≤ 2) :
                      Filter.Tendsto (fun (q : ℝ) => q ^ (2 / θ - 1)) (nhdsWithin 0 (Set.Ioi 0)) (nhds (if θ = 2 then 1 else 0))

                      The scalar correction exponent distinguishes the Brownian endpoint.