[{"publication":"Studies in Applied Mathematics","abstract":[{"text":"<jats:title>Abstract</jats:title><jats:p>We give an overview of analytical results concerned with chemotaxis systems where the signal is absorbed. We recall results on existence and properties of solutions for the prototypical chemotaxis‐consumption model and various variants and review more recent findings on its ability to support the emergence of spatial structures.</jats:p>","lang":"eng"}],"keyword":["Applied Mathematics"],"language":[{"iso":"eng"}],"issue":"4","year":"2023","publisher":"Wiley","date_created":"2024-04-07T12:50:45Z","title":"Depleting the signal: Analysis of chemotaxis‐consumption models—A survey","type":"journal_article","status":"public","_id":"53338","user_id":"31496","publication_status":"published","publication_identifier":{"issn":["0022-2526","1467-9590"]},"citation":{"ieee":"J. Lankeit and M. Winkler, “Depleting the signal: Analysis of chemotaxis‐consumption models—A survey,” <i>Studies in Applied Mathematics</i>, vol. 151, no. 4, pp. 1197–1229, 2023, doi: <a href=\"https://doi.org/10.1111/sapm.12625\">10.1111/sapm.12625</a>.","chicago":"Lankeit, Johannes, and Michael Winkler. “Depleting the Signal: Analysis of Chemotaxis‐consumption Models—A Survey.” <i>Studies in Applied Mathematics</i> 151, no. 4 (2023): 1197–1229. <a href=\"https://doi.org/10.1111/sapm.12625\">https://doi.org/10.1111/sapm.12625</a>.","ama":"Lankeit J, Winkler M. Depleting the signal: Analysis of chemotaxis‐consumption models—A survey. <i>Studies in Applied Mathematics</i>. 2023;151(4):1197-1229. doi:<a href=\"https://doi.org/10.1111/sapm.12625\">10.1111/sapm.12625</a>","short":"J. Lankeit, M. Winkler, Studies in Applied Mathematics 151 (2023) 1197–1229.","bibtex":"@article{Lankeit_Winkler_2023, title={Depleting the signal: Analysis of chemotaxis‐consumption models—A survey}, volume={151}, DOI={<a href=\"https://doi.org/10.1111/sapm.12625\">10.1111/sapm.12625</a>}, number={4}, journal={Studies in Applied Mathematics}, publisher={Wiley}, author={Lankeit, Johannes and Winkler, Michael}, year={2023}, pages={1197–1229} }","mla":"Lankeit, Johannes, and Michael Winkler. “Depleting the Signal: Analysis of Chemotaxis‐consumption Models—A Survey.” <i>Studies in Applied Mathematics</i>, vol. 151, no. 4, Wiley, 2023, pp. 1197–229, doi:<a href=\"https://doi.org/10.1111/sapm.12625\">10.1111/sapm.12625</a>.","apa":"Lankeit, J., &#38; Winkler, M. (2023). Depleting the signal: Analysis of chemotaxis‐consumption models—A survey. <i>Studies in Applied Mathematics</i>, <i>151</i>(4), 1197–1229. <a href=\"https://doi.org/10.1111/sapm.12625\">https://doi.org/10.1111/sapm.12625</a>"},"intvolume":"       151","page":"1197-1229","date_updated":"2025-12-18T20:16:04Z","author":[{"first_name":"Johannes","full_name":"Lankeit, Johannes","last_name":"Lankeit"},{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"volume":151,"doi":"10.1111/sapm.12625"},{"status":"public","publication":"ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE","type":"journal_article","language":[{"iso":"eng"}],"article_number":"286","user_id":"31496","_id":"63243","citation":{"apa":"Colasuonno, F., &#38; Winkler, M. (2023). Stability vs.~instability of singular steady states in the parabolic-elliptic Keller-Segel system on $\\R^n$. <i>ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE</i>, Article 286. <a href=\"https://doi.org/10.2422/2036-2145.202303_006\">https://doi.org/10.2422/2036-2145.202303_006</a>","short":"F. Colasuonno, M. Winkler, ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE (2023).","bibtex":"@article{Colasuonno_Winkler_2023, title={Stability vs.~instability of singular steady states in the parabolic-elliptic Keller-Segel system on $\\R^n$}, DOI={<a href=\"https://doi.org/10.2422/2036-2145.202303_006\">10.2422/2036-2145.202303_006</a>}, number={286}, journal={ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE}, publisher={Scuola Normale Superiore - Edizioni della Normale}, author={Colasuonno, Francesca and Winkler, Michael}, year={2023} }","mla":"Colasuonno, Francesca, and Michael Winkler. “Stability vs.~instability of Singular Steady States in the Parabolic-Elliptic Keller-Segel System on $\\R^n$.” <i>ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE</i>, 286, Scuola Normale Superiore - Edizioni della Normale, 2023, doi:<a href=\"https://doi.org/10.2422/2036-2145.202303_006\">10.2422/2036-2145.202303_006</a>.","ama":"Colasuonno F, Winkler M. Stability vs.~instability of singular steady states in the parabolic-elliptic Keller-Segel system on $\\R^n$. <i>ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE</i>. Published online 2023. doi:<a href=\"https://doi.org/10.2422/2036-2145.202303_006\">10.2422/2036-2145.202303_006</a>","chicago":"Colasuonno, Francesca, and Michael Winkler. “Stability vs.~instability of Singular Steady States in the Parabolic-Elliptic Keller-Segel System on $\\R^n$.” <i>ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE</i>, 2023. <a href=\"https://doi.org/10.2422/2036-2145.202303_006\">https://doi.org/10.2422/2036-2145.202303_006</a>.","ieee":"F. Colasuonno and M. Winkler, “Stability vs.~instability of singular steady states in the parabolic-elliptic Keller-Segel system on $\\R^n$,” <i>ANNALI SCUOLA NORMALE SUPERIORE - CLASSE DI SCIENZE</i>, Art. no. 286, 2023, doi: <a href=\"https://doi.org/10.2422/2036-2145.202303_006\">10.2422/2036-2145.202303_006</a>."},"year":"2023","publication_identifier":{"issn":["2036-2145","0391-173X"]},"publication_status":"published","doi":"10.2422/2036-2145.202303_006","title":"Stability vs.~instability of singular steady states in the parabolic-elliptic Keller-Segel system on $\\R^n$","author":[{"last_name":"Colasuonno","full_name":"Colasuonno, Francesca","first_name":"Francesca"},{"last_name":"Winkler","full_name":"Winkler, Michael","id":"31496","first_name":"Michael"}],"date_created":"2025-12-18T18:58:40Z","date_updated":"2025-12-18T20:17:21Z","publisher":"Scuola Normale Superiore - Edizioni della Normale"},{"language":[{"iso":"eng"}],"_id":"35528","department":[{"_id":"34"},{"_id":"10"},{"_id":"90"}],"user_id":"15645","status":"public","publication":"Nonlinearity","type":"journal_article","title":"Radial solutions to a chemotaxis-consumption model involving prescribed signal concentrations on the boundary","date_updated":"2023-01-20T13:18:15Z","volume":35,"author":[{"last_name":"Lankeit","full_name":"Lankeit, Johannes","first_name":"Johannes"},{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"date_created":"2023-01-09T15:33:38Z","year":"2022","page":"719-749","intvolume":"        35","citation":{"ieee":"J. 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Radial solutions to a chemotaxis-consumption model involving prescribed signal concentrations on the boundary. <i>Nonlinearity</i>. 