2020
DOI: 10.1017/s0956792520000364
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Thin-layer solutions of the Helmholtz equation

Abstract: This paper gives a brief overview of some configurations in which high-frequency wave propagation modelled by Helmholtz equation gives rise to solutions that vary rapidly across thin layers. The configurations are grouped according to their mathematical structure and tractability and one of them concerns a famous open problem of mathematical physics.

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Cited by 7 publications
(5 citation statements)
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“…We have explored the simplest problem of diffraction on non-smooth contours, where the incidence is tangential and the contour curvature changes with jump. We hope that the developed technique will be useful in the study of similar problems with concave-convex transitions, which attract significant attention in the smooth case (see, e.g., [9,10,12,13,14,15,16,17,18]).…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…We have explored the simplest problem of diffraction on non-smooth contours, where the incidence is tangential and the contour curvature changes with jump. We hope that the developed technique will be useful in the study of similar problems with concave-convex transitions, which attract significant attention in the smooth case (see, e.g., [9,10,12,13,14,15,16,17,18]).…”
Section: Discussionmentioning
confidence: 99%
“…There are two reasons for revisiting this problem. First, for half a century, steady interest has been seen in the description of the effects of high-frequency diffraction by contours in which the curvature is neither strictly positive nor strictly negative (see, e.g., [7,8,9,10,11,12,13,14,1,15,16,17,18,19]). A.…”
Section: Introductionmentioning
confidence: 99%
“…On the convex side, there are no whispering-gallery modes; instead, there are creeping waves and rays [26][27][28][29] propagating close to the mirror while getting weaker as they shed waves tangentially into the space above. The whispering-gallery modes and the creeping waves are well understood, but the transformation of one into the other across an inflection is not [30][31][32].…”
Section: Discussionmentioning
confidence: 99%
“…Importantly the point τ = 0, corresponding to t → +∞, remains a regular point for (22) hence with a well-defined (strong) limit of Ũ0 (τ, τ 1 ) as τ → 0+. Using now the transformation (13) in reverse, determines the unitary propagator U 0 (t, t 1 ) for the unperturbed (i.e. with no boundary) problem for (2) with the above described asymptotic behaviour as t → +∞.…”
Section: Further Interpretations Of Theorem 1: Searchlight Wave Opera...mentioning
confidence: 99%
“…It is more convenient to work with an equivalently transformed via (13) problem for G(η, τ ) solving (22), which we re-write as…”
Section: Proof Of Theoremmentioning
confidence: 99%