A further quantification of the unique continuation properties of eigenfunctions of the magnetic Schrödinger operator

preprint2015arXivOpen access

Abstract

We prove quantitative unique continuation results for solutions of Δw−k2w=Vw+W⋅∇wΔw - k^2 w = V w + W\cdot \nabla w in a neighborhood of infinity, where k>0k > 0, and VV and WW are complex-valued decaying potentials that satisfy ∣V(x)∣≲∣x∣−N|V(x)| \lesssim |x|^{-N} and ∣W(x)∣≲∣x∣−P|W(x)| \lesssim |x|^{-P} for some N,P>1N, P > 1. For M(R,4n/k)=inf⁡{∣∣w∣∣L2(B4n/k(x0)):∣x0∣=R}M(R, 4n/k) = \inf \{||w||_{L^2(B_{4n/k}(x_0))} : |x_0| = R \}, we show that if the solution ww is non-zero, bounded, and normalized, then M(R,4n/k)≳exp⁡(−kR−Glog⁡R)M(R, 4n/k) \gtrsim \exp(-kR - G \log R), where G>n−12G > \frac{n-1}{2} is a constant. An examination of radial solutions to Δw−k2w=Vw+W⋅∇wΔw - k^2 w = V w + W\cdot \nabla w shows that this new estimate for M(R,4n/k)M(R, 4n/k) is sharp up to logarithmic terms.

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