2022;35:719-749.","bibtex":"@article{Lankeit_Winkler_2022, title={Radial solutions to a chemotaxis-consumption model involving prescribed signal concentrations on the boundary}, volume={35}, journal={Nonlinearity}, author={Lankeit, Johannes and Winkler, Michael}, year={2022}, pages={719–749} }","mla":"Lankeit, Johannes, and Michael Winkler. “Radial Solutions to a Chemotaxis-Consumption Model Involving Prescribed Signal Concentrations on the Boundary.” <i>Nonlinearity</i>, vol. 35, 2022, pp. 719–49.","short":"J. Lankeit, M. Winkler, Nonlinearity 35 (2022) 719–749.","apa":"Lankeit, J., &#38; Winkler, M. (2022). Radial solutions to a chemotaxis-consumption model involving prescribed signal concentrations on the boundary. <i>Nonlinearity</i>, <i>35</i>, 719–749."}},{"year":"2022","intvolume":"       389","page":"439-489","citation":{"mla":"Winkler, Michael. “Reaction-Driven Relaxation in Threee-Dimensional Keller-Segel-Navier-Stokes Interaction.” <i>Communications in Mathematical Physics</i>, vol. 389, 2022, pp. 439–89.","bibtex":"@article{Winkler_2022, title={Reaction-driven relaxation in threee-dimensional Keller-Segel-Navier-Stokes interaction.}, volume={389}, journal={Communications in Mathematical Physics}, author={Winkler, Michael}, year={2022}, pages={439–489} }","short":"M. Winkler, Communications in Mathematical Physics 389 (2022) 439–489.","apa":"Winkler, M. (2022). Reaction-driven relaxation in threee-dimensional Keller-Segel-Navier-Stokes interaction. <i>Communications in Mathematical Physics</i>, <i>389</i>, 439–489.","ama":"Winkler M. 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Xiang, “A smallness condition ensuring boundedness in a two-dimensional chemotaxis-Navier-Stokes system involving Dirichlet boundary conditions for the signal.,” <i>Acta Mathematica Sinica (English Series)</i>, vol. 38, pp. 985–1001, 2022."},"year":"2022","language":[{"iso":"eng"}],"department":[{"_id":"34"},{"_id":"10"},{"_id":"90"}],"user_id":"15645","_id":"35565","status":"public","publication":"Acta Mathematica Sinica (English Series)","type":"journal_article"},{"publication":"Analysis and Applications","type":"journal_article","status":"public","_id":"35560","department":[{"_id":"34"},{"_id":"10"},{"_id":"90"}],"user_id":"15645","language":[{"iso":"eng"}],"year":"2022","intvolume":"        20","page":"141-170","citation":{"ama":"Wang Y, Winkler M, Xiang Z. 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Nonnegative solutions to a doubly degenerate nutrient taxis system . <i>Communications on Pure and Applied Analysis</i>. 2022;21:687-784.","ieee":"G. Li and M. Winkler, “Nonnegative solutions to a doubly degenerate nutrient taxis system ,” <i>Communications on Pure and Applied Analysis</i>, vol. 21, pp. 687–784, 2022.","chicago":"Li, Genglin, and Michael Winkler. “Nonnegative Solutions to a Doubly Degenerate Nutrient Taxis System .” <i>Communications on Pure and Applied Analysis</i> 21 (2022): 687–784.","bibtex":"@article{Li_Winkler_2022, title={Nonnegative solutions to a doubly degenerate nutrient taxis system }, volume={21}, journal={Communications on Pure and Applied Analysis}, author={Li, Genglin and Winkler, Michael}, year={2022}, pages={687–784} }","short":"G. Li, M. Winkler, Communications on Pure and Applied Analysis 21 (2022) 687–784.","mla":"Li, Genglin, and Michael Winkler. “Nonnegative Solutions to a Doubly Degenerate Nutrient Taxis System .” <i>Communications on Pure and Applied Analysis</i>, vol. 21, 2022, pp. 687–784.","apa":"Li, G., &#38; Winkler, M. (2022). Nonnegative solutions to a doubly degenerate nutrient taxis system . <i>Communications on Pure and Applied Analysis</i>, <i>21</i>, 687–784."},"page":"687-784","intvolume":"        21","language":[{"iso":"eng"}],"_id":"35532","user_id":"15645","department":[{"_id":"34"},{"_id":"10"},{"_id":"90"}],"status":"public","type":"journal_article","publication":"Communications on Pure and Applied Analysis"},{"abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title><jats:p>The chemotaxis–Stokes system<jats:disp-formula id=\"j_ans-2022-0004_eq_001\"><jats:alternatives><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_001.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"block\"><m:mfenced open=\"{\" close=\"\"><m:mrow><m:mtable displaystyle=\"true\"><m:mtr><m:mtd columnalign=\"left\"><m:msub><m:mrow><m:mi>n</m:mi></m:mrow><m:mrow><m:mi>t</m:mi></m:mrow></m:msub><m:mo>+</m:mo><m:mi>u</m:mi><m:mo>⋅</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi>n</m:mi><m:mo>=</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mo>⋅</m:mo><m:mrow><m:mo stretchy=\"false\">(</m:mo><m:mrow/></m:mrow><m:mi>D</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>n</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi>n</m:mi><m:mrow><m:mo stretchy=\"false\">)</m:mo><m:mrow/></m:mrow><m:mo>−</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mo>⋅</m:mo><m:mrow><m:mo stretchy=\"false\">(</m:mo><m:mrow/></m:mrow><m:mi>n</m:mi><m:mi>S</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>x</m:mi><m:mo>,</m:mo><m:mi>n</m:mi><m:mo>,</m:mo><m:mi>c</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>⋅</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi>c</m:mi><m:mrow><m:mo stretchy=\"false\">)</m:mo><m:mrow/></m:mrow><m:mo>,</m:mo></m:mtd></m:mtr><m:mtr><m:mtd columnalign=\"left\"><m:msub><m:mrow><m:mi>c</m:mi></m:mrow><m:mrow><m:mi>t</m:mi></m:mrow></m:msub><m:mo>+</m:mo><m:mi>u</m:mi><m:mo>⋅</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi>c</m:mi><m:mo>=</m:mo><m:mi mathvariant=\"normal\">Δ</m:mi><m:mi>c</m:mi><m:mo>−</m:mo><m:mi>n</m:mi><m:mi>c</m:mi><m:mo>,</m:mo></m:mtd></m:mtr><m:mtr><m:mtd columnalign=\"left\"><m:msub><m:mrow><m:mi>u</m:mi></m:mrow><m:mrow><m:mi>t</m:mi></m:mrow></m:msub><m:mo>=</m:mo><m:mi mathvariant=\"normal\">Δ</m:mi><m:mi>u</m:mi><m:mo>+</m:mo><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi>P</m:mi><m:mo>+</m:mo><m:mi>n</m:mi><m:mrow><m:mo>∇</m:mo></m:mrow><m:mi mathvariant=\"normal\">Φ</m:mi><m:mo>,</m:mo><m:mspace width=\"1.0em\"/><m:mrow><m:mo>∇</m:mo></m:mrow><m:mo>⋅</m:mo><m:mi>u</m:mi><m:mo>=</m:mo><m:mn>0</m:mn><m:mo>,</m:mo></m:mtd></m:mtr></m:mtable></m:mrow></m:mfenced></m:math><jats:tex-math>\\left\\{\\begin{array}{l}{n}_{t}+u\\cdot \\nabla n=\\nabla \\cdot (D\\left(n)\\nabla n)-\\nabla \\cdot (nS\\left(x,n,c)\\cdot \\nabla c),\\\\ {c}_{t}+u\\cdot \\nabla c=\\Delta c-nc,\\\\ {u}_{t}=\\Delta u+\\nabla P+n\\nabla \\Phi ,\\hspace{1.0em}\\nabla \\cdot u=0,\\end{array}\\right.</jats:tex-math></jats:alternatives></jats:disp-formula>is considered in a smoothly bounded convex domain<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_002.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi mathvariant=\"normal\">Ω</m:mi><m:mo>⊂</m:mo><m:msup><m:mrow><m:mi mathvariant=\"double-struck\">R</m:mi></m:mrow><m:mrow><m:mn>3</m:mn></m:mrow></m:msup></m:math><jats:tex-math>\\Omega \\subset {{\\mathbb{R}}}^{3}</jats:tex-math></jats:alternatives></jats:inline-formula>, with given suitably regular functions<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_003.