Finite grids for the minimum time of the stable bridge #
The closed stable bridge has cyclically invariant grid increments and an atomless minimum time. Cyclic invariance follows by composing full reversal with reversal of the strict prefix. These are the finite-grid inputs to the uniform minimum-time law.
Reference: J. Bertoin, Lévy Processes, Cambridge University Press, 1996, Chapter VIII (Vervaat's transformation and the uniform law of the minimum time); L. Chaumont, Excursion normalisée, méandre et pont pour les processus de Lévy stables, Bull. Sci. Math. 121 (1997), 377–403.
The grid time i/N in [0,1] (N = M + 1, i ≤ N as a natural number).
Equations
- BGW.StableTrees.gridTime M i = Set.projIcc 0 1 BGW.StableTrees.gridTime._proof_1 (↑i / (↑M + 1))
Instances For
Grid increments f((i+1)/N) - f(i/N), i < N.
Equations
- BGW.StableTrees.gridIncr M f i = f (BGW.StableTrees.gridTime M (↑i + 1)) - f (BGW.StableTrees.gridTime M ↑i)
Instances For
Evaluation of the complete grid-increment vector is measurable.
Reversing all coordinates preserves the bridge grid-increment law.
The increments preceding the terminal grid interval are exchangeable.
Exchangeability of the bridge increments under cyclic shifts of the grid.
No deterministic time can be the minimum time of the stable bridge.
Values on the grid excluding the duplicate terminal endpoint.
Equations
- BGW.StableTrees.bridgeGridValues M f i = f (BGW.StableTrees.gridTime M ↑i)
Instances For
The finite-grid values are measurable.
On a loop the final grid increment wraps back to the initial value.