[{"type":"journal_article","publication":"Nonlinearity","abstract":[{"text":"<jats:title>Abstract</jats:title>\r\n               <jats:p>The Neumann problem for the Keller-Segel system <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mtable columnalign=\"left\" displaystyle=\"true\">\r\n                              <mml:mtr>\r\n                                 <mml:mtd>\r\n                                    <mml:mrow>\r\n                                       <mml:mo>{</mml:mo>\r\n                                       <mml:mtable columnalign=\"left\" displaystyle=\"true\">\r\n                                          <mml:mtr>\r\n                                             <mml:mtd>\r\n                                                <mml:msub>\r\n                                                   <mml:mi>u</mml:mi>\r\n                                                   <mml:mi>t</mml:mi>\r\n                                                </mml:msub>\r\n                                                <mml:mo>=</mml:mo>\r\n                                                <mml:mi mathvariant=\"normal\">∇</mml:mi>\r\n                                                <mml:mo>⋅</mml:mo>\r\n                                                <mml:mrow>\r\n                                                   <mml:mo>(</mml:mo>\r\n                                                   <mml:mi>D</mml:mi>\r\n                                                   <mml:mrow>\r\n                                                      <mml:mo>(</mml:mo>\r\n                                                      <mml:mi>u</mml:mi>\r\n                                                      <mml:mo>)</mml:mo>\r\n                                                   </mml:mrow>\r\n                                                   <mml:mi mathvariant=\"normal\">∇</mml:mi>\r\n                                                   <mml:mi>u</mml:mi>\r\n                                                   <mml:mo>)</mml:mo>\r\n                                                </mml:mrow>\r\n                                                <mml:mo>−</mml:mo>\r\n                                                <mml:mi mathvariant=\"normal\">∇</mml:mi>\r\n                                                <mml:mo>⋅</mml:mo>\r\n                                                <mml:mrow>\r\n                                                   <mml:mo>(</mml:mo>\r\n                                                   <mml:mi>S</mml:mi>\r\n                                                   <mml:mrow>\r\n                                                      <mml:mo>(</mml:mo>\r\n                                                      <mml:mi>u</mml:mi>\r\n                                                      <mml:mo>)</mml:mo>\r\n                                                   </mml:mrow>\r\n                                                   <mml:mi mathvariant=\"normal\">∇</mml:mi>\r\n                                                   <mml:mi>v</mml:mi>\r\n                                                   <mml:mo>)</mml:mo>\r\n                                                </mml:mrow>\r\n                                                <mml:mo>,</mml:mo>\r\n                                             </mml:mtd>\r\n                                          </mml:mtr>\r\n                                          <mml:mtr>\r\n                                             <mml:mtd>\r\n                                                <mml:mn>0</mml:mn>\r\n                                                <mml:mo>=</mml:mo>\r\n                                                <mml:mi mathvariant=\"normal\">Δ</mml:mi>\r\n                                                <mml:mi>v</mml:mi>\r\n                                                <mml:mo>−</mml:mo>\r\n                                                <mml:mi>μ</mml:mi>\r\n                                                <mml:mo>+</mml:mo>\r\n                                                <mml:mi>u</mml:mi>\r\n                                                <mml:mo>,</mml:mo>\r\n                                                <mml:mstyle scriptlevel=\"0\"/>\r\n                                                <mml:mi>μ</mml:mi>\r\n                                                <mml:mo>=</mml:mo>\r\n                                                <mml:mstyle displaystyle=\"true\" scriptlevel=\"0\">\r\n                                                   <mml:mo>−</mml:mo>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:mstyle scriptlevel=\"0\"/>\r\n                                                   <mml:msub>\r\n                                                      <mml:mo>∫</mml:mo>\r\n                                                      <mml:mi mathvariant=\"normal\">Ω</mml:mi>\r\n                                                   </mml:msub>\r\n                                                   <mml:mi>u</mml:mi>\r\n                                                   <mml:mtext>d</mml:mtext>\r\n                                                   <mml:mi>x</mml:mi>\r\n                                                   <mml:mo>,</mml:mo>\r\n                                                </mml:mstyle>\r\n                                             </mml:mtd>\r\n                                          </mml:mtr>\r\n                                       </mml:mtable>\r\n                                    </mml:mrow>\r\n                                 </mml:mtd>\r\n                              </mml:mtr>\r\n                           </mml:mtable>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> is considered in <jats:italic>n</jats:italic>-dimensional balls Ω with <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mi>n</mml:mi>\r\n                           <mml:mtext>⩾</mml:mtext>\r\n                           <mml:mn>2</mml:mn>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula>, with suitably regular and radially symmetric, radially nonincreasing initial data <jats:italic>u</jats:italic>\r\n                  <jats:sub>0</jats:sub>. The functions <jats:italic>D</jats:italic> and <jats:italic>S</jats:italic> are only assumed to belong to <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:msup>\r\n                              <mml:mi>C</mml:mi>\r\n                              <mml:mn>2</mml:mn>\r\n                           </mml:msup>\r\n                           <mml:mo stretchy=\"false\">(</mml:mo>\r\n                           <mml:mo stretchy=\"false\">[</mml:mo>\r\n                           <mml:mn>0</mml:mn>\r\n                           <mml:mo>,</mml:mo>\r\n                           <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> and to satisfy <jats:italic>D</jats:italic> &gt; 0 and <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mi>S</mml:mi>\r\n                           <mml:mtext>⩾</mml:mtext>\r\n                           <mml:mn>0</mml:mn>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> on <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mo stretchy=\"false\">[</mml:mo>\r\n                           <mml:mn>0</mml:mn>\r\n                           <mml:mo>,</mml:mo>\r\n                           <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> as well as <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mi>S</mml:mi>\r\n                           <mml:mo stretchy=\"false\">(</mml:mo>\r\n                           <mml:mn>0</mml:mn>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                           <mml:mo>=</mml:mo>\r\n                           <mml:mn>0</mml:mn>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula>; in particular, diffusivities with arbitrarily fast decay are included.