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Math."],"published-print":{"date-parts":[[2023,4]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>We say that <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, the boundary of a bounded Lipschitz domain, is locally dilation invariant if, at each <jats:inline-formula><jats:alternatives><jats:tex-math>$$x\\in \\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>x<\/mml:mi>\n                    <mml:mo>\u2208<\/mml:mo>\n                    <mml:mi>\u0393<\/mml:mi>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> is either locally <jats:inline-formula><jats:alternatives><jats:tex-math>$$C^1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msup>\n                    <mml:mi>C<\/mml:mi>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:msup>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> or locally coincides (in some coordinate system centred at <jats:italic>x<\/jats:italic>) with a Lipschitz graph <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma _x$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>\u0393<\/mml:mi>\n                    <mml:mi>x<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> such that <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma _x=\\alpha _x\\Gamma _x$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msub>\n                      <mml:mi>\u0393<\/mml:mi>\n                      <mml:mi>x<\/mml:mi>\n                    <\/mml:msub>\n                    <mml:mo>=<\/mml:mo>\n                    <mml:msub>\n                      <mml:mi>\u03b1<\/mml:mi>\n                      <mml:mi>x<\/mml:mi>\n                    <\/mml:msub>\n                    <mml:msub>\n                      <mml:mi>\u0393<\/mml:mi>\n                      <mml:mi>x<\/mml:mi>\n                    <\/mml:msub>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, for some <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\alpha _x\\in (0,1)$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msub>\n                      <mml:mi>\u03b1<\/mml:mi>\n                      <mml:mi>x<\/mml:mi>\n                    <\/mml:msub>\n                    <mml:mo>\u2208<\/mml:mo>\n                    <mml:mrow>\n                      <mml:mo>(<\/mml:mo>\n                      <mml:mn>0<\/mml:mn>\n                      <mml:mo>,<\/mml:mo>\n                      <mml:mn>1<\/mml:mn>\n                      <mml:mo>)<\/mml:mo>\n                    <\/mml:mrow>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. In this paper we study, for such <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, the essential spectrum of <jats:inline-formula><jats:alternatives><jats:tex-math>$$D_\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>D<\/mml:mi>\n                    <mml:mi>\u0393<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, the double-layer (or Neumann\u2013Poincar\u00e9) operator of potential theory, on <jats:inline-formula><jats:alternatives><jats:tex-math>$$L^2(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msup>\n                      <mml:mi>L<\/mml:mi>\n                      <mml:mn>2<\/mml:mn>\n                    <\/mml:msup>\n                    <mml:mrow>\n                      <mml:mo>(<\/mml:mo>\n                      <mml:mi>\u0393<\/mml:mi>\n                      <mml:mo>)<\/mml:mo>\n                    <\/mml:mrow>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. We show, via localisation and Floquet\u2013Bloch-type arguments, that this essential spectrum is the union of the spectra of related continuous families of operators <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_t$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>K<\/mml:mi>\n                    <mml:mi>t<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, for <jats:inline-formula><jats:alternatives><jats:tex-math>$$t\\in [-\\pi ,\\pi ]$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>t<\/mml:mi>\n                    <mml:mo>\u2208<\/mml:mo>\n                    <mml:mo>[<\/mml:mo>\n                    <mml:mo>-<\/mml:mo>\n                    <mml:mi>\u03c0<\/mml:mi>\n                    <mml:mo>,<\/mml:mo>\n                    <mml:mi>\u03c0<\/mml:mi>\n                    <mml:mo>]<\/mml:mo>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>; moreover, each <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_t$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>K<\/mml:mi>\n                    <mml:mi>t<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> is compact if <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> is <jats:inline-formula><jats:alternatives><jats:tex-math>$$C^1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msup>\n                    <mml:mi>C<\/mml:mi>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:msup>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> except at finitely many points. For the 2D case where, additionally, <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> is piecewise analytic, we construct convergent sequences of approximations to the essential spectrum of <jats:inline-formula><jats:alternatives><jats:tex-math>$$D_\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>D<\/mml:mi>\n                    <mml:mi>\u0393<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>; each approximation is the union of the eigenvalues of finitely many finite matrices arising from Nystr\u00f6m-method approximations to the operators <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_t$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>K<\/mml:mi>\n                    <mml:mi>t<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. Through error estimates with explicit constants, we also construct functionals that determine whether any particular locally-dilation-invariant piecewise-analytic <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> satisfies the well-known spectral radius conjecture, that the essential spectral radius of <jats:inline-formula><jats:alternatives><jats:tex-math>$$D_\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>D<\/mml:mi>\n                    <mml:mi>\u0393<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> on <jats:inline-formula><jats:alternatives><jats:tex-math>$$L^2(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msup>\n                      <mml:mi>L<\/mml:mi>\n                      <mml:mn>2<\/mml:mn>\n                    <\/mml:msup>\n                    <mml:mrow>\n                      <mml:mo>(<\/mml:mo>\n                      <mml:mi>\u0393<\/mml:mi>\n                      <mml:mo>)<\/mml:mo>\n                    <\/mml:mrow>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> is <jats:inline-formula><jats:alternatives><jats:tex-math>$$&lt;1\/2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mo>&lt;<\/mml:mo>\n                    <mml:mn>1<\/mml:mn>\n                    <mml:mo>\/<\/mml:mo>\n                    <mml:mn>2<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> for all Lipschitz <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u0393<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. We illustrate this theory with examples; for each we show that the essential spectral radius <jats:italic>is<\/jats:italic><jats:inline-formula><jats:alternatives><jats:tex-math>$$&lt;1\/2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mo>&lt;<\/mml:mo>\n                    <mml:mn>1<\/mml:mn>\n                    <mml:mo>\/<\/mml:mo>\n                    <mml:mn>2<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, providing additional support for the conjecture. We also, via new results on the invariance of the essential spectral radius under locally-conformal <jats:inline-formula><jats:alternatives><jats:tex-math>$$C^{1,\\beta }$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msup>\n                    <mml:mi>C<\/mml:mi>\n                    <mml:mrow>\n                      <mml:mn>1<\/mml:mn>\n                      <mml:mo>,<\/mml:mo>\n                      <mml:mi>\u03b2<\/mml:mi>\n                    <\/mml:mrow>\n                  <\/mml:msup>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> diffeomorphisms, show that the spectral radius conjecture holds for all Lipschitz curvilinear polyhedra.\n<\/jats:p>","DOI":"10.1007\/s00211-023-01353-z","type":"journal-article","created":{"date-parts":[[2023,5,3]],"date-time":"2023-05-03T17:01:57Z","timestamp":1683133317000},"page":"635-699","update-policy":"http:\/\/dx.doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":1,"title":["On the spectrum of the double-layer operator on locally-dilation-invariant Lipschitz domains"],"prefix":"10.1007","volume":"153","author":[{"given":"Simon N.","family":"Chandler-Wilde","sequence":"first","affiliation":[]},{"given":"Raffael","family":"Hagger","sequence":"additional","affiliation":[]},{"given":"Karl-Mikael","family":"Perfekt","sequence":"additional","affiliation":[]},{"given":"Jani A.","family":"Virtanen","sequence":"additional","affiliation":[]}],"member":"297","published-online":{"date-parts":[[2023,5,3]]},"reference":[{"key":"1353_CR1","doi-asserted-by":"crossref","first-page":"109","DOI":"10.1007\/s00205-015-0928-0","volume":"220","author":"H Ammari","year":"2016","unstructured":"Ammari, H., Deng, Y., Millien, P.: Surface plasmon resonance of nanoparticles and applications in imaging. 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