Conformal mapping for cavity inverse problem: an explicit reconstruction formula

Abstract

International audienceIn this paper, we address a classical case of the Calder\'on (or conductivity) inverse problem in dimension two. We aim to recover the location and the shape of a single cavity ω\omega (with boundary γ\gamma) contained in a domain Ω\Omega (with boundary Γ\Gamma) from the knowledge of the Dirichlet-to-Neumann (DtN) map Λγ:fnufΓ\Lambda_\gamma: f \longmapsto \partial_n u^f|_{\Gamma}, where ufu^f is harmonic in Ωω\Omega\setminus\overline{\omega}, ufΓ=fu^f|_{\Gamma}=f and ufγ=cfu^f|_{\gamma}=c^f, cfc^f being the constant such that γnufds=0\int_{\gamma}\partial_n u^f\,{\rm d}s=0. We obtain an explicit formula for the complex coefficients ama_m arising in the expression of the Riemann map za1z+a0+m1amzmz\longmapsto a_1 z + a_0 + \sum_{m\leqslant -1} a_m z^{m} that conformally maps the exterior of the unit disk onto the exterior of ω\omega. This formula is derived by using two ingredients: a new factorization result of the DtN map and the so-called generalized P\'olia-Szeg\"o tensors (GPST) of the cavity. As a byproduct of our analysis, we also prove the analytic dependence of the coefficients ama_m with respect to the DtN. Numerical results are provided to illustrate the efficiency and simplicity of the method

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