</jats:p>\r\n               <jats:p>In this general context, it is shown that it is merely the asymptotic behavior as <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mi>ξ</mml:mi>\r\n                           <mml:mo accent=\"false\" stretchy=\"false\">→</mml:mo>\r\n                           <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> of the expression <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:mtable columnalign=\"left\" displaystyle=\"true\">\r\n                              <mml:mtr>\r\n                                 <mml:mtd>\r\n                                    <mml:mi>I</mml:mi>\r\n                                    <mml:mrow>\r\n                                       <mml:mo>(</mml:mo>\r\n                                       <mml:mi>ξ</mml:mi>\r\n                                       <mml:mo>)</mml:mo>\r\n                                    </mml:mrow>\r\n                                    <mml:mo>:=</mml:mo>\r\n                                    <mml:mfrac>\r\n                                       <mml:mrow>\r\n                                          <mml:mi>S</mml:mi>\r\n                                          <mml:mrow>\r\n                                             <mml:mo>(</mml:mo>\r\n                                             <mml:mi>ξ</mml:mi>\r\n                                             <mml:mo>)</mml:mo>\r\n                                          </mml:mrow>\r\n                                       </mml:mrow>\r\n                                       <mml:mrow>\r\n                                          <mml:msup>\r\n                                             <mml:mi>ξ</mml:mi>\r\n                                             <mml:mfrac>\r\n                                                <mml:mn>2</mml:mn>\r\n                                                <mml:mi>n</mml:mi>\r\n                                             </mml:mfrac>\r\n                                          </mml:msup>\r\n                                          <mml:mi>D</mml:mi>\r\n                                          <mml:mrow>\r\n                                             <mml:mo>(</mml:mo>\r\n                                             <mml:mi>ξ</mml:mi>\r\n                                             <mml:mo>)</mml:mo>\r\n                                          </mml:mrow>\r\n                                       </mml:mrow>\r\n                                    </mml:mfrac>\r\n                                    <mml:mo>,</mml:mo>\r\n                                    <mml:mstyle scriptlevel=\"0\"/>\r\n                                    <mml:mi>ξ</mml:mi>\r\n                                    <mml:mo>&gt;</mml:mo>\r\n                                    <mml:mn>0</mml:mn>\r\n                                    <mml:mo>,</mml:mo>\r\n                                 </mml:mtd>\r\n                              </mml:mtr>\r\n                           </mml:mtable>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> which decides about the occurrence of blow-up: Namely, it is seen that\r\n<jats:list id=\"nonad871al1\" list-type=\"bullet\">\r\n                     <jats:list-item id=\"nonad871al1.1\">\r\n                        <jats:label>•</jats:label>\r\n                        <jats:p>if <jats:inline-formula>\r\n                              <jats:tex-math/>\r\n                              <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                                 <mml:mrow>\r\n                                    <mml:munder>\r\n                                       <mml:mo movablelimits=\"true\">lim</mml:mo>\r\n                                       <mml:mrow>\r\n                                          <mml:mi>ξ</mml:mi>\r\n                                          <mml:mo accent=\"false\" stretchy=\"false\">→</mml:mo>\r\n                                          <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                                       </mml:mrow>\r\n                                    </mml:munder>\r\n                                    <mml:mi>I</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">(</mml:mo>\r\n                                    <mml:mi>ξ</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">)</mml:mo>\r\n                                    <mml:mo>=</mml:mo>\r\n                                    <mml:mn>0</mml:mn>\r\n                                 </mml:mrow>\r\n                              </mml:math>\r\n                           </jats:inline-formula>, then any such solution is global and bounded, that</jats:p>\r\n                     </jats:list-item>\r\n                     <jats:list-item id=\"nonad871al1.2\">\r\n                        <jats:label>•</jats:label>\r\n                        <jats:p>if <jats:inline-formula>\r\n                              <jats:tex-math/>\r\n                              <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                                 <mml:mrow>\r\n                                    <mml:munder>\r\n                                       <mml:mo movablelimits=\"true\">lim sup</mml:mo>\r\n                                       <mml:mrow>\r\n                                          <mml:mi>ξ</mml:mi>\r\n                                          <mml:mo accent=\"false\" stretchy=\"false\">→</mml:mo>\r\n                                          <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                                       </mml:mrow>\r\n                                    </mml:munder>\r\n                                    <mml:mi>I</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">(</mml:mo>\r\n                                    <mml:mi>ξ</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">)</mml:mo>\r\n                                    <mml:mo>&lt;</mml:mo>\r\n                                    <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                                 </mml:mrow>\r\n                              </mml:math>\r\n                           </jats:inline-formula> and <jats:inline-formula>\r\n                              <jats:tex-math/>\r\n                              <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                                 <mml:mrow>\r\n                                    <mml:msub>\r\n                                       <mml:mo>∫</mml:mo>\r\n                                       <mml:mi mathvariant=\"normal\">Ω</mml:mi>\r\n                                    </mml:msub>\r\n                                    <mml:msub>\r\n                                       <mml:mi>u</mml:mi>\r\n                                       <mml:mn>0</mml:mn>\r\n                                    </mml:msub>\r\n                                 </mml:mrow>\r\n                              </mml:math>\r\n                           </jats:inline-formula> is suitably small, then the corresponding solution is global and bounded, and that</jats:p>\r\n                     </jats:list-item>\r\n                     <jats:list-item id=\"nonad871al1.3\">\r\n                        <jats:label>•</jats:label>\r\n                        <jats:p>if <jats:inline-formula>\r\n                              <jats:tex-math/>\r\n                              <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                                 <mml:mrow>\r\n                                    <mml:munder>\r\n                                       <mml:mo movablelimits=\"true\">lim inf</mml:mo>\r\n                                       <mml:mrow>\r\n                                          <mml:mi>ξ</mml:mi>\r\n                                          <mml:mo accent=\"false\" stretchy=\"false\">→</mml:mo>\r\n                                          <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                                       </mml:mrow>\r\n                                    </mml:munder>\r\n                                    <mml:mi>I</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">(</mml:mo>\r\n                                    <mml:mi>ξ</mml:mi>\r\n                                    <mml:mo stretchy=\"false\">)</mml:mo>\r\n                                    <mml:mo>&gt;</mml:mo>\r\n                                    <mml:mn>0</mml:mn>\r\n                                 </mml:mrow>\r\n                              </mml:math>\r\n                           </jats:inline-formula>, then at each appropriately large mass level <jats:italic>m</jats:italic>, there exist radial initial data <jats:italic>u</jats:italic>\r\n                           <jats:sub>0</jats:sub> such that <jats:inline-formula>\r\n                              <jats:tex-math/>\r\n                              <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                                 <mml:mrow>\r\n                                    <mml:msub>\r\n                                       <mml:mo>∫</mml:mo>\r\n                                       <mml:mi mathvariant=\"normal\">Ω</mml:mi>\r\n                                    </mml:msub>\r\n                                    <mml:msub>\r\n                                       <mml:mi>u</mml:mi>\r\n                                       <mml:mn>0</mml:mn>\r\n                                    </mml:msub>\r\n                                    <mml:mo>=</mml:mo>\r\n                                    <mml:mi>m</mml:mi>\r\n                                 </mml:mrow>\r\n                              </mml:math>\r\n                           </jats:inline-formula>, and that the associated solution blows up either in finite or in infinite time.