Ladder exponent algebra and Laplace functionals #
Algebra of the exact ladder exponent and the boundary and ladder Laplace functionals.
The boundary potential of the path: ∫_{(0,∞)} e^{-qt-λS_t} dM_t, M = supLocalTime
(Stieltjes measure supLocalTimeStieltjes), in ℝ≥0∞ (no junk).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The ladder Laplace transform φ_{q,λ}(z) = E exp(-q A_z - λ B_z).
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
BGW.StableTrees.inv_supLadderExponent_eq_integral
{θ : ℝ}
(hθ : 1 < θ ∧ θ ≤ 2)
{q lam : ℝ}
(hq : 0 < q)
(hlam : 0 ≤ lam)
:
(supLadderExponent θ q lam)⁻¹ = q ^ (1 / θ) / q * ∫ (p : Skorokhod.DLoc × ℝ), Real.exp (-lam * supRunning p.1 p.2.toNNReal) ∂expClockLaw θ q
1/κ is the mean potential (Φ/q) F_q(λ), including the diagonal
(F_q(Φ) = 1/θ, from BGW.StableTrees.SupremumDrawdown). Pure algebra from
integral_exp_neg_supRunning_expTime; no ladder object enters.
Reference: Bertoin, Lévy Processes, Chapter VI.
theorem
BGW.StableTrees.tendsto_supLadderExponent_zero
{θ : ℝ}
(hθ : 1 < θ ∧ θ ≤ 2)
{lam : ℝ}
(hlam : 0 ≤ lam)
:
Filter.Tendsto (fun (q : ℝ) => supLadderExponent θ q lam) (nhdsWithin 0 (Set.Ioi 0)) (nhds (supLadderExponent θ 0 lam))
Continuity of κ in q ↓ 0 at fixed λ ≥ 0 (to κ(0,λ) = λ^{θ-1}; at λ = 0 the
value is 0), needed to pass from q > 0 to q = 0.