Abstract
We consider the barrier crossing in a bistable potential for a random-walk process that is driven by Lévy noise of stable index α. It is shown that the survival probability decays exponentially, but with a power law dependence Tc(α,D) = C(α)D−μ(α) of the mean escape time on the noise intensity D. Here C is a constant, and the exponent μ varies slowly over a large range of the stable index α∊[1,2). For the Cauchy case, we explicitly calculate the escape rate.