</jats:p>\r\n                     </jats:list-item>\r\n                  </jats:list>\r\n               </jats:p>\r\n               <jats:p>This especially reveals the presence of critical mass phenomena whenever <jats:inline-formula>\r\n                     <jats:tex-math/>\r\n                     <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\">\r\n                        <mml:mrow>\r\n                           <mml:munder>\r\n                              <mml:mo movablelimits=\"true\">lim</mml:mo>\r\n                              <mml:mrow>\r\n                                 <mml:mi>ξ</mml:mi>\r\n                                 <mml:mo accent=\"false\" stretchy=\"false\">→</mml:mo>\r\n                                 <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                              </mml:mrow>\r\n                           </mml:munder>\r\n                           <mml:mi>I</mml:mi>\r\n                           <mml:mo stretchy=\"false\">(</mml:mo>\r\n                           <mml:mi>ξ</mml:mi>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                           <mml:mo>∈</mml:mo>\r\n                           <mml:mo stretchy=\"false\">(</mml:mo>\r\n                           <mml:mn>0</mml:mn>\r\n                           <mml:mo>,</mml:mo>\r\n                           <mml:mi mathvariant=\"normal\">∞</mml:mi>\r\n                           <mml:mo stretchy=\"false\">)</mml:mo>\r\n                        </mml:mrow>\r\n                     </mml:math>\r\n                  </jats:inline-formula> exists.</jats:p>","lang":"eng"}],"status":"public","_id":"63253","user_id":"31496","article_number":"125006","language":[{"iso":"eng"}],"publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"issue":"12","year":"2024","citation":{"chicago":"Ding, Mengyao, and Michael Winkler. “Radial Blow-up in Quasilinear Keller-Segel Systems: Approaching the Full Picture.” <i>Nonlinearity</i> 37, no. 12 (2024). <a href=\"https://doi.org/10.1088/1361-6544/ad871a\">https://doi.org/10.1088/1361-6544/ad871a</a>.","ieee":"M. Ding and M. Winkler, “Radial blow-up in quasilinear Keller-Segel systems: approaching the full picture,” <i>Nonlinearity</i>, vol. 37, no. 12, Art. no. 125006, 2024, doi: <a href=\"https://doi.org/10.1088/1361-6544/ad871a\">10.1088/1361-6544/ad871a</a>.","ama":"Ding M, Winkler M. Radial blow-up in quasilinear Keller-Segel systems: approaching the full picture. <i>Nonlinearity</i>. 2024;37(12). doi:<a href=\"https://doi.org/10.1088/1361-6544/ad871a\">10.1088/1361-6544/ad871a</a>","short":"M. Ding, M. Winkler, Nonlinearity 37 (2024).","bibtex":"@article{Ding_Winkler_2024, title={Radial blow-up in quasilinear Keller-Segel systems: approaching the full picture}, volume={37}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/ad871a\">10.1088/1361-6544/ad871a</a>}, number={12125006}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Ding, Mengyao and Winkler, Michael}, year={2024} }","mla":"Ding, Mengyao, and Michael Winkler. “Radial Blow-up in Quasilinear Keller-Segel Systems: Approaching the Full Picture.” <i>Nonlinearity</i>, vol. 37, no. 12, 125006, IOP Publishing, 2024, doi:<a href=\"https://doi.org/10.1088/1361-6544/ad871a\">10.1088/1361-6544/ad871a</a>.","apa":"Ding, M., &#38; Winkler, M. (2024). Radial blow-up in quasilinear Keller-Segel systems: approaching the full picture. <i>Nonlinearity</i>, <i>37</i>(12), Article 125006. <a href=\"https://doi.org/10.1088/1361-6544/ad871a\">https://doi.org/10.1088/1361-6544/ad871a</a>"},"intvolume":"        37","date_updated":"2025-12-18T20:13:49Z","publisher":"IOP Publishing","date_created":"2025-12-18T19:04:45Z","author":[{"last_name":"Ding","full_name":"Ding, Mengyao","first_name":"Mengyao"},{"last_name":"Winkler","id":"31496","full_name":"Winkler, Michael","first_name":"Michael"}],"volume":37,"title":"Radial blow-up in quasilinear Keller-Segel systems: approaching the full picture","doi":"10.1088/1361-6544/ad871a"},{"status":"public","abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title><jats:p>A no-flux initial-boundary value problem for<jats:disp-formula id=\"nonace22eueqn1\"><jats:tex-math><?CDATA \\begin{align*} \\begin{cases} u_t = \\Delta \\big(u\\phi(v)\\big), \\\\[1mm] v_t = \\Delta v-uv, \\end{cases} \\qquad \\qquad (\\star) \\end{align*}?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"block\" overflow=\"scroll\"><mml:mtable columnalign=\"right left right left right left right left right left right left\" columnspacing=\"0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em\" rowspacing=\"3pt\"><mml:mtr><mml:mtd><mml:mfenced close=\"\" open=\"{\"><mml:mtable columnalign=\"left left\" columnspacing=\"1em\" rowspacing=\".1em\"><mml:mtr><mml:mtd><mml:msub><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant=\"normal\">Δ</mml:mi><mml:mrow><mml:mo maxsize=\"1.2em\" minsize=\"1.2em\">(</mml:mo></mml:mrow><mml:mi>u</mml:mi><mml:mi>ϕ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>v</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mo maxsize=\"1.2em\" minsize=\"1.2em\">)</mml:mo></mml:mrow><mml:mo>,</mml:mo></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>v</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant=\"normal\">Δ</mml:mi><mml:mi>v</mml:mi><mml:mo>−</mml:mo><mml:mi>u</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋆</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" orientation=\"portrait\" position=\"float\" xlink:href=\"nonace22eueqn1.gif\" xlink:type=\"simple\" /></jats:disp-formula>is considered in smoothly bounded subdomains of<jats:inline-formula><jats:tex-math><?CDATA $\\mathbb{R}^n$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msup><mml:mrow><mml:mi mathvariant=\"double-struck\">R</mml:mi></mml:mrow><mml:mi>n</mml:mi></mml:msup></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn1.gif\" xlink:type=\"simple\" /></jats:inline-formula>with<jats:inline-formula><jats:tex-math><?CDATA $n\\geqslant 1$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn2.gif\" xlink:type=\"simple\" /></jats:inline-formula>and suitably regular initial data, where<jats:italic>φ</jats:italic>is assumed to reflect algebraic type cross-degeneracies by sharing essential features with<jats:inline-formula><jats:tex-math><?CDATA $0\\leqslant \\xi\\mapsto \\xi^\\alpha$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mn>0</mml:mn><mml:mo>⩽</mml:mo><mml:mi>ξ</mml:mi><mml:mo stretchy=\"false\">↦</mml:mo><mml:msup><mml:mi>ξ</mml:mi><mml:mi>α</mml:mi></mml:msup></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn3.gif\" xlink:type=\"simple\" /></jats:inline-formula>for some<jats:inline-formula><jats:tex-math><?CDATA $\\alpha\\geqslant 1$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn4.gif\" xlink:type=\"simple\" /></jats:inline-formula>. Based on the discovery of a gradient structure acting at regularity levels mild enough to be consistent with degeneracy-driven limitations of smoothness information, in this general setting it is shown that with some measurable limit profile<jats:inline-formula><jats:tex-math><?CDATA $u_\\infty$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msub><mml:mi>u</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msub></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn5.gif\" xlink:type=\"simple\" /></jats:inline-formula>and some null set<jats:inline-formula><jats:tex-math><?CDATA $N_\\star\\subset (0,\\infty)$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msub><mml:mi>N</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>⊂</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn6.gif\" xlink:type=\"simple\" /></jats:inline-formula>, a corresponding global generalized solution, known to exist according to recent literature, satisfies<jats:disp-formula id=\"nonace22eueqn2\"><jats:tex-math><?CDATA \\begin{align*} \\rho(u(\\cdot,t))\\stackrel{\\star}{\\rightharpoonup} \\rho(u_\\infty) \\quad \\textrm{in } L^\\infty(\\Omega) \\quad\\;\\; \\textrm{ and } \\quad\\;\\; v(\\cdot,t)\\to 0 \\quad \\textrm{in } L^p(\\Omega)\\; \\textrm{for all } p\\geqslant 1 \\end{align*}?