Abstract
In the proof of Proposition A.2 of Appendix in our published paper [1], we used the continuity of the normal derivative of q(x) at @G. This is not true because q(x) is not a double layer potential. A correct proof can be given as follows: Let R(') = 0 with ' 2 H 1=2(@G). Then z = S['] satisfies (Formula Presented). By the unique continuation property of solutions of the Laplace equation, we have S['] = z = 0 on @G. Then by the bijectivity of S : H-1,2(@G) ! H-1,2(@G) given in Proposition A.1, we have ' = 0, which proves the injectivity of R.
| Original language | English |
|---|---|
| Pages (from-to) | 907 |
| Number of pages | 1 |
| Journal | Inverse Problems and Imaging |
| Volume | 17 |
| Issue number | 4 |
| DOIs |
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| State | Published - Aug 2023 |