2015
DOI: 10.1007/s10444-015-9406-3
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Electromagnetic inverse shape problem for coated obstacles

Abstract: We address the inverse problem of retrieving the shape of an obstacle with impedance in the form of a surface wave operator using the knowledge of electromagnetic scattering amplitude at a fixed frequency. We prove unique reconstructions from infinitely many measures. We then provide a characterization of the scattering amplitude derivative with respect to the obstacle shape. This derivative includes the case of shape dependent impedance parameters. We then employ a gradientdescent algorithm with H 1 boundary … Show more

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Cited by 2 publications
(3 citation statements)
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“…We extend the Lagrangian approach to derive the shape gradient on the basis of complex‐valued solutions of adjoint P and state E boundary value problems. The shape sensitivity analysis for Maxwell's equations gets more complicated because of the regularity preservation . In Section 2, it is discussed that we need to use the covariant transformation to guarantee that solutions of adjoint and state problems in the mapped domain are still H (curl; Ω) functions.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…We extend the Lagrangian approach to derive the shape gradient on the basis of complex‐valued solutions of adjoint P and state E boundary value problems. The shape sensitivity analysis for Maxwell's equations gets more complicated because of the regularity preservation . In Section 2, it is discussed that we need to use the covariant transformation to guarantee that solutions of adjoint and state problems in the mapped domain are still H (curl; Ω) functions.…”
Section: Introductionmentioning
confidence: 99%
“…The shape sensitivity analysis for Maxwell's equations gets more complicated because of the regularity preservation. 14,15 In Section 2, it is discussed that we need to use the covariant transformation to guarantee that solutions of adjoint and state problems in the mapped domain are still H(curl; Ω) functions. The final formula is of a volume integral, which is continuous in the energy norm and well defined on the natural variational space.…”
Section: Introductionmentioning
confidence: 99%
“…For example, we can mention the works of Cakoni et al [15,14] and Caubet et al [17] for the Laplace's equation, of Bourgeois et al [12] and Kateb et al [37] for the Helmholtz equation and of Chaulet et al [19] for the Maxwell's equations.…”
Section: Introduction and General Notationsmentioning
confidence: 99%