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"block\" overflow=\"scroll\"><mml:mtable columnalign=\"right left right left right left right left right left right left\" columnspacing=\"0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em\" rowspacing=\"3pt\"><mml:mtr><mml:mtd><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>u</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mover><mml:mrow><mml:mo stretchy=\"false\">⇀</mml:mo></mml:mrow><mml:mrow><mml:mo>⋆</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext>in </mml:mtext></mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext> and </mml:mtext></mml:mrow><mml:mi>v</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">→</mml:mo><mml:mn>0</mml:mn><mml:mrow><mml:mtext>in </mml:mtext></mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mi>p</mml:mi></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext>for all </mml:mtext></mml:mrow><mml:mi>p</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" orientation=\"portrait\" position=\"float\" xlink:href=\"nonace22eueqn2.gif\" xlink:type=\"simple\" /></jats:disp-formula>as<jats:inline-formula><jats:tex-math><?CDATA $(0,\\infty)\\setminus N_\\star \\ni t\\to \\infty$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>∖</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>∋</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn7.gif\" xlink:type=\"simple\" /></jats:inline-formula>, where<jats:inline-formula><jats:tex-math><?CDATA $\\rho(\\xi): = \\frac{\\xi^2}{(\\xi+1)^2}$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>ξ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>:=</mml:mo><mml:mfrac><mml:msup><mml:mi>ξ</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>ξ</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mrow><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mrow></mml:mfrac></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn8.gif\" xlink:type=\"simple\" /></jats:inline-formula>,<jats:inline-formula><jats:tex-math><?CDATA $\\xi\\geqslant 0$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>ξ</mml:mi><mml:mo>⩾</mml:mo><mml:mn>0</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn9.gif\" xlink:type=\"simple\" /></jats:inline-formula>. In the particular case when either<jats:inline-formula><jats:tex-math><?CDATA $n\\leqslant 2$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩽</mml:mo><mml:mn>2</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn10.gif\" xlink:type=\"simple\" /></jats:inline-formula>and<jats:inline-formula><jats:tex-math><?CDATA $\\alpha\\geqslant 1$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn11.gif\" xlink:type=\"simple\" /></jats:inline-formula>is arbitrary, or<jats:inline-formula><jats:tex-math><?CDATA $n\\geqslant 1$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn12.gif\" xlink:type=\"simple\" /></jats:inline-formula>and<jats:inline-formula><jats:tex-math><?CDATA $\\alpha\\in [1,2]$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>∈</mml:mo><mml:mo stretchy=\"false\">[</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">]</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn13.gif\" xlink:type=\"simple\" /></jats:inline-formula>, additional quantitative information on the deviation of trajectories from the initial data is derived. This is found to imply a lower estimate for the spatial oscillation of the respective first components throughout evolution, and moreover this is seen to entail that each of the uncountably many steady states<jats:inline-formula><jats:tex-math><?CDATA $(u_\\star,0)$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>,</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn14.gif\" xlink:type=\"simple\" /></jats:inline-formula>of (<jats:inline-formula><jats:tex-math><?CDATA $\\star$?></jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo>⋆</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn15.gif\" xlink:type=\"simple\" /></jats:inline-formula>) is stable with respect to a suitably chosen norm topology.</jats:p>"}],"publication":"Nonlinearity","type":"journal_article","language":[{"iso":"eng"}],"keyword":["Applied Mathematics","General Physics and Astronomy","Mathematical Physics","Statistical and Nonlinear Physics"],"user_id":"31496","_id":"53345","page":"4438-4469","intvolume":"        36","citation":{"mla":"Winkler, Michael. “Stabilization despite Pervasive Strong Cross-Degeneracies in a Nonlinear Diffusion Model for Migration–Consumption Interaction.” <i>Nonlinearity</i>, vol. 36, no. 8, IOP Publishing, 2023, pp. 4438–69, doi:<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>.","bibtex":"@article{Winkler_2023, title={Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction}, volume={36}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>}, number={8}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Winkler, Michael}, year={2023}, pages={4438–4469} }","short":"M. Winkler, Nonlinearity 36 (2023) 4438–4469.","apa":"Winkler, M. (2023). Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction. <i>Nonlinearity</i>, <i>36</i>(8), 4438–4469. <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">https://doi.org/10.1088/1361-6544/ace22e</a>","ama":"Winkler M. Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction. <i>Nonlinearity</i>. 2023;36(8):4438-4469. doi:<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>","ieee":"M. Winkler, “Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction,” <i>Nonlinearity</i>, vol. 36, no. 8, pp. 4438–4469, 2023, doi: <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>.","chicago":"Winkler, Michael. “Stabilization despite Pervasive Strong Cross-Degeneracies in a Nonlinear Diffusion Model for Migration–Consumption Interaction.” <i>Nonlinearity</i> 36, no. 8 (2023): 4438–69. <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">https://doi.org/10.1088/1361-6544/ace22e</a>."},"year":"2023","issue":"8","publication_identifier":{"issn":["0951-7715","1361-6544"]},"publication_status":"published","doi":"10.1088/1361-6544/ace22e","title":"Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction","volume":36,"date_created":"2024-04-07T12:56:35Z","author":[{"full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"date_updated":"2024-04-07T12:56:40Z","publisher":"IOP Publishing"},{"title":"Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction","doi":"10.1088/1361-6544/ace22e","date_updated":"2025-12-18T20:12:06Z","publisher":"IOP Publishing","volume":36,"date_created":"2025-12-18T19:17:01Z","author":[{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"year":"2023","intvolume":"        36","page":"4438-4469","citation":{"ieee":"M. Winkler, “Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction,” <i>Nonlinearity</i>, vol. 36, no. 8, pp. 4438–4469, 2023, doi: <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>.","chicago":"Winkler, Michael. “Stabilization despite Pervasive Strong Cross-Degeneracies in a Nonlinear Diffusion Model for Migration–Consumption Interaction.” <i>Nonlinearity</i> 36, no. 8 (2023): 4438–69. <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">https://doi.org/10.1088/1361-6544/ace22e</a>.","ama":"Winkler M. Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction. <i>Nonlinearity</i>. 2023;36(8):4438-4469. doi:<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>","bibtex":"@article{Winkler_2023, title={Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction}, volume={36}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>}, number={8}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Winkler, Michael}, year={2023}, pages={4438–4469} }","mla":"Winkler, Michael. “Stabilization despite Pervasive Strong Cross-Degeneracies in a Nonlinear Diffusion Model for Migration–Consumption Interaction.” <i>Nonlinearity</i>, vol. 36, no. 8, IOP Publishing, 2023, pp. 4438–69, doi:<a href=\"https://doi.org/10.1088/1361-6544/ace22e\">10.1088/1361-6544/ace22e</a>.","short":"M. Winkler, Nonlinearity 36 (2023) 4438–4469.","apa":"Winkler, M. (2023). Stabilization despite pervasive strong cross-degeneracies in a nonlinear diffusion model for migration–consumption interaction. <i>Nonlinearity</i>, <i>36</i>(8), 4438–4469. <a href=\"https://doi.org/10.1088/1361-6544/ace22e\">https://doi.org/10.1088/1361-6544/ace22e</a>"},"publication_identifier":{"issn":["0951-7715","1361-6544"]},"publication_status":"published","issue":"8","language":[{"iso":"eng"}],"_id":"63281","user_id":"31496","abstract":[{"text":"<jats:title>Abstract</jats:title><jats:p>A no-flux initial-boundary value problem for<jats:disp-formula id=\"nonace22eueqn1\"><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"block\" overflow=\"scroll\"><mml:mtable columnalign=\"right left right left right left right left right left right