On the forward in time propagation of zeros in fractional heat type problems
Abstract
In this short note we prove that if u solves (∂t - )s u = Vu in Rnx × Rt, and vanishes to infinite order at a point (x0, t0), then u 0 in Rnx × Rt. This sharpens (and completes) our earlier result that proves u(·, t) 0 for t ≤ t0 if it vanishes to infinite order at (x0, t0).
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