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Math."],"published-print":{"date-parts":[[2023,1]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>For the spectral fractional diffusion operator of order 2<jats:italic>s<\/jats:italic>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$s \\in (0,1)$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>s<\/mml:mi>\n                    <mml:mo>\u2208<\/mml:mo>\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:math><\/jats:alternatives><\/jats:inline-formula>, in bounded, curvilinear polygonal domains <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\varOmega \\subset {{\\mathbb {R}}}^2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>\u03a9<\/mml:mi>\n                    <mml:mo>\u2282<\/mml:mo>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mi>R<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mn>2<\/mml:mn>\n                    <\/mml:msup>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> we prove exponential convergence of two classes of <jats:italic>hp<\/jats:italic> discretizations under the assumption of analytic data (coefficients and source terms, without any boundary compatibility), in the natural fractional Sobolev norm <jats:inline-formula><jats:alternatives><jats:tex-math>$${\\mathbb {H}}^s(\\varOmega )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mi>H<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mi>s<\/mml:mi>\n                    <\/mml:msup>\n                    <mml:mrow>\n                      <mml:mo>(<\/mml:mo>\n                      <mml:mi>\u03a9<\/mml:mi>\n                      <mml:mo>)<\/mml:mo>\n                    <\/mml:mrow>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. The first <jats:italic>hp<\/jats:italic> discretization is based on writing the solution as a co-normal derivative of a <jats:inline-formula><jats:alternatives><jats:tex-math>$$2+1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mn>2<\/mml:mn>\n                    <mml:mo>+<\/mml:mo>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>-dimensional local, linear elliptic boundary value problem, to which an <jats:italic>hp<\/jats:italic>-FE discretization is applied. A diagonalization in the extended variable reduces the numerical approximation of the inverse of the spectral fractional diffusion operator to the numerical approximation of a system of <jats:italic>local, decoupled, second order reaction-diffusion equations in<\/jats:italic><jats:inline-formula><jats:alternatives><jats:tex-math>$$\\varOmega $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u03a9<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. Leveraging results on robust exponential convergence of <jats:italic>hp<\/jats:italic>-FEM for second order, linear reaction diffusion boundary value problems in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\varOmega $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u03a9<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, exponential convergence rates for solutions <jats:inline-formula><jats:alternatives><jats:tex-math>$$u\\in {\\mathbb {H}}^s(\\varOmega )$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>u<\/mml:mi>\n                    <mml:mo>\u2208<\/mml:mo>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mi>H<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mi>s<\/mml:mi>\n                    <\/mml:msup>\n                    <mml:mrow>\n                      <mml:mo>(<\/mml:mo>\n                      <mml:mi>\u03a9<\/mml:mi>\n                      <mml:mo>)<\/mml:mo>\n                    <\/mml:mrow>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> of <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\mathcal {L}^s u = f$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mi>L<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mi>s<\/mml:mi>\n                    <\/mml:msup>\n                    <mml:mi>u<\/mml:mi>\n                    <mml:mo>=<\/mml:mo>\n                    <mml:mi>f<\/mml:mi>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> follow. Key ingredient in this <jats:italic>hp<\/jats:italic>-FEM are <jats:italic>boundary fitted meshes with geometric mesh refinement towards<\/jats:italic><jats:inline-formula><jats:alternatives><jats:tex-math>$$\\partial \\varOmega $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>\u2202<\/mml:mi>\n                    <mml:mi>\u03a9<\/mml:mi>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. The second discretization is based on exponentially convergent numerical sinc quadrature approximations of the Balakrishnan integral representation of <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\mathcal {L}^{-s}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msup>\n                    <mml:mrow>\n                      <mml:mi>L<\/mml:mi>\n                    <\/mml:mrow>\n                    <mml:mrow>\n                      <mml:mo>-<\/mml:mo>\n                      <mml:mi>s<\/mml:mi>\n                    <\/mml:mrow>\n                  <\/mml:msup>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> combined with <jats:italic>hp<\/jats:italic>-FE discretizations of a <jats:italic>decoupled system of local, linear, singularly perturbed reaction-diffusion equations in<\/jats:italic><jats:inline-formula><jats:alternatives><jats:tex-math>$$\\varOmega $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u03a9<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. The present analysis for either approach extends to (polygonal subsets <jats:inline-formula><jats:alternatives><jats:tex-math>$${\\widetilde{\\mathcal {M}}}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mover>\n                    <mml:mi>M<\/mml:mi>\n                    <mml:mo>~<\/mml:mo>\n                  <\/mml:mover>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> of) analytic, compact 2-manifolds <jats:inline-formula><jats:alternatives><jats:tex-math>$${\\mathcal {M}}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>M<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>, parametrized by a global, analytic chart <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\chi $$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mi>\u03c7<\/mml:mi>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> with polygonal Euclidean parameter domain <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\varOmega \\subset {{\\mathbb {R}}}^2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>\u03a9<\/mml:mi>\n                    <mml:mo>\u2282<\/mml:mo>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mi>R<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mn>2<\/mml:mn>\n                    <\/mml:msup>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>. Numerical experiments for model problems in nonconvex polygonal domains and with incompatible data confirm the theoretical results. Exponentially small bounds on Kolmogorov <jats:italic>n<\/jats:italic>-widths of solution sets for spectral fractional diffusion in curvilinear polygons and for analytic source terms are deduced.<\/jats:p>","DOI":"10.1007\/s00211-022-01329-5","type":"journal-article","created":{"date-parts":[[2022,12,2]],"date-time":"2022-12-02T16:33:10Z","timestamp":1669998790000},"page":"1-47","update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":10,"title":["Exponential convergence of hp FEM for spectral fractional diffusion in polygons"],"prefix":"10.1007","volume":"153","author":[{"given":"Lehel","family":"Banjai","sequence":"first","affiliation":[]},{"given":"Jens M.","family":"Melenk","sequence":"additional","affiliation":[]},{"given":"Christoph","family":"Schwab","sequence":"additional","affiliation":[]}],"member":"297","published-online":{"date-parts":[[2022,12,2]]},"reference":[{"key":"1329_CR1","doi-asserted-by":"crossref","unstructured":"Ainsworth, M., Glusa, C.: Hybrid finite element-spectral method for the fractional Laplacian: approximation theory and efficient solver. 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