Predicting the ultimate supremum of a stable L\'evy process with no negative jumps

Abstract

Given a stable L\'evy process X=(Xt)0 t T of index α∈(1,2) with no negative jumps, and letting St=0 s tXs denote its running supremum for t∈ [0,T], we consider the optimal prediction problem \[V=∈f0τ TE(ST-Xτ)p,\] where the infimum is taken over all stopping times τ of X, and the error parameter p∈(1,α) is given and fixed. Reducing the optimal prediction problem to a fractional free-boundary problem of Riemann--Liouville type, and finding an explicit solution to the latter, we show that there exists α*∈(1,2) (equal to 1.57 approximately) and a strictly increasing function p*:(α*,2)→(1,2) satisfying p*(α*+)=1, p*(2-)=2 and p*(α)<α for α∈(α*,2) such that for every α∈ (α*,2) and p∈(1,p*(α)) the following stopping time is optimal \[τ*=∈f\t∈[0,T]:St-Xt z*(T-t)1/α\,\] where z*∈(0,∞) is the unique root to a transcendental equation (with parameters α and p). Moreover, if either α∈(1,α*) or p∈(p*(α),α) then it is not optimal to stop at t∈[0,T) when St-Xt is sufficiently large. The existence of the breakdown points α* and p*(α) stands in sharp contrast with the Brownian motion case (formally corresponding to α=2), and the phenomenon itself may be attributed to the interplay between the jump structure (admitting a transition from lighter to heavier tails) and the individual preferences (represented by the error parameter p).

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