2020
DOI: 10.48550/arxiv.2003.02406
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Surface-localized transmission eigenstates, super-resolution imaging and pseudo surface plasmon modes

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Cited by 3 publications
(8 citation statements)
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“…That is, all the results hold for the partial-data transmission eigenvalue problem, namely in (1.2) the transmission boundary conditions on ∂Ω is required to hold only in a small neighbourhood of the corner point. It is mentioned that a global rigidity result of the geometric structure of the transmission eigenfunctions was presented in [14].…”
Section: Lemma 11 ( [23])mentioning
confidence: 99%
“…That is, all the results hold for the partial-data transmission eigenvalue problem, namely in (1.2) the transmission boundary conditions on ∂Ω is required to hold only in a small neighbourhood of the corner point. It is mentioned that a global rigidity result of the geometric structure of the transmission eigenfunctions was presented in [14].…”
Section: Lemma 11 ( [23])mentioning
confidence: 99%
“…Moreover, it can be shown (cf. [7,26]) that invisibility occurs for an incident field u i if and only if (u| Ω , u i | Ω ) is a pair of transmission eigenfunctions associated with the transmission eigenvalue k 2 and the target scatterer (Ω, V ). Hence, for the good sake of invisibility, one should expect the transmission eigenvalues and transmission eigenfunctions of (3.20) should be as "dense" as possible, and this is in sharp difference to that for the LSM which requires the "sparse" the better; see our discussion in Section 2.2.…”
Section: More Connections To Inverse Scattering Problems and Invisibi...mentioning
confidence: 99%
“…Let 0 < k 2 1 ≤ k 2 2 ≤ • • • ≤ k 2 j → +∞ denote the real transmission eigenvalues, and (u k j , v k j ) be the corresponding pair of transmission eigenfunctions associated with the eigenvalue k 2 j . It is shown in [26,27] that there exists a subsequence (k jn ) ⊂ (k j ) with k 2 jn → +∞ as n → +∞ such that either (u jn ) is a sequence of surface-localized eigenstates or (v jn ) is a sequence of surface-localized eigenstates. The existence of surface-localized (u jn ) or (v jn ) depends on V .…”
Section: Lemma 42 ( [7]mentioning
confidence: 99%
“…There are several further studies on the locally vanishing property of the transmission eigenfunctions in different physical scenarios [6,8,12,14,17]. In [19], a global rigidity property is discovered, showing that the transmission eigenfunctions tend to localize on ∂Ω. Both the local and global geometric structures of transmission eigenfunctions can produce interesting and significant applications.…”
mentioning
confidence: 99%
“…Second, they have been used to establish novel unique identifiability results for the inverse scattering problems by a single far-field measurement [6, 8, 10-12, 17, 18, 26, 36, 37], which constitutes a longstanding problem in the inverse scattering theory [20,39]. Furthermore, in [19], a super-resolution wave imaging scheme was developed by making use the geometric properties of the transmission eigenfunctions.…”
mentioning
confidence: 99%