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Corrigendum: The enclosure method for a generalized anisotropic complex conductivity equation (2021 Inverse Problems 37 055010)

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In the proof of theorem 4.1, the sequence Uη, j, which is established in lemma 3.4, only converges in Ωt to the oscillating decaying solution uω,t,χt ,ξ,N . Therefore, we… Click to show full abstract

In the proof of theorem 4.1, the sequence Uη, j, which is established in lemma 3.4, only converges in Ωt to the oscillating decaying solution uω,t,χt ,ξ,N . Therefore, we can not use (4.2) when t > t∗, and the assertion in case (b) is incorrect. We have to modify it to be an assertion about t = t∗, which corresponds to the case when Ωt and D are just touched, and in doing so we need the stronger assumption that D has a Lipschitz boundary. With this modification, it turns out that |Iω,t,χt(τ )| in (b) has a lower bound of order τ 2−n, while that in (a) is of exponential decay in τ . The modified statement is given below.

Keywords: anisotropic complex; method generalized; corrigendum enclosure; generalized anisotropic; inverse problems; enclosure method

Journal Title: Inverse Problems
Year Published: 2021

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