left\" columnspacing=\"0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em\" rowspacing=\"3pt\"><mml:mtr><mml:mtd><mml:mfenced close=\"\" open=\"{\"><mml:mtable columnalign=\"left left\" columnspacing=\"1em\" rowspacing=\".1em\"><mml:mtr><mml:mtd><mml:msub><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant=\"normal\">Δ</mml:mi><mml:mrow><mml:mo maxsize=\"1.2em\" minsize=\"1.2em\">(</mml:mo></mml:mrow><mml:mi>u</mml:mi><mml:mi>ϕ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>v</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mo maxsize=\"1.2em\" minsize=\"1.2em\">)</mml:mo></mml:mrow><mml:mo>,</mml:mo></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>v</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant=\"normal\">Δ</mml:mi><mml:mi>v</mml:mi><mml:mo>−</mml:mo><mml:mi>u</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋆</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" orientation=\"portrait\" position=\"float\" xlink:href=\"nonace22eueqn1.gif\" xlink:type=\"simple\"/></jats:disp-formula>is considered in smoothly bounded subdomains of<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msup><mml:mrow><mml:mi mathvariant=\"double-struck\">R</mml:mi></mml:mrow><mml:mi>n</mml:mi></mml:msup></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn1.gif\" xlink:type=\"simple\"/></jats:inline-formula>with<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn2.gif\" xlink:type=\"simple\"/></jats:inline-formula>and suitably regular initial data, where<jats:italic>φ</jats:italic>is assumed to reflect algebraic type cross-degeneracies by sharing essential features with<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mn>0</mml:mn><mml:mo>⩽</mml:mo><mml:mi>ξ</mml:mi><mml:mo stretchy=\"false\">↦</mml:mo><mml:msup><mml:mi>ξ</mml:mi><mml:mi>α</mml:mi></mml:msup></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn3.gif\" xlink:type=\"simple\"/></jats:inline-formula>for some<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn4.gif\" xlink:type=\"simple\"/></jats:inline-formula>. Based on the discovery of a gradient structure acting at regularity levels mild enough to be consistent with degeneracy-driven limitations of smoothness information, in this general setting it is shown that with some measurable limit profile<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msub><mml:mi>u</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msub></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn5.gif\" xlink:type=\"simple\"/></jats:inline-formula>and some null set<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:msub><mml:mi>N</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>⊂</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn6.gif\" xlink:type=\"simple\"/></jats:inline-formula>, a corresponding global generalized solution, known to exist according to recent literature, satisfies<jats:disp-formula id=\"nonace22eueqn2\"><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"block\" overflow=\"scroll\"><mml:mtable columnalign=\"right left right left right left right left right left right left\" columnspacing=\"0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em 2em 0.2777777777777778em\" rowspacing=\"3pt\"><mml:mtr><mml:mtd><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>u</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mover><mml:mrow><mml:mo stretchy=\"false\">⇀</mml:mo></mml:mrow><mml:mrow><mml:mo>⋆</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext>in </mml:mtext></mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext> and </mml:mtext></mml:mrow><mml:mi>v</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">→</mml:mo><mml:mn>0</mml:mn><mml:mrow><mml:mtext>in </mml:mtext></mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mi>p</mml:mi></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mrow><mml:mtext>for all </mml:mtext></mml:mrow><mml:mi>p</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" orientation=\"portrait\" position=\"float\" xlink:href=\"nonace22eueqn2.gif\" xlink:type=\"simple\"/></jats:disp-formula>as<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>∖</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>∋</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi mathvariant=\"normal\">∞</mml:mi></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn7.gif\" xlink:type=\"simple\"/></jats:inline-formula>, where<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>ρ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>ξ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>:=</mml:mo><mml:mfrac><mml:msup><mml:mi>ξ</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>ξ</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mrow><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mrow></mml:mfrac></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn8.gif\" xlink:type=\"simple\"/></jats:inline-formula>,<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>ξ</mml:mi><mml:mo>⩾</mml:mo><mml:mn>0</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn9.gif\" xlink:type=\"simple\"/></jats:inline-formula>. In the particular case when either<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩽</mml:mo><mml:mn>2</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn10.gif\" xlink:type=\"simple\"/></jats:inline-formula>and<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn11.gif\" xlink:type=\"simple\"/></jats:inline-formula>is arbitrary, or<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>n</mml:mi><mml:mo>⩾</mml:mo><mml:mn>1</mml:mn></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn12.gif\" xlink:type=\"simple\"/></jats:inline-formula>and<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mi>α</mml:mi><mml:mo>∈</mml:mo><mml:mo stretchy=\"false\">[</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">]</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn13.gif\" xlink:type=\"simple\"/></jats:inline-formula>, additional quantitative information on the deviation of trajectories from the initial data is derived. This is found to imply a lower estimate for the spatial oscillation of the respective first components throughout evolution, and moreover this is seen to entail that each of the uncountably many steady states<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mo>⋆</mml:mo></mml:msub><mml:mo>,</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn14.gif\" xlink:type=\"simple\"/></jats:inline-formula>of (<jats:inline-formula><jats:tex-math/><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"><mml:mo>⋆</mml:mo></mml:math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"nonace22eieqn15.gif\" xlink:type=\"simple\"/></jats:inline-formula>) is stable with respect to a suitably chosen norm topology.</jats:p>","lang":"eng"}],"status":"public","publication":"Nonlinearity","type":"journal_article"},{"date_updated":"2022-09-07T08:36:46Z","author":[{"id":"97359","full_name":"von der Gracht, Sören","orcid":"0000-0002-8054-2058","last_name":"von der Gracht","first_name":"Sören"},{"full_name":"Nijholt, Eddie","last_name":"Nijholt","first_name":"Eddie"},{"first_name":"Bob","last_name":"Rink","full_name":"Rink, Bob"}],"volume":35,"doi":"10.1088/1361-6544/ac5463","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"citation":{"apa":"von der Gracht, S., Nijholt, E., &#38; Rink, B. (2022). Amplified steady state bifurcations in feedforward networks. <i>Nonlinearity</i>, <i>35</i>(4), 2073–2120. <a href=\"https://doi.org/10.1088/1361-6544/ac5463\">https://doi.org/10.1088/1361-6544/ac5463</a>","bibtex":"@article{von der Gracht_Nijholt_Rink_2022, title={Amplified steady state bifurcations in feedforward networks}, volume={35}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/ac5463\">10.1088/1361-6544/ac5463</a>}, number={4}, journal={Nonlinearity}, publisher={IOP Publishing}, author={von der Gracht, Sören and Nijholt, Eddie and Rink, Bob}, year={2022}, pages={2073–2120} }","short":"S. von der Gracht, E. Nijholt, B. Rink, Nonlinearity 35 (2022) 2073–2120.","mla":"von der Gracht, Sören, et al. “Amplified Steady State Bifurcations in Feedforward Networks.” <i>Nonlinearity</i>, vol. 35, no. 4, IOP Publishing, 2022, pp. 2073–120, doi:<a href=\"https://doi.org/10.1088/1361-6544/ac5463\">10.1088/1361-6544/ac5463</a>.","chicago":"Gracht, Sören von der, Eddie Nijholt, and Bob Rink. “Amplified Steady State Bifurcations in Feedforward Networks.” <i>Nonlinearity</i> 35, no. 4 (2022): 2073–2120. <a href=\"https://doi.org/10.1088/1361-6544/ac5463\">https://doi.org/10.1088/1361-6544/ac5463</a>.","ieee":"S. von der Gracht, E. Nijholt, and B. Rink, “Amplified steady state bifurcations in feedforward networks,” <i>Nonlinearity</i>, vol. 35, no. 4, pp. 2073–2120, 2022, doi: <a href=\"https://doi.org/10.1088/1361-6544/ac5463\">10.1088/1361-6544/ac5463</a>.","ama":"von der Gracht S, Nijholt E, Rink B. Amplified steady state bifurcations in feedforward networks. <i>Nonlinearity</i>. 