2016
DOI: 10.1016/j.jde.2016.01.033
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An inverse stability result for non-compactly supported potentials by one arbitrary lateral Neumann observation

Abstract: International audienceIn this paper we investigate the inverse problem of determining the time independent scalar potential of the dynamic Schrödinger equation in an infinite cylindrical domain, from partial measurement of the solution on the boundary. Namely, if the potential is known in a neighborhood of the boundary of the spatial domain, we prove that it can be logarithmic stably determined in the whole waveguide from a single observation of the solution on any arbitrary strip-shaped subset of the boundary

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Cited by 23 publications
(32 citation statements)
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“…Let us mention that inverse boundary value problems in an infinite slab were addressed by Yang in [Y] for bi-harmonic operators. Recently, several stability results were derived in [CS,Ki,KPS1,KPS2,BKS] for non compactly supported coefficients inverse problems in an infinite waveguide with a bounded cross section. More specifically, we refer to [KKS, CKS] for the analysis of inverse problems in the framework of a periodic cylindrical domain examined in this paper.…”
Section: Introductionmentioning
confidence: 99%
“…Let us mention that inverse boundary value problems in an infinite slab were addressed by Yang in [Y] for bi-harmonic operators. Recently, several stability results were derived in [CS,Ki,KPS1,KPS2,BKS] for non compactly supported coefficients inverse problems in an infinite waveguide with a bounded cross section. More specifically, we refer to [KKS, CKS] for the analysis of inverse problems in the framework of a periodic cylindrical domain examined in this paper.…”
Section: Introductionmentioning
confidence: 99%
“…Let n be the outward unit normal vector of ∂Ω. 1 Since Ω is only subjected to the condition Ω ⊂ Ω 1 we may have Ω = Ω 1 this is why we use a different notation for the outward unit normal vector of Ω 1 and Ω. Before we state our result, let us also recall that for any A ∈ L ∞ (Ω) 3 satisfying div(A) ∈ L ∞ (Ω), we can define the trace map A · n as the unique element of…”
Section: Statement Of the Main Resultsmentioning
confidence: 99%
“…In this section we will complete the proof of Theorem 1.1. We fix q = q 2 − q 1 on and we extend it by q = 0 on R 3 \ . We assume that the constant ε given in the beginning of § 4 is chosen in such a way that for any θ ∈ {y ∈ S 1 : |y − θ 0 | ε} we have ∂ω −,ε,θ ⊂ G .…”
Section: Uniqueness Resultsmentioning
confidence: 99%