The law of the supremum of a stable L\'evy process with no negative jumps

Abstract

Let X=(Xt)t0 be a stable L\'evy process of index α ∈(1,2) with no negative jumps and let St=0 s tXs denote its running supremum for t>0. We show that the density function ft of St can be characterized as the unique solution to a weakly singular Volterra integral equation of the first kind or, equivalently, as the unique solution to a first-order Riemann--Liouville fractional differential equation satisfying a boundary condition at zero. This yields an explicit series representation for ft. Recalling the familiar relation between St and the first entry time τx of X into [x,∞), this further translates into an explicit series representation for the density function of τx.

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