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>D</m:mi><m:mo>:</m:mo><m:mrow><m:mo stretchy=\"false\">[</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo stretchy=\"false\">)</m:mo></m:mrow><m:mo>→</m:mo><m:mrow><m:mo stretchy=\"false\">[</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo stretchy=\"false\">)</m:mo></m:mrow></m:math><jats:tex-math>D:{[}0,\\infty )\\to {[}0,\\infty )</jats:tex-math></jats:alternatives></jats:inline-formula>,<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_004.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>S</m:mi><m:mo>:</m:mo><m:mover accent=\"true\"><m:mrow><m:mi mathvariant=\"normal\">Ω</m:mi></m:mrow><m:mrow><m:mo stretchy=\"true\">¯</m:mo></m:mrow></m:mover><m:mo>×</m:mo><m:mrow><m:mo stretchy=\"false\">[</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo stretchy=\"false\">)</m:mo></m:mrow><m:mo>×</m:mo><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>→</m:mo><m:msup><m:mrow><m:mi mathvariant=\"double-struck\">R</m:mi></m:mrow><m:mrow><m:mn>3</m:mn><m:mo>×</m:mo><m:mn>3</m:mn></m:mrow></m:msup></m:math><jats:tex-math>S:\\overline{\\Omega }\\times {[}0,\\infty )\\times \\left(0,\\infty )\\to {{\\mathbb{R}}}^{3\\times 3}</jats:tex-math></jats:alternatives></jats:inline-formula>and<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_005.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi mathvariant=\"normal\">Φ</m:mi><m:mo>:</m:mo><m:mover accent=\"true\"><m:mrow><m:mi mathvariant=\"normal\">Ω</m:mi></m:mrow><m:mrow><m:mo stretchy=\"true\">¯</m:mo></m:mrow></m:mover><m:mo>→</m:mo><m:mi mathvariant=\"double-struck\">R</m:mi></m:math><jats:tex-math>\\Phi :\\overline{\\Omega }\\to {\\mathbb{R}}</jats:tex-math></jats:alternatives></jats:inline-formula>such that<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_006.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>D</m:mi><m:mo>&gt;</m:mo><m:mn>0</m:mn></m:math><jats:tex-math>D\\gt 0</jats:tex-math></jats:alternatives></jats:inline-formula>on<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_007.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:math><jats:tex-math>\\left(0,\\infty )</jats:tex-math></jats:alternatives></jats:inline-formula>. It is shown that if with some nondecreasing<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_008.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:msub><m:mrow><m:mi>S</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub><m:mo>:</m:mo><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>→</m:mo><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:math><jats:tex-math>{S}_{0}:\\left(0,\\infty )\\to \\left(0,\\infty )</jats:tex-math></jats:alternatives></jats:inline-formula>we have<jats:disp-formula id=\"j_ans-2022-0004_eq_002\"><jats:alternatives><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_009.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"block\"><m:mo>∣</m:mo><m:mi>S</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>x</m:mi><m:mo>,</m:mo><m:mi>n</m:mi><m:mo>,</m:mo><m:mi>c</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>∣</m:mo><m:mo>≤</m:mo><m:mfrac><m:mrow><m:msub><m:mrow><m:mi>S</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>c</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:mrow><m:mrow><m:msup><m:mrow><m:mi>c</m:mi></m:mrow><m:mrow><m:mstyle displaystyle=\"false\"><m:mfrac><m:mrow><m:mn>1</m:mn></m:mrow><m:mrow><m:mn>2</m:mn></m:mrow></m:mfrac></m:mstyle></m:mrow></m:msup></m:mrow></m:mfrac><m:mspace width=\"1.0em\"/><m:mspace width=\"0.1em\"/><m:mtext>for all</m:mtext><m:mspace width=\"0.1em\"/><m:mspace width=\"0.33em\"/><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>x</m:mi><m:mo>,</m:mo><m:mi>n</m:mi><m:mo>,</m:mo><m:mi>c</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>∈</m:mo><m:mover accent=\"true\"><m:mrow><m:mi mathvariant=\"normal\">Ω</m:mi></m:mrow><m:mrow><m:mo stretchy=\"true\">¯</m:mo></m:mrow></m:mover><m:mo>×</m:mo><m:mrow><m:mo stretchy=\"false\">[</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo stretchy=\"false\">)</m:mo></m:mrow><m:mo>×</m:mo><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn><m:mo>,</m:mo><m:mi>∞</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>,</m:mo></m:math><jats:tex-math>| S\\left(x,n,c)| \\le \\frac{{S}_{0}\\left(c)}{{c}^{\\tfrac{1}{2}}}\\hspace{1.0em}\\hspace{0.1em}\\text{for all}\\hspace{0.1em}\\hspace{0.33em}\\left(x,n,c)\\in \\overline{\\Omega }\\times {[}0,\\infty )\\times \\left(0,\\infty ),</jats:tex-math></jats:alternatives></jats:disp-formula>then for all<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_010.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>M</m:mi><m:mo>&gt;</m:mo><m:mn>0</m:mn></m:math><jats:tex-math>M\\gt 0</jats:tex-math></jats:alternatives></jats:inline-formula>there exists<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_011.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>L</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>M</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>&gt;</m:mo><m:mn>0</m:mn></m:math><jats:tex-math>L\\left(M)\\gt 0</jats:tex-math></jats:alternatives></jats:inline-formula>such that whenever<jats:disp-formula id=\"j_ans-2022-0004_eq_003\"><jats:alternatives><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_012.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"block\"><m:munder><m:mrow><m:mi>liminf</m:mi></m:mrow><m:mrow><m:mi>n</m:mi><m:mo>→</m:mo><m:mi>∞</m:mi></m:mrow></m:munder><m:mi>D</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>n</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>&gt;</m:mo><m:mi>L</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>M</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mspace width=\"1.0em\"/><m:mspace width=\"0.1em\"/><m:mtext>and</m:mtext><m:mspace width=\"0.1em\"/><m:mspace width=\"1.0em\"/><m:munder><m:mrow><m:mi>liminf</m:mi></m:mrow><m:mrow><m:mi>n</m:mi><m:mo>↘</m:mo><m:mn>0</m:mn></m:mrow></m:munder><m:mfrac><m:mrow><m:mi>D</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>n</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:mrow><m:mrow><m:mi>n</m:mi></m:mrow></m:mfrac><m:mo>&gt;</m:mo><m:mn>0</m:mn><m:mo>,</m:mo></m:math><jats:tex-math>\\mathop{\\mathrm{liminf}}\\limits_{n\\to \\infty }D\\left(n)\\gt L\\left(M)\\hspace{1.0em}\\hspace{0.1em}\\text{and}\\hspace{0.1em}\\hspace{1.0em}\\mathop{\\mathrm{liminf}}\\limits_{n\\searrow 0}\\frac{D\\left(n)}{n}\\gt 0,</jats:tex-math></jats:alternatives></jats:disp-formula>for all sufficiently regular initial data<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_013.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mrow><m:mo>(</m:mo><m:mrow><m:msub><m:mrow><m:mi>n</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub><m:mo>,</m:mo><m:msub><m:mrow><m:mi>c</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub><m:mo>,</m:mo><m:msub><m:mrow><m:mi>u</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub></m:mrow><m:mo>)</m:mo></m:mrow></m:math><jats:tex-math>\\left({n}_{0},{c}_{0},{u}_{0})</jats:tex-math></jats:alternatives></jats:inline-formula>fulfilling<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_014.