2022;35(4):2073-2120. doi:<a href=\"https://doi.org/10.1088/1361-6544/ac5463\">10.1088/1361-6544/ac5463</a>"},"intvolume":"        35","page":"2073-2120","_id":"33264","user_id":"97359","extern":"1","type":"journal_article","status":"public","publisher":"IOP Publishing","date_created":"2022-09-06T11:38:15Z","title":"Amplified steady state bifurcations in feedforward networks","issue":"4","year":"2022","external_id":{"arxiv":["2105.02547"]},"keyword":["Applied Mathematics","General Physics and Astronomy","Mathematical Physics","Statistical and Nonlinear Physics"],"language":[{"iso":"eng"}],"publication":"Nonlinearity","abstract":[{"text":"We investigate bifurcations in feedforward coupled cell networks. Feedforward structure (the absence of feedback) can be defined by a partial order on the cells. We use this property to study generic one-parameter steady state bifurcations for such networks. Branching solutions and their asymptotics are described in terms of Taylor coefficients of the internal dynamics. They can be determined via an algorithm that only exploits the network structure. Similar to previous results on feedforward chains, we observe amplifications of the growth rates of steady state branches induced by the feedforward structure. However, contrary to these earlier results, as the interaction scenarios can be more complicated in general feedforward networks, different branching patterns and different amplifications can occur for different regions in the space of Taylor coefficients.","lang":"eng"}]},{"status":"public","type":"journal_article","article_type":"original","extern":"1","_id":"19939","user_id":"85279","department":[{"_id":"636"}],"citation":{"mla":"Kreusser, Lisa Maria, et al. “Detection of High Codimensional Bifurcations in Variational PDEs.” <i>Nonlinearity</i>, vol. 33, no. 5, 2020, pp. 2335–63, doi:<a href=\"https://doi.org/10.1088/1361-6544/ab7293\">10.1088/1361-6544/ab7293</a>.","bibtex":"@article{Kreusser_McLachlan_Offen_2020, title={Detection of high codimensional bifurcations in variational PDEs}, volume={33}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/ab7293\">10.1088/1361-6544/ab7293</a>}, number={5}, journal={Nonlinearity}, author={Kreusser, Lisa Maria and McLachlan, Robert I and Offen, Christian}, year={2020}, pages={2335–2363} }","short":"L.M. Kreusser, R.I. McLachlan, C. Offen, Nonlinearity 33 (2020) 2335–2363.","apa":"Kreusser, L. M., McLachlan, R. I., &#38; Offen, C. (2020). Detection of high codimensional bifurcations in variational PDEs. <i>Nonlinearity</i>, <i>33</i>(5), 2335–2363. <a href=\"https://doi.org/10.1088/1361-6544/ab7293\">https://doi.org/10.1088/1361-6544/ab7293</a>","ama":"Kreusser LM, McLachlan RI, Offen C. Detection of high codimensional bifurcations in variational PDEs. <i>Nonlinearity</i>. 2020;33(5):2335-2363. doi:<a href=\"https://doi.org/10.1088/1361-6544/ab7293\">10.1088/1361-6544/ab7293</a>","chicago":"Kreusser, Lisa Maria, Robert I McLachlan, and Christian Offen. “Detection of High Codimensional Bifurcations in Variational PDEs.” <i>Nonlinearity</i> 33, no. 5 (2020): 2335–63. <a href=\"https://doi.org/10.1088/1361-6544/ab7293\">https://doi.org/10.1088/1361-6544/ab7293</a>.","ieee":"L. M. Kreusser, R. I. McLachlan, and C. Offen, “Detection of high codimensional bifurcations in variational PDEs,” <i>Nonlinearity</i>, vol. 33, no. 5, pp. 2335–2363, 2020."},"page":"2335-2363","intvolume":"        33","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"main_file_link":[{"open_access":"1","url":"https://doi.org/10.1088/1361-6544/ab7293"}],"doi":"10.1088/1361-6544/ab7293","oa":"1","date_updated":"2022-01-06T06:54:14Z","author":[{"first_name":"Lisa Maria","full_name":"Kreusser, Lisa Maria","last_name":"Kreusser"},{"first_name":"Robert I","last_name":"McLachlan","full_name":"McLachlan, Robert I"},{"full_name":"Offen, Christian","id":"85279","orcid":"https://orcid.org/0000-0002-5940-8057","last_name":"Offen","first_name":"Christian"}],"volume":33,"publication":"Nonlinearity","language":[{"iso":"eng"}],"year":"2020","issue":"5","title":"Detection of high codimensional bifurcations in variational PDEs","date_created":"2020-10-06T16:32:04Z"},{"citation":{"bibtex":"@article{McLachlan_Offen_2018, title={Bifurcation of solutions to Hamiltonian boundary value problems}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/aab630\">10.1088/1361-6544/aab630</a>}, journal={Nonlinearity}, author={McLachlan, Robert I and Offen, Christian}, year={2018}, pages={2895–2927} }","short":"R.I. McLachlan, C. Offen, Nonlinearity (2018) 2895–2927.","mla":"McLachlan, Robert I., and Christian Offen. “Bifurcation of Solutions to Hamiltonian Boundary Value Problems.” <i>Nonlinearity</i>, 2018, pp. 2895–927, doi:<a href=\"https://doi.org/10.1088/1361-6544/aab630\">10.1088/1361-6544/aab630</a>.","apa":"McLachlan, R. I., &#38; Offen, C. (2018). Bifurcation of solutions to Hamiltonian boundary value problems. <i>Nonlinearity</i>, 2895–2927. <a href=\"https://doi.org/10.1088/1361-6544/aab630\">https://doi.org/10.1088/1361-6544/aab630</a>","ieee":"R. I. McLachlan and C. Offen, “Bifurcation of solutions to Hamiltonian boundary value problems,” <i>Nonlinearity</i>, pp. 2895–2927, 2018.","chicago":"McLachlan, Robert I, and Christian Offen. “Bifurcation of Solutions to Hamiltonian Boundary Value Problems.” <i>Nonlinearity</i>, 2018, 2895–2927. <a href=\"https://doi.org/10.1088/1361-6544/aab630\">https://doi.org/10.1088/1361-6544/aab630</a>.","ama":"McLachlan RI, Offen C. Bifurcation of solutions to Hamiltonian boundary value problems. <i>Nonlinearity</i>. 2018:2895-2927. doi:<a href=\"https://doi.org/10.1088/1361-6544/aab630\">10.1088/1361-6544/aab630</a>"},"page":"2895-2927","year":"2018","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"main_file_link":[{"url":"https://doi.org/10.1088/1361-6544/aab630"}],"doi":"10.1088/1361-6544/aab630","title":"Bifurcation of solutions to Hamiltonian boundary value problems","author":[{"first_name":"Robert I","full_name":"McLachlan, Robert I","last_name":"McLachlan"},{"orcid":"https://orcid.org/0000-0002-5940-8057","last_name":"Offen","id":"85279","full_name":"Offen, Christian","first_name":"Christian"}],"date_created":"2020-10-06T16:28:36Z","date_updated":"2022-01-06T06:54:14Z","status":"public","abstract":[{"lang":"eng","text":"A bifurcation is a qualitative change in a family of solutions to an equation produced by varying parameters. In contrast to the local bifurcations of dynamical systems that are often related to a change in the number or stability of equilibria, bifurcations of boundary value problems are global in nature and may not be related to any obvious change in dynamical behaviour. Catastrophe theory is a well-developed framework which studies the bifurcations of critical points of functions. In this paper we study the bifurcations of solutions of boundary-value problems for symplectic maps, using the language of (finite-dimensional) singularity theory. We associate certain such problems with a geometric picture involving the intersection of Lagrangian submanifolds, and hence with the critical points of a suitable generating function. Within this framework, we then study the effect of three special cases: (i) some common boundary conditions, such as Dirichlet boundary conditions for second-order systems, restrict the possible types of bifurcations (for example, in generic planar systems only the A-series beginning with folds and cusps can occur); (ii) integrable systems, such as planar Hamiltonian systems, can exhibit a novel periodic pitchfork bifurcation; and (iii) systems with Hamiltonian symmetries or reversing symmetries can exhibit restricted bifurcations associated with the symmetry. This approach offers an alternative to the analysis of critical points in function spaces, typically used in the study of bifurcation of variational problems, and opens the way to the detection of more exotic bifurcations than the simple folds and cusps that are often found in examples. "}],"type":"journal_article","publication":"Nonlinearity","extern":"1","language":[{"iso":"eng"}],"article_type":"original","user_id":"85279","department":[{"_id":"636"}],"_id":"19935"},{"title":"Tensor-based dynamic mode decomposition","doi":"10.1088/1361-6544/aabc8f","date_updated":"2022-01-06T07:04:00Z","volume":31,"date_created":"2019-03-29T13:32:04Z","author":[{"first_name":"Stefan","last_name":"Klus","full_name":"Klus, Stefan"},{"first_name":"Patrick","full_name":"Gelß, Patrick","last_name":"Gelß"},{"first_name":"Sebastian","id":"47427","full_name":"Peitz, Sebastian","last_name":"Peitz","orcid":"https://orcid.org/0000-0002-3389-793X"},{"first_name":"Christof","last_name":"Schütte","full_name":"Schütte, Christof"}],"year":"2018","page":"3359-3380","intvolume":"        31","citation":{"chicago":"Klus, Stefan, Patrick Gelß, Sebastian Peitz, and Christof Schütte. “Tensor-Based Dynamic Mode Decomposition.” <i>Nonlinearity</i> 31, no. 7 (2018): 3359–80. <a href=\"https://doi.org/10.1088/1361-6544/aabc8f\">https://doi.org/10.1088/1361-6544/aabc8f</a>.","ieee":"S. Klus, P. Gelß, S. Peitz, and C. Schütte, “Tensor-based dynamic mode decomposition,” <i>Nonlinearity</i>, vol. 31, no. 7, pp. 3359–3380, 2018.","ama":"Klus S, Gelß P, Peitz S, Schütte C. Tensor-based dynamic mode decomposition. <i>Nonlinearity</i>. 