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Let be a stable L'{e}vy process of index with no negative jumps and let denote its running supremum for . We show that the density function of 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 . Recalling the familiar relation between and the first entry time of into , this further translates into an explicit series representation for the density function of .

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