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mo>‖</m:mo><m:msub><m:mrow><m:mi>c</m:mi></m:mrow><m:mrow><m:mn>0</m:mn></m:mrow></m:msub><m:msub><m:mrow><m:mo>‖</m:mo></m:mrow><m:mrow><m:msup><m:mrow><m:mi>L</m:mi></m:mrow><m:mrow><m:mi>∞</m:mi></m:mrow></m:msup><m:mrow><m:mo>(</m:mo><m:mrow><m:mi mathvariant=\"normal\">Ω</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:mrow></m:msub><m:mo>≤</m:mo><m:mi>M</m:mi></m:math><jats:tex-math>\\Vert {c}_{0}{\\Vert }_{{L}^{\\infty }\\left(\\Omega )}\\le M</jats:tex-math></jats:alternatives></jats:inline-formula>an associated no-flux/no-flux/Dirichlet initial-boundary value problem admits a global bounded weak solution, classical if additionally<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_015.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>D</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mn>0</m:mn></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>&gt;</m:mo><m:mn>0</m:mn></m:math><jats:tex-math>D\\left(0)\\gt 0</jats:tex-math></jats:alternatives></jats:inline-formula>. When combined with previously known results, this particularly implies global existence of bounded solutions when<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_016.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>D</m:mi><m:mrow><m:mo>(</m:mo><m:mrow><m:mi>n</m:mi></m:mrow><m:mo>)</m:mo></m:mrow><m:mo>=</m:mo><m:msup><m:mrow><m:mi>n</m:mi></m:mrow><m:mrow><m:mi>m</m:mi><m:mo>−</m:mo><m:mn>1</m:mn></m:mrow></m:msup></m:math><jats:tex-math>D\\left(n)={n}^{m-1}</jats:tex-math></jats:alternatives></jats:inline-formula>,<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_017.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>n</m:mi><m:mo>≥</m:mo><m:mn>0</m:mn></m:math><jats:tex-math>n\\ge 0</jats:tex-math></jats:alternatives></jats:inline-formula>, with arbitrary<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_018.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mi>m</m:mi><m:mo>&gt;</m:mo><m:mn>1</m:mn></m:math><jats:tex-math>m\\gt 1</jats:tex-math></jats:alternatives></jats:inline-formula>, but beyond this asserts global boundedness also in the presence of diffusivities which exhibit arbitrarily slow divergence to<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_ans-2022-0004_eq_019.png\"/><m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mo>+</m:mo><m:mi>∞</m:mi></m:math><jats:tex-math>+\\infty</jats:tex-math></jats:alternatives></jats:inline-formula>at large densities and of possibly singular chemotactic sensitivities.</jats:p>"}],"status":"public","publication":"Advanced Nonlinear Studies","type":"journal_article","language":[{"iso":"eng"}],"_id":"63310","user_id":"31496","year":"2022","page":"88-117","intvolume":"        22","citation":{"apa":"Winkler, M. (2022). Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings. <i>Advanced Nonlinear Studies</i>, <i>22</i>(1), 88–117. <a href=\"https://doi.org/10.1515/ans-2022-0004\">https://doi.org/10.1515/ans-2022-0004</a>","bibtex":"@article{Winkler_2022, title={Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings}, volume={22}, DOI={<a href=\"https://doi.org/10.1515/ans-2022-0004\">10.1515/ans-2022-0004</a>}, number={1}, journal={Advanced Nonlinear Studies}, publisher={Walter de Gruyter GmbH}, author={Winkler, Michael}, year={2022}, pages={88–117} }","short":"M. Winkler, Advanced Nonlinear Studies 22 (2022) 88–117.","mla":"Winkler, Michael. “Chemotaxis-Stokes Interaction with Very Weak Diffusion Enhancement: Blow-up Exclusion via Detection of Absorption-Induced Entropy Structures Involving Multiplicative Couplings.” <i>Advanced Nonlinear Studies</i>, vol. 22, no. 1, Walter de Gruyter GmbH, 2022, pp. 88–117, doi:<a href=\"https://doi.org/10.1515/ans-2022-0004\">10.1515/ans-2022-0004</a>.","chicago":"Winkler, Michael. “Chemotaxis-Stokes Interaction with Very Weak Diffusion Enhancement: Blow-up Exclusion via Detection of Absorption-Induced Entropy Structures Involving Multiplicative Couplings.” <i>Advanced Nonlinear Studies</i> 22, no. 1 (2022): 88–117. <a href=\"https://doi.org/10.1515/ans-2022-0004\">https://doi.org/10.1515/ans-2022-0004</a>.","ieee":"M. Winkler, “Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings,” <i>Advanced Nonlinear Studies</i>, vol. 22, no. 1, pp. 88–117, 2022, doi: <a href=\"https://doi.org/10.1515/ans-2022-0004\">10.1515/ans-2022-0004</a>.","ama":"Winkler M. Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings. <i>Advanced Nonlinear Studies</i>. 2022;22(1):88-117. doi:<a href=\"https://doi.org/10.1515/ans-2022-0004\">10.1515/ans-2022-0004</a>"},"publication_identifier":{"issn":["2169-0375"]},"publication_status":"published","issue":"1","title":"Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings","doi":"10.1515/ans-2022-0004","publisher":"Walter de Gruyter GmbH","date_updated":"2025-12-18T20:05:30Z","volume":22,"date_created":"2025-12-18T19:29:40Z","author":[{"first_name":"Michael","last_name":"Winkler","id":"31496","full_name":"Winkler, Michael"}]},{"user_id":"31496","_id":"63305","language":[{"iso":"eng"}],"article_number":"108","type":"journal_article","publication":"Calculus of Variations and Partial Differential Equations","status":"public","abstract":[{"text":"<jats:title>Abstract</jats:title><jats:p>A no-flux initial-boundary value problem for the doubly degenrate parabolic system <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\left\\{ \\begin{array}{l} u_t = \\nabla \\cdot \\big ( uv\\nabla u\\big ) + \\ell uv, \\\\ v_t = \\Delta v - uv, \\end{array} \\right. \\qquad \\qquad (\\star ) \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\r\n                            <mml:mfenced>\r\n                              <mml:mrow>\r\n                                <mml:mtable>\r\n                                  <mml:mtr>\r\n                                    <mml:mtd>\r\n                                      <mml:mrow>\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>∇</mml:mi>\r\n                                        <mml:mo>·</mml:mo>\r\n                                        <mml:mrow>\r\n                                          <mml:mo>(</mml:mo>\r\n                                        </mml:mrow>\r\n                                        <mml:mi>u</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n                                        <mml:mi>∇</mml:mi>\r\n                                        <mml:mi>u</mml:mi>\r\n                                        <mml:mrow>\r\n                                          <mml:mo>)</mml:mo>\r\n                                        </mml:mrow>\r\n                                        <mml:mo>+</mml:mo>\r\n                                        <mml:mi>ℓ</mml:mi>\r\n                                        <mml:mi>u</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n                                        <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n                                    </mml:mtd>\r\n                                  </mml:mtr>\r\n                                  <mml:mtr>\r\n                                    <mml:mtd>\r\n                                      <mml:mrow>\r\n                                        <mml:mrow/>\r\n                                        <mml:msub>\r\n                                          <mml:mi>v</mml:mi>\r\n                                          <mml:mi>t</mml:mi>\r\n                                        </mml:msub>\r\n                                        <mml:mo>=</mml:mo>\r\n                                        <mml:mi>Δ</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n                                        <mml:mo>-</mml:mo>\r\n                                        <mml:mi>u</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n                                        <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n                                    </mml:mtd>\r\n                                  </mml:mtr>\r\n                                </mml:mtable>\r\n                              </mml:mrow>\r\n                            </mml:mfenced>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n                              <mml:mo>⋆</mml:mo>\r\n                              <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>is considered in a smoothly bounded convex domain <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Omega \\subset \\mathbb {R}^n$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>Ω</mml:mi>\r\n                    <mml:mo>⊂</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mrow>\r\n                        <mml:mi>R</mml:mi>\r\n                      </mml:mrow>\r\n                      <mml:mi>n</mml:mi>\r\n                    </mml:msup>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, with <jats:inline-formula><jats:alternatives><jats:tex-math>$$n\\ge 1$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n                    <mml:mo>≥</mml:mo>\r\n                    <mml:mn>1</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\ell \\ge 0$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>ℓ</mml:mi>\r\n                    <mml:mo>≥</mml:mo>\r\n                    <mml:mn>0</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>. The first of the main results asserts that for nonnegative initial data <jats:inline-formula><jats:alternatives><jats:tex-math>$$(u_0,v_0)\\in (L^\\infty (\\Omega ))^2$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\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:msub>\r\n                        <mml:mi>v</mml:mi>\r\n                        <mml:mn>0</mml:mn>\r\n                      </mml:msub>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mrow>\r\n                        <mml:mo>(</mml:mo>\r\n                        <mml:msup>\r\n                          <mml:mi>L</mml:mi>\r\n                          <mml:mi>∞</mml:mi>\r\n                        </mml:msup>\r\n                        <mml:mrow>\r\n                          <mml:mo>(</mml:mo>\r\n                          <mml:mi>Ω</mml:mi>\r\n                          <mml:mo>)</mml:mo>\r\n                        </mml:mrow>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mn>2</mml:mn>\r\n                    </mml:msup>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0\\not \\equiv 0$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\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:mn>0</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$v_0\\not \\equiv 0$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mi>v</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n                    <mml:mo>≢</mml:mo>\r\n                    <mml:mn>0</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\sqrt{v_0}\\in W^{1,2}(\\Omega )$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msqrt>\r\n                      <mml:msub>\r\n                        <mml:mi>v</mml:mi>\r\n                        <mml:mn>0</mml:mn>\r\n                      </mml:msub>\r\n                    </mml:msqrt>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>W</mml:mi>\r\n                      <mml:mrow>\r\n                        <mml:mn>1</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mn>2</mml:mn>\r\n                      </mml:mrow>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mi>Ω</mml:mi>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, there exists a global weak solution (<jats:italic>u</jats:italic>, <jats:italic>v</jats:italic>) which, inter alia, belongs to <jats:inline-formula><jats:alternatives><jats:tex-math>$$C^0(\\overline{\\Omega }\\times (0,\\infty )) \\times C^{2,1}(\\overline{\\Omega }\\times (0,\\infty ))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mover>\r\n                        <mml:mi>Ω</mml:mi>\r\n                        <mml:mo>¯</mml:mo>\r\n                      </mml:mover>\r\n                      <mml:mo>×</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mo>(</mml:mo>\r\n                        <mml:mn>0</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mi>∞</mml:mi>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                    <mml:mo>×</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mrow>\r\n                        <mml:mn>2</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mn>1</mml:mn>\r\n                      </mml:mrow>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mover>\r\n                        <mml:mi>Ω</mml:mi>\r\n                        <mml:mo>¯</mml:mo>\r\n                      </mml:mover>\r\n                      <mml:mo>×</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mo>(</mml:mo>\r\n                        <mml:mn>0</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mi>∞</mml:mi>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> and satisfies <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\sup _{t&gt;0} \\Vert u(\\cdot ,t)\\Vert _{L^p(\\Omega )}&lt;\\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mo>sup</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mi>t</mml:mi>\r\n                        <mml:mo>&gt;</mml:mo>\r\n                        <mml:mn>0</mml:mn>\r\n                      </mml:mrow>\r\n                    </mml:msub>\r\n                    <mml:msub>\r\n                      <mml:mrow>\r\n                        <mml:mo>‖</mml:mo>\r\n                        <mml:mi>u</mml:mi>\r\n                        <mml:mrow>\r\n                          <mml:mo>(</mml:mo>\r\n                          <mml:mo>·</mml:mo>\r\n                          <mml:mo>,</mml:mo>\r\n                          <mml:mi>t</mml:mi>\r\n                          <mml:mo>)</mml:mo>\r\n                        </mml:mrow>\r\n                        <mml:mo>‖</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mrow>\r\n                        <mml:msup>\r\n                          <mml:mi>L</mml:mi>\r\n                          <mml:mi>p</mml:mi>\r\n                        </mml:msup>\r\n                        <mml:mrow>\r\n                          <mml:mo>(</mml:mo>\r\n                          <mml:mi>Ω</mml:mi>\r\n                          <mml:mo>)</mml:mo>\r\n                        </mml:mrow>\r\n                      </mml:mrow>\r\n                    </mml:msub>\r\n                    <mml:mo>&lt;</mml:mo>\r\n                    <mml:mi>∞</mml:mi>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> for all <jats:inline-formula><jats:alternatives><jats:tex-math>$$p\\in [1,p_0)$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>p</mml:mi>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:mo>[</mml:mo>\r\n                    <mml:mn>1</mml:mn>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:msub>\r\n                      <mml:mi>p</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n                    <mml:mo>)</mml:mo>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_0:=\\frac{n}{(n-2)_+}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mi>p</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n                    <mml:mo>:</mml:mo>\r\n                    <mml:mo>=</mml:mo>\r\n                    <mml:mfrac>\r\n                      <mml:mi>n</mml:mi>\r\n                      <mml:msub>\r\n                        <mml:mrow>\r\n                          <mml:mo>(</mml:mo>\r\n                          <mml:mi>n</mml:mi>\r\n                          <mml:mo>-</mml:mo>\r\n                          <mml:mn>2</mml:mn>\r\n                          <mml:mo>)</mml:mo>\r\n                        </mml:mrow>\r\n                        <mml:mo>+</mml:mo>\r\n                      </mml:msub>\r\n                    </mml:mfrac>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>. It is next seen that for each of these solutions one can find <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_\\infty \\in \\bigcap _{p\\in [1,p_0)} L^p(\\Omega )$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mi>u</mml:mi>\r\n                      <mml:mi>∞</mml:mi>\r\n                    </mml:msub>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msub>\r\n                      <mml:mo>⋂</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mi>p</mml:mi>\r\n                        <mml:mo>∈</mml:mo>\r\n                        <mml:mo>[</mml:mo>\r\n                        <mml:mn>1</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:msub>\r\n                          <mml:mi>p</mml:mi>\r\n                          <mml:mn>0</mml:mn>\r\n                        </mml:msub>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                    </mml:msub>\r\n                    <mml:msup>\r\n                      <mml:mi>L</mml:mi>\r\n                      <mml:mi>p</mml:mi>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mi>Ω</mml:mi>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> such that, within an appropriate topological setting, <jats:inline-formula><jats:alternatives><jats:tex-math>$$(u(\\cdot ,t),v(\\cdot ,t))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\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:mo>·</mml:mo>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:mi>t</mml:mi>\r\n                    <mml:mo>)</mml:mo>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:mi>v</mml:mi>\r\n                    <mml:mo>(</mml:mo>\r\n                    <mml:mo>·</mml:mo>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:mi>t</mml:mi>\r\n                    <mml:mo>)</mml:mo>\r\n                    <mml:mo>)</mml:mo>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> approaches the equilibrium <jats:inline-formula><jats:alternatives><jats:tex-math>$$(u_\\infty ,0)$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mo>(</mml:mo>\r\n                    <mml:msub>\r\n                      <mml:mi>u</mml:mi>\r\n                      <mml:mi>∞</mml:mi>\r\n                    </mml:msub>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:mn>0</mml:mn>\r\n                    <mml:mo>)</mml:mo>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> in the large time limit. Finally, in the case <jats:inline-formula><jats:alternatives><jats:tex-math>$$n\\le 5$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n                    <mml:mo>≤</mml:mo>\r\n                    <mml:mn>5</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> a result ensuring a certain stability property of any member in the uncountably large family of steady states <jats:inline-formula><jats:alternatives><jats:tex-math>$$(u_0,0)$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mo>(</mml:mo>\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:mn>0</mml:mn>\r\n                    <mml:mo>)</mml:mo>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, with arbitrary and suitably regular <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0:\\Omega \\rightarrow [0,\\infty )$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\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>Ω</mml:mi>\r\n                    <mml:mo>→</mml:mo>\r\n                    <mml:mrow>\r\n                      <mml:mo>[</mml:mo>\r\n                      <mml:mn>0</mml:mn>\r\n                      <mml:mo>,</mml:mo>\r\n                      <mml:mi>∞</mml:mi>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, is derived. This provides some rigorous evidence for the appropriateness of (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>) to model the emergence of a strikingly large variety of stable structures observed in experiments on bacterial motion in nutrient-poor environments. Essential parts of the analysis rely on the use of an apparently novel class of functional inequalities to suitably cope with the doubly degenerate diffusion mechanism in (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>).</jats:p>","lang":"eng"}],"author":[{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"date_created":"2025-12-18T19:26:32Z","volume":61,"publisher":"Springer Science and Business Media LLC","date_updated":"2025-12-18T20:04:43Z","doi":"10.1007/s00526-021-02168-2","title":"Stabilization of arbitrary structures in a doubly degenerate reaction-diffusion system modeling bacterial motion on a nutrient-poor agar","issue":"3","publication_status":"published","publication_identifier":{"issn":["0944-2669","1432-0835"]},"citation":{"chicago":"Winkler, Michael. “Stabilization of Arbitrary Structures in a Doubly Degenerate Reaction-Diffusion System Modeling Bacterial Motion on a Nutrient-Poor Agar.” <i>Calculus of Variations and Partial Differential Equations</i> 61, no. 3 (2022). <a href=\"https://doi.org/10.1007/s00526-021-02168-2\">https://doi.org/10.1007/s00526-021-02168-2</a>.","ieee":"M. Winkler, “Stabilization of arbitrary structures in a doubly degenerate reaction-diffusion system modeling bacterial motion on a nutrient-poor agar,” <i>Calculus of Variations and Partial Differential Equations</i>, vol. 61, no. 3, Art. no. 108, 2022, doi: <a href=\"https://doi.org/10.1007/s00526-021-02168-2\">10.1007/s00526-021-02168-2</a>.","ama":"Winkler M. Stabilization of arbitrary structures in a doubly degenerate reaction-diffusion system modeling bacterial motion on a nutrient-poor agar. <i>Calculus of Variations and Partial Differential Equations</i>. 