2018;31(7):3359-3380. doi:<a href=\"https://doi.org/10.1088/1361-6544/aabc8f\">10.1088/1361-6544/aabc8f</a>","apa":"Klus, S., Gelß, P., Peitz, S., &#38; Schütte, C. (2018). Tensor-based dynamic mode decomposition. <i>Nonlinearity</i>, <i>31</i>(7), 3359–3380. <a href=\"https://doi.org/10.1088/1361-6544/aabc8f\">https://doi.org/10.1088/1361-6544/aabc8f</a>","mla":"Klus, Stefan, et al. “Tensor-Based Dynamic Mode Decomposition.” <i>Nonlinearity</i>, vol. 31, no. 7, 2018, pp. 3359–80, doi:<a href=\"https://doi.org/10.1088/1361-6544/aabc8f\">10.1088/1361-6544/aabc8f</a>.","bibtex":"@article{Klus_Gelß_Peitz_Schütte_2018, title={Tensor-based dynamic mode decomposition}, volume={31}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/aabc8f\">10.1088/1361-6544/aabc8f</a>}, number={7}, journal={Nonlinearity}, author={Klus, Stefan and Gelß, Patrick and Peitz, Sebastian and Schütte, Christof}, year={2018}, pages={3359–3380} }","short":"S. Klus, P. Gelß, S. Peitz, C. Schütte, Nonlinearity 31 (2018) 3359–3380."},"publication_identifier":{"issn":["0951-7715","1361-6544"]},"publication_status":"published","issue":"7","article_type":"original","language":[{"iso":"eng"}],"_id":"8755","project":[{"name":"Computing Resources Provided by the Paderborn Center for Parallel Computing","_id":"52"}],"department":[{"_id":"101"}],"user_id":"47427","abstract":[{"lang":"eng","text":"Dynamic mode decomposition (DMD) is a recently developed tool for the analysis of the behavior of complex dynamical systems. In this paper, we will propose an extension of DMD that exploits low-rank tensor decompositions of potentially high-dimensional data sets to compute the corresponding DMD modes and eigenvalues. The goal is to reduce the computational complexity and also the amount of memory required to store the data in order to mitigate the curse of dimensionality. The efficiency of these tensor-based methods will be illustrated with the aid of several different fluid dynamics problems such as the von Kármán vortex street and the simulation of two merging vortices."}],"status":"public","publication":"Nonlinearity","type":"journal_article"},{"type":"journal_article","publication":"Nonlinearity","status":"public","user_id":"31496","_id":"63370","language":[{"iso":"eng"}],"issue":"4","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"citation":{"mla":"Espejo, Elio, and Michael Winkler. “Global Classical Solvability and Stabilization in a Two-Dimensional Chemotaxis-Navier–Stokes System Modeling Coral Fertilization.” <i>Nonlinearity</i>, vol. 31, no. 4, IOP Publishing, 2018, pp. 1227–59, doi:<a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">10.1088/1361-6544/aa9d5f</a>.","bibtex":"@article{Espejo_Winkler_2018, title={Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier–Stokes system modeling coral fertilization}, volume={31}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">10.1088/1361-6544/aa9d5f</a>}, number={4}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Espejo, Elio and Winkler, Michael}, year={2018}, pages={1227–1259} }","short":"E. Espejo, M. Winkler, Nonlinearity 31 (2018) 1227–1259.","apa":"Espejo, E., &#38; Winkler, M. (2018). Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier–Stokes system modeling coral fertilization. <i>Nonlinearity</i>, <i>31</i>(4), 1227–1259. <a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">https://doi.org/10.1088/1361-6544/aa9d5f</a>","ama":"Espejo E, Winkler M. Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier–Stokes system modeling coral fertilization. <i>Nonlinearity</i>. 2018;31(4):1227-1259. doi:<a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">10.1088/1361-6544/aa9d5f</a>","chicago":"Espejo, Elio, and Michael Winkler. “Global Classical Solvability and Stabilization in a Two-Dimensional Chemotaxis-Navier–Stokes System Modeling Coral Fertilization.” <i>Nonlinearity</i> 31, no. 4 (2018): 1227–59. <a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">https://doi.org/10.1088/1361-6544/aa9d5f</a>.","ieee":"E. Espejo and M. Winkler, “Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier–Stokes system modeling coral fertilization,” <i>Nonlinearity</i>, vol. 31, no. 4, pp. 1227–1259, 2018, doi: <a href=\"https://doi.org/10.1088/1361-6544/aa9d5f\">10.1088/1361-6544/aa9d5f</a>."},"page":"1227-1259","intvolume":"        31","year":"2018","author":[{"last_name":"Espejo","full_name":"Espejo, Elio","first_name":"Elio"},{"first_name":"Michael","last_name":"Winkler","id":"31496","full_name":"Winkler, Michael"}],"date_created":"2025-12-19T11:03:26Z","volume":31,"date_updated":"2025-12-19T11:03:32Z","publisher":"IOP Publishing","doi":"10.1088/1361-6544/aa9d5f","title":"Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier–Stokes system modeling coral fertilization"},{"publication":"Nonlinearity","type":"journal_article","status":"public","_id":"63376","user_id":"31496","language":[{"iso":"eng"}],"publication_identifier":{"issn":["0951-7715","1361-6544"]},"publication_status":"published","issue":"5","year":"2018","intvolume":"        31","page":"2031-2056","citation":{"ama":"Winkler M. A critical blow-up exponent in a chemotaxis system with nonlinear signal production. <i>Nonlinearity</i>. 2018;31(5):2031-2056. doi:<a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">10.1088/1361-6544/aaaa0e</a>","ieee":"M. Winkler, “A critical blow-up exponent in a chemotaxis system with nonlinear signal production,” <i>Nonlinearity</i>, vol. 31, no. 5, pp. 2031–2056, 2018, doi: <a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">10.1088/1361-6544/aaaa0e</a>.","chicago":"Winkler, Michael. “A Critical Blow-up Exponent in a Chemotaxis System with Nonlinear Signal Production.” <i>Nonlinearity</i> 31, no. 5 (2018): 2031–56. <a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">https://doi.org/10.1088/1361-6544/aaaa0e</a>.","mla":"Winkler, Michael. “A Critical Blow-up Exponent in a Chemotaxis System with Nonlinear Signal Production.” <i>Nonlinearity</i>, vol. 31, no. 5, IOP Publishing, 2018, pp. 2031–56, doi:<a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">10.1088/1361-6544/aaaa0e</a>.","bibtex":"@article{Winkler_2018, title={A critical blow-up exponent in a chemotaxis system with nonlinear signal production}, volume={31}, DOI={<a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">10.1088/1361-6544/aaaa0e</a>}, number={5}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Winkler, Michael}, year={2018}, pages={2031–2056} }","short":"M. Winkler, Nonlinearity 31 (2018) 2031–2056.","apa":"Winkler, M. (2018). A critical blow-up exponent in a chemotaxis system with nonlinear signal production. <i>Nonlinearity</i>, <i>31</i>(5), 2031–2056. <a href=\"https://doi.org/10.1088/1361-6544/aaaa0e\">https://doi.org/10.1088/1361-6544/aaaa0e</a>"},"date_updated":"2025-12-19T11:06:40Z","publisher":"IOP Publishing","volume":31,"date_created":"2025-12-19T11:06:33Z","author":[{"last_name":"Winkler","id":"31496","full_name":"Winkler, Michael","first_name":"Michael"}],"title":"A critical blow-up exponent in a chemotaxis system with nonlinear signal production","doi":"10.1088/1361-6544/aaaa0e"},{"keyword":["Applied Mathematics","General Physics and Astronomy","Mathematical Physics","Statistical and Nonlinear Physics"],"language":[{"iso":"eng"}],"_id":"34659","user_id":"23686","department":[{"_id":"34"},{"_id":"10"},{"_id":"90"}],"status":"public","type":"journal_article","publication":"Nonlinearity","title":"Blow-up of weak solutions to a chemotaxis system under influence of an external chemoattractant","doi":"10.1088/0951-7715/29/6/1865","publisher":"IOP