The unconditional stable law and its convolution semigroup #
This module packages the scalar stable density as a probability measure for every
1 < θ ≤ 2, identifies its Laplace and characteristic transforms, and proves the time
semigroup for the corresponding laws and densities.
References: V. M. Zolotarev, One-dimensional Stable Distributions, 1986; K. Sato, Lévy Processes and Infinitely Divisible Distributions, 1999, §14; W. Feller, An Introduction to Probability Theory and Its Applications, vol. II, ch. XVII.
The spectrally positive θ-stable law, normalized by E[exp(-λ X)] = exp(λ^θ), for
1 < θ ≤ 2; the Dirac mass at 0 outside this range (a junk value).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The stable law has density Scalar.stableDensity θ (C15.1).
The stable law is the only probability measure with this Laplace transform (C15.1).
At θ = 2 the stable law is the centered Gaussian of variance 2 (C15; §1.1).
The density of the stable law at time t > 0: t^{-1/θ} p₁(t^{-1/θ} x) (C15.4).
Equations
- BGW.StableTrees.stableDensityAt θ t x = t ^ (-1 / θ) * BGW.StableTrees.Scalar.stableDensity θ (t ^ (-1 / θ) * x)
Instances For
The stable law at time t > 0, image of stableLaw θ under x ↦ t^{1/θ} x (C15.4).
Equations
- BGW.StableTrees.stableLawAt θ t = (BGW.StableTrees.stableLaw θ).map fun (x : ℝ) => t ^ (1 / θ) * x
Instances For
stableLawAt θ t has density stableDensityAt θ t (C15.4).