Abstract
We study the Fisher-KPP equation with a fractional laplacian of order α \in (0, 1). We know that the stable state invades the unstable one at constant speed for α = 1, and at an exponential in time velocity for α \in (0, 1). The transition between these two different speeds is examined in this paper. We prove that during a time of the order - ln(1 - α), the propagation is linear and then it is exponential.
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