Publishing","date_updated":"2022-12-21T10:05:45Z","author":[{"orcid":"0000-0001-9963-0800","last_name":"Black","full_name":"Black, Tobias","id":"23686","first_name":"Tobias"}],"date_created":"2022-12-21T09:46:00Z","volume":29,"year":"2016","citation":{"short":"T. Black, Nonlinearity 29 (2016) 1865–1886.","bibtex":"@article{Black_2016, title={Blow-up of weak solutions to a chemotaxis system under influence of an external chemoattractant}, volume={29}, DOI={<a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">10.1088/0951-7715/29/6/1865</a>}, number={6}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Black, Tobias}, year={2016}, pages={1865–1886} }","mla":"Black, Tobias. “Blow-up of Weak Solutions to a Chemotaxis System under Influence of an External Chemoattractant.” <i>Nonlinearity</i>, vol. 29, no. 6, IOP Publishing, 2016, pp. 1865–86, doi:<a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">10.1088/0951-7715/29/6/1865</a>.","apa":"Black, T. (2016). Blow-up of weak solutions to a chemotaxis system under influence of an external chemoattractant. <i>Nonlinearity</i>, <i>29</i>(6), 1865–1886. <a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">https://doi.org/10.1088/0951-7715/29/6/1865</a>","ama":"Black T. Blow-up of weak solutions to a chemotaxis system under influence of an external chemoattractant. <i>Nonlinearity</i>. 2016;29(6):1865-1886. doi:<a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">10.1088/0951-7715/29/6/1865</a>","chicago":"Black, Tobias. “Blow-up of Weak Solutions to a Chemotaxis System under Influence of an External Chemoattractant.” <i>Nonlinearity</i> 29, no. 6 (2016): 1865–86. <a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">https://doi.org/10.1088/0951-7715/29/6/1865</a>.","ieee":"T. Black, “Blow-up of weak solutions to a chemotaxis system under influence of an external chemoattractant,” <i>Nonlinearity</i>, vol. 29, no. 6, pp. 1865–1886, 2016, doi: <a href=\"https://doi.org/10.1088/0951-7715/29/6/1865\">10.1088/0951-7715/29/6/1865</a>."},"intvolume":"        29","page":"1865-1886","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"issue":"6"},{"type":"journal_article","publication":"Nonlinearity","status":"public","_id":"26511","user_id":"48188","language":[{"iso":"eng"}],"publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]},"year":"2014","citation":{"ama":"Barkhofen S, Faure F, Weich T. Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum. <i>Nonlinearity</i>. Published online 2014:1829-1858. doi:<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>","chicago":"Barkhofen, Sonja, F Faure, and T Weich. “Resonance Chains in Open Systems, Generalized Zeta Functions and Clustering of the Length Spectrum.” <i>Nonlinearity</i>, 2014, 1829–58. <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">https://doi.org/10.1088/0951-7715/27/8/1829</a>.","ieee":"S. Barkhofen, F. Faure, and T. Weich, “Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum,” <i>Nonlinearity</i>, pp. 1829–1858, 2014, doi: <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>.","apa":"Barkhofen, S., Faure, F., &#38; Weich, T. (2014). Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum. <i>Nonlinearity</i>, 1829–1858. <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">https://doi.org/10.1088/0951-7715/27/8/1829</a>","mla":"Barkhofen, Sonja, et al. “Resonance Chains in Open Systems, Generalized Zeta Functions and Clustering of the Length Spectrum.” <i>Nonlinearity</i>, 2014, pp. 1829–58, doi:<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>.","bibtex":"@article{Barkhofen_Faure_Weich_2014, title={Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum}, DOI={<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>}, journal={Nonlinearity}, author={Barkhofen, Sonja and Faure, F and Weich, T}, year={2014}, pages={1829–1858} }","short":"S. Barkhofen, F. Faure, T. Weich, Nonlinearity (2014) 1829–1858."},"page":"1829-1858","date_updated":"2022-01-06T06:57:21Z","author":[{"id":"48188","full_name":"Barkhofen, Sonja","last_name":"Barkhofen","first_name":"Sonja"},{"first_name":"F","last_name":"Faure","full_name":"Faure, F"},{"last_name":"Weich","full_name":"Weich, T","first_name":"T"}],"date_created":"2021-10-19T07:14:45Z","title":"Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum","doi":"10.1088/0951-7715/27/8/1829"},{"language":[{"iso":"eng"}],"keyword":["Applied Mathematics","General Physics and Astronomy","Mathematical Physics","Statistical and Nonlinear Physics"],"external_id":{"arxiv":["1403.7771 "]},"publication":"Nonlinearity","title":"Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum","date_created":"2022-05-17T12:58:25Z","publisher":"IOP Publishing","year":"2014","issue":"8","user_id":"48188","department":[{"_id":"10"},{"_id":"548"},{"_id":"288"}],"_id":"31296","status":"public","type":"journal_article","doi":"10.1088/0951-7715/27/8/1829","author":[{"first_name":"Sonja","last_name":"Barkhofen","full_name":"Barkhofen, Sonja","id":"48188"},{"full_name":"Faure, F","last_name":"Faure","first_name":"F"},{"orcid":"0000-0002-9648-6919","last_name":"Weich","id":"49178","full_name":"Weich, Tobias","first_name":"Tobias"}],"volume":27,"date_updated":"2023-01-19T08:56:12Z","citation":{"apa":"Barkhofen, S., Faure, F., &#38; Weich, T. (2014). Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum. <i>Nonlinearity</i>, <i>27</i>(8), 1829–1858. <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">https://doi.org/10.1088/0951-7715/27/8/1829</a>","mla":"Barkhofen, Sonja, et al. “Resonance Chains in Open Systems, Generalized Zeta Functions and Clustering of the Length Spectrum.” <i>Nonlinearity</i>, vol. 27, no. 8, IOP Publishing, 2014, pp. 1829–58, doi:<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>.","short":"S. Barkhofen, F. Faure, T. Weich, Nonlinearity 27 (2014) 1829–1858.","bibtex":"@article{Barkhofen_Faure_Weich_2014, title={Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum}, volume={27}, DOI={<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>}, number={8}, journal={Nonlinearity}, publisher={IOP Publishing}, author={Barkhofen, Sonja and Faure, F and Weich, Tobias}, year={2014}, pages={1829–1858} }","chicago":"Barkhofen, Sonja, F Faure, and Tobias Weich. “Resonance Chains in Open Systems, Generalized Zeta Functions and Clustering of the Length Spectrum.” <i>Nonlinearity</i> 27, no. 8 (2014): 1829–58. <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">https://doi.org/10.1088/0951-7715/27/8/1829</a>.","ieee":"S. Barkhofen, F. Faure, and T. Weich, “Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum,” <i>Nonlinearity</i>, vol. 27, no. 8, pp. 1829–1858, 2014, doi: <a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>.","ama":"Barkhofen S, Faure F, Weich T. Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum. <i>Nonlinearity</i>. 2014;27(8):1829-1858. doi:<a href=\"https://doi.org/10.1088/0951-7715/27/8/1829\">10.1088/0951-7715/27/8/1829</a>"},"intvolume":"        27","page":"1829-1858","publication_status":"published","publication_identifier":{"issn":["0951-7715","1361-6544"]}},{"citation":{"short":"M. Dellnitz, G. Froyland, S. Sertl, Nonlinearity (2000) 1171–1188.","bibtex":"@article{Dellnitz_Froyland_Sertl_2000, title={On the isolated spectrum of the Perron-Frobenius operator}, DOI={<a href=\"https://doi.org/10.1088/0951-7715/13/4/310\">10.1088/0951-7715/13/4/310</a>}, journal={Nonlinearity}, author={Dellnitz, Michael and Froyland, Gary and Sertl, Stefan}, year={2000}, pages={1171–1188} }","mla":"Dellnitz, Michael, et al. “On the Isolated Spectrum of the Perron-Frobenius Operator.” <i>Nonlinearity</i>, 2000, pp. 1171–88, doi:<a href=\"https://doi.org/10.1088/0951-7715/13/4/310\">10.1088/0951-7715/13/4/310</a>.","apa":"Dellnitz, M., Froyland, G., &#38; Sertl, S. (2000). On the isolated spectrum of the Perron-Frobenius operator. <i>Nonlinearity</i>, 1171–1188. <a href=\"https://doi.org/10.1088/0951-7715/13/4/310\">https://doi.org/10.1088/0951-7715/13/4/310</a>","ama":"Dellnitz M, Froyland G, Sertl S. On the isolated spectrum of the Perron-Frobenius operator. <i>Nonlinearity</i>. 2000:1171-1188. doi:<a href=\"https://doi.org/10.1088/0951-7715/13/4/310\">10.1088/0951-7715/13/4/310</a>","ieee":"M. Dellnitz, G. Froyland, and S. 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Generic bifurcation of Hamiltonian vector fields with symmetry. <i>Nonlinearity</i>, 979–996. <a href=\"https://doi.org/10.1088/0951-7715/5/4/008\">https://doi.org/10.1088/0951-7715/5/4/008</a>","short":"M. Dellnitz, I. Melbourne, J.E. 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