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Math."],"published-print":{"date-parts":[[2022,2]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>It is well known that, with a particular choice of norm, the classical double-layer potential operator<jats:italic>D<\/jats:italic>has essential norm<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\"><mml:mrow><mml:mo>&lt;<\/mml:mo><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>as an operator on the natural trace space<jats:inline-formula><jats:alternatives><jats:tex-math>$$H^{1\/2}(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:msup><mml:mi>H<\/mml:mi><mml:mrow><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>whenever<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Gamma $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>\u0393<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>is the boundary of a bounded Lipschitz domain. This implies, for the standard second-kind boundary integral equations for the interior and exterior Dirichlet and Neumann problems in potential theory, convergence of the Galerkin method in<jats:inline-formula><jats:alternatives><jats:tex-math>$$H^{1\/2}(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:msup><mml:mi>H<\/mml:mi><mml:mrow><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>for any sequence of finite-dimensional subspaces<jats:inline-formula><jats:alternatives><jats:tex-math>$$({{\\mathcal {H}}}_N)_{N=1}^\\infty $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:msubsup><mml:mrow><mml:mo>(<\/mml:mo><mml:msub><mml:mi>H<\/mml:mi><mml:mi>N<\/mml:mi><\/mml:msub><mml:mo>)<\/mml:mo><\/mml:mrow><mml:mrow><mml:mi>N<\/mml:mi><mml:mo>=<\/mml:mo><mml:mn>1<\/mml:mn><\/mml:mrow><mml:mi>\u221e<\/mml:mi><\/mml:msubsup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>that is asymptotically dense in<jats:inline-formula><jats:alternatives><jats:tex-math>$$H^{1\/2}(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:msup><mml:mi>H<\/mml:mi><mml:mrow><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>. Long-standing open questions are whether the essential norm is also<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\"><mml:mrow><mml:mo>&lt;<\/mml:mo><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>for<jats:italic>D<\/jats:italic>as an operator 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\"><mml:mrow><mml:msup><mml:mi>L<\/mml:mi><mml:mn>2<\/mml:mn><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/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\"><mml:mi>\u0393<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>in 2-d; or whether, 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\"><mml:mi>\u0393<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>in 2-d and 3-d, or at least for the smaller class of Lipschitz polyhedra in 3-d, the weaker condition holds that the operators<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\pm \\frac{1}{2}I+D$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mo>\u00b1<\/mml:mo><mml:mfrac><mml:mn>1<\/mml:mn><mml:mn>2<\/mml:mn><\/mml:mfrac><mml:mi>I<\/mml:mi><mml:mo>+<\/mml:mo><mml:mi>D<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>are compact perturbations of coercive operators\u2014this a necessary and sufficient condition for the convergence of the Galerkin method for every sequence of subspaces<jats:inline-formula><jats:alternatives><jats:tex-math>$$({{\\mathcal {H}}}_N)_{N=1}^\\infty $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:msubsup><mml:mrow><mml:mo>(<\/mml:mo><mml:msub><mml:mi>H<\/mml:mi><mml:mi>N<\/mml:mi><\/mml:msub><mml:mo>)<\/mml:mo><\/mml:mrow><mml:mrow><mml:mi>N<\/mml:mi><mml:mo>=<\/mml:mo><mml:mn>1<\/mml:mn><\/mml:mrow><mml:mi>\u221e<\/mml:mi><\/mml:msubsup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>that is asymptotically dense in<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\"><mml:mrow><mml:msup><mml:mi>L<\/mml:mi><mml:mn>2<\/mml:mn><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>. We settle these open questions negatively. We give examples of 2-d and 3-d Lipschitz domains with Lipschitz constant equal to one for which the essential norm of<jats:italic>D<\/jats:italic>is<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\ge 1\/2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mo>\u2265<\/mml:mo><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>, and examples with Lipschitz constant two for which the operators<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\pm \\frac{1}{2}I +D$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mo>\u00b1<\/mml:mo><mml:mfrac><mml:mn>1<\/mml:mn><mml:mn>2<\/mml:mn><\/mml:mfrac><mml:mi>I<\/mml:mi><mml:mo>+<\/mml:mo><mml:mi>D<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>are not coercive plus compact. We also give, for every<jats:inline-formula><jats:alternatives><jats:tex-math>$$C&gt;0$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mi>C<\/mml:mi><mml:mo>&gt;<\/mml:mo><mml:mn>0<\/mml:mn><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>, examples of Lipschitz polyhedra for which the essential norm is<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\ge C$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mo>\u2265<\/mml:mo><mml:mi>C<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>and for which<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\lambda I+D$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mi>\u03bb<\/mml:mi><mml:mi>I<\/mml:mi><mml:mo>+<\/mml:mo><mml:mi>D<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>is not a compact perturbation of a coercive operator for any real or complex<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\lambda $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>\u03bb<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>with<jats:inline-formula><jats:alternatives><jats:tex-math>$$|\\lambda |\\le C$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mo>|<\/mml:mo><mml:mi>\u03bb<\/mml:mi><mml:mo>|<\/mml:mo><mml:mo>\u2264<\/mml:mo><mml:mi>C<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>. We then, via a new result on the Galerkin method in Hilbert spaces, explore the implications of these results for the convergence of Galerkin boundary element methods in the<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\"><mml:mrow><mml:msup><mml:mi>L<\/mml:mi><mml:mn>2<\/mml:mn><\/mml:msup><mml:mrow><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>setting. Finally, we resolve negatively a related open question in the convergence theory for collocation methods, showing that, for our polyhedral examples, there is no weighted norm on<jats:inline-formula><jats:alternatives><jats:tex-math>$$C(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mi>C<\/mml:mi><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>, equivalent to the standard supremum norm, for which the essential norm of<jats:italic>D<\/jats:italic>on<jats:inline-formula><jats:alternatives><jats:tex-math>$$C(\\Gamma )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow><mml:mi>C<\/mml:mi><mml:mo>(<\/mml:mo><mml:mi>\u0393<\/mml:mi><mml:mo>)<\/mml:mo><\/mml:mrow><\/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\"><mml:mrow><mml:mo>&lt;<\/mml:mo><mml:mn>1<\/mml:mn><mml:mo>\/<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>.<\/jats:p>","DOI":"10.1007\/s00211-021-01256-x","type":"journal-article","created":{"date-parts":[[2021,12,24]],"date-time":"2021-12-24T16:02:50Z","timestamp":1640361770000},"page":"299-371","update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":7,"title":["Coercivity, essential norms, and the Galerkin method for second-kind integral equations on polyhedral and Lipschitz domains"],"prefix":"10.1007","volume":"150","author":[{"given":"S. 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