2022;61(3). doi:<a href=\"https://doi.org/10.1007/s00526-021-02168-2\">10.1007/s00526-021-02168-2</a>","apa":"Winkler, M. (2022). Stabilization of arbitrary structures in a doubly degenerate reaction-diffusion system modeling bacterial motion on a nutrient-poor agar. <i>Calculus of Variations and Partial Differential Equations</i>, <i>61</i>(3), Article 108. <a href=\"https://doi.org/10.1007/s00526-021-02168-2\">https://doi.org/10.1007/s00526-021-02168-2</a>","bibtex":"@article{Winkler_2022, title={Stabilization of arbitrary structures in a doubly degenerate reaction-diffusion system modeling bacterial motion on a nutrient-poor agar}, volume={61}, DOI={<a href=\"https://doi.org/10.1007/s00526-021-02168-2\">10.1007/s00526-021-02168-2</a>}, number={3108}, journal={Calculus of Variations and Partial Differential Equations}, publisher={Springer Science and Business Media LLC}, author={Winkler, Michael}, year={2022} }","mla":"Winkler, Michael. “Stabilization of Arbitrary Structures in a Doubly Degenerate Reaction-Diffusion System Modeling Bacterial Motion on a Nutrient-Poor Agar.” <i>Calculus of Variations and Partial Differential Equations</i>, vol. 61, no. 3, 108, Springer Science and Business Media LLC, 2022, doi:<a href=\"https://doi.org/10.1007/s00526-021-02168-2\">10.1007/s00526-021-02168-2</a>.","short":"M. Winkler, Calculus of Variations and Partial Differential Equations 61 (2022)."},"intvolume":"        61","year":"2022"},{"citation":{"apa":"Winkler, M. (2022). Oscillatory decay in a degenerate parabolic equation. <i>Partial Differential Equations and Applications</i>, <i>3</i>(4), Article 47. <a href=\"https://doi.org/10.1007/s42985-022-00186-z\">https://doi.org/10.1007/s42985-022-00186-z</a>","short":"M. Winkler, Partial Differential Equations and Applications 3 (2022).","bibtex":"@article{Winkler_2022, title={Oscillatory decay in a degenerate parabolic equation}, volume={3}, DOI={<a href=\"https://doi.org/10.1007/s42985-022-00186-z\">10.1007/s42985-022-00186-z</a>}, number={447}, journal={Partial Differential Equations and Applications}, publisher={Springer Science and Business Media LLC}, author={Winkler, Michael}, year={2022} }","mla":"Winkler, Michael. “Oscillatory Decay in a Degenerate Parabolic Equation.” <i>Partial Differential Equations and Applications</i>, vol. 3, no. 4, 47, Springer Science and Business Media LLC, 2022, doi:<a href=\"https://doi.org/10.1007/s42985-022-00186-z\">10.1007/s42985-022-00186-z</a>.","ieee":"M. Winkler, “Oscillatory decay in a degenerate parabolic equation,” <i>Partial Differential Equations and Applications</i>, vol. 3, no. 4, Art. no. 47, 2022, doi: <a href=\"https://doi.org/10.1007/s42985-022-00186-z\">10.1007/s42985-022-00186-z</a>.","chicago":"Winkler, Michael. “Oscillatory Decay in a Degenerate Parabolic Equation.” <i>Partial Differential Equations and Applications</i> 3, no. 4 (2022). <a href=\"https://doi.org/10.1007/s42985-022-00186-z\">https://doi.org/10.1007/s42985-022-00186-z</a>.","ama":"Winkler M. Oscillatory decay in a degenerate parabolic equation. <i>Partial Differential Equations and Applications</i>. 2022;3(4). doi:<a href=\"https://doi.org/10.1007/s42985-022-00186-z\">10.1007/s42985-022-00186-z</a>"},"intvolume":"         3","year":"2022","issue":"4","publication_status":"published","publication_identifier":{"issn":["2662-2963","2662-2971"]},"doi":"10.1007/s42985-022-00186-z","title":"Oscillatory decay in a degenerate parabolic equation","date_created":"2025-12-18T19:30:04Z","author":[{"last_name":"Winkler","full_name":"Winkler, Michael","id":"31496","first_name":"Michael"}],"volume":3,"publisher":"Springer Science and Business Media LLC","date_updated":"2025-12-18T20:05:38Z","status":"public","abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title><jats:p>The Cauchy problem in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\mathbb {R}^n$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mi>R</mml:mi>\r\n                    </mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n                  </mml:msup>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$n\\ge 1$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n                    <mml:mo>≥</mml:mo>\r\n                    <mml:mn>1</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, for the degenerate parabolic equation <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} u_t=u^p \\Delta u \\qquad \\qquad (\\star ) \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\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:msup>\r\n                              <mml:mi>u</mml:mi>\r\n                              <mml:mi>p</mml:mi>\r\n                            </mml:msup>\r\n                            <mml:mi>Δ</mml:mi>\r\n                            <mml:mi>u</mml:mi>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n                              <mml:mo>⋆</mml:mo>\r\n                              <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>is considered for <jats:inline-formula><jats:alternatives><jats:tex-math>$$p\\ge 1$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>p</mml:mi>\r\n                    <mml:mo>≥</mml:mo>\r\n                    <mml:mn>1</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>. It is shown that given any positive <jats:inline-formula><jats:alternatives><jats:tex-math>$$f\\in C^0([0,\\infty ))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>f</mml:mi>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mo>[</mml:mo>\r\n                        <mml:mn>0</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mi>∞</mml:mi>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$$g\\in C^0([0,\\infty ))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>g</mml:mi>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n                      <mml:mrow>\r\n                        <mml:mo>[</mml:mo>\r\n                        <mml:mn>0</mml:mn>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mi>∞</mml:mi>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                      <mml:mo>)</mml:mo>\r\n                    </mml:mrow>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> satisfying <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} f(t)\\rightarrow + \\infty \\quad \\text{ and } \\quad g(t)\\rightarrow 0 \\qquad \\text{ as } t\\rightarrow \\infty , \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\r\n                            <mml:mi>f</mml:mi>\r\n                            <mml:mo>(</mml:mo>\r\n                            <mml:mi>t</mml:mi>\r\n                            <mml:mo>)</mml:mo>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mo>+</mml:mo>\r\n                            <mml:mi>∞</mml:mi>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>and</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mi>g</mml:mi>\r\n                            <mml:mo>(</mml:mo>\r\n                            <mml:mi>t</mml:mi>\r\n                            <mml:mo>)</mml:mo>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>as</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mi>t</mml:mi>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mi>∞</mml:mi>\r\n                            <mml:mo>,</mml:mo>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>one can find positive and radially symmetric continuous initial data with the property that the initial value problem for (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>) admits a positive classical solution such that <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} t^\\frac{1}{p} \\Vert u(\\cdot ,t)\\Vert _{L^\\infty (\\mathbb {R}^n)} \\rightarrow \\infty \\qquad \\text{ and } \\qquad \\Vert u(\\cdot ,t)\\Vert _{L^\\infty (\\mathbb {R}^n)} \\rightarrow 0 \\qquad \\text{ as } t\\rightarrow \\infty , \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\r\n                            <mml:msup>\r\n                              <mml:mi>t</mml:mi>\r\n                              <mml:mfrac>\r\n                                <mml:mn>1</mml:mn>\r\n                                <mml:mi>p</mml:mi>\r\n                              </mml:mfrac>\r\n                            </mml:msup>\r\n                            <mml:msub>\r\n                              <mml:mrow>\r\n                                <mml:mo>‖</mml:mo>\r\n                                <mml:mi>u</mml:mi>\r\n                                <mml:mrow>\r\n                                  <mml:mo>(</mml:mo>\r\n                                  <mml:mo>·</mml:mo>\r\n                                  <mml:mo>,</mml:mo>\r\n                                  <mml:mi>t</mml:mi>\r\n                                  <mml:mo>)</mml:mo>\r\n                                </mml:mrow>\r\n                                <mml:mo>‖</mml:mo>\r\n                              </mml:mrow>\r\n                              <mml:mrow>\r\n                                <mml:msup>\r\n                                  <mml:mi>L</mml:mi>\r\n                                  <mml:mi>∞</mml:mi>\r\n                                </mml:msup>\r\n                                <mml:mrow>\r\n                                  <mml:mo>(</mml:mo>\r\n                                  <mml:msup>\r\n                                    <mml:mrow>\r\n                                      <mml:mi>R</mml:mi>\r\n                                    </mml:mrow>\r\n                                    <mml:mi>n</mml:mi>\r\n                                  </mml:msup>\r\n                                  <mml:mo>)</mml:mo>\r\n                                </mml:mrow>\r\n                              </mml:mrow>\r\n                            </mml:msub>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mi>∞</mml:mi>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>and</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:msub>\r\n                              <mml:mrow>\r\n                                <mml:mo>‖</mml:mo>\r\n                                <mml:mi>u</mml:mi>\r\n                                <mml:mrow>\r\n                                  <mml:mo>(</mml:mo>\r\n                                  <mml:mo>·</mml:mo>\r\n                                  <mml:mo>,</mml:mo>\r\n                                  <mml:mi>t</mml:mi>\r\n                                  <mml:mo>)</mml:mo>\r\n                                </mml:mrow>\r\n                                <mml:mo>‖</mml:mo>\r\n                              </mml:mrow>\r\n                              <mml:mrow>\r\n                                <mml:msup>\r\n                                  <mml:mi>L</mml:mi>\r\n                                  <mml:mi>∞</mml:mi>\r\n                                </mml:msup>\r\n                                <mml:mrow>\r\n                                  <mml:mo>(</mml:mo>\r\n                                  <mml:msup>\r\n                                    <mml:mrow>\r\n                                      <mml:mi>R</mml:mi>\r\n                                    </mml:mrow>\r\n                                    <mml:mi>n</mml:mi>\r\n                                  </mml:msup>\r\n                                  <mml:mo>)</mml:mo>\r\n                                </mml:mrow>\r\n                              </mml:mrow>\r\n                            </mml:msub>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>as</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mi>t</mml:mi>\r\n                            <mml:mo>→</mml:mo>\r\n                            <mml:mi>∞</mml:mi>\r\n                            <mml:mo>,</mml:mo>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>but that <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\liminf _{t\\rightarrow \\infty } \\frac{t^\\frac{1}{p} \\Vert u(\\cdot ,t)\\Vert _{L^\\infty (\\mathbb {R}^n)}}{f(t)} =0 \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\r\n                            <mml:munder>\r\n                              <mml:mo>lim inf</mml:mo>\r\n                              <mml:mrow>\r\n                                <mml:mi>t</mml:mi>\r\n                                <mml:mo>→</mml:mo>\r\n                                <mml:mi>∞</mml:mi>\r\n                              </mml:mrow>\r\n                            </mml:munder>\r\n                            <mml:mfrac>\r\n                              <mml:mrow>\r\n                                <mml:msup>\r\n                                  <mml:mi>t</mml:mi>\r\n                                  <mml:mfrac>\r\n                                    <mml:mn>1</mml:mn>\r\n                                    <mml:mi>p</mml:mi>\r\n                                  </mml:mfrac>\r\n                                </mml:msup>\r\n                                <mml:msub>\r\n                                  <mml:mrow>\r\n                                    <mml:mo>‖</mml:mo>\r\n                                    <mml:mi>u</mml:mi>\r\n                                    <mml:mrow>\r\n                                      <mml:mo>(</mml:mo>\r\n                                      <mml:mo>·</mml:mo>\r\n                                      <mml:mo>,</mml:mo>\r\n                                      <mml:mi>t</mml:mi>\r\n                                      <mml:mo>)</mml:mo>\r\n                                    </mml:mrow>\r\n                                    <mml:mo>‖</mml:mo>\r\n                                  </mml:mrow>\r\n                                  <mml:mrow>\r\n                                    <mml:msup>\r\n                                      <mml:mi>L</mml:mi>\r\n                                      <mml:mi>∞</mml:mi>\r\n                                    </mml:msup>\r\n                                    <mml:mrow>\r\n                                      <mml:mo>(</mml:mo>\r\n                                      <mml:msup>\r\n                                        <mml:mrow>\r\n                                          <mml:mi>R</mml:mi>\r\n                                        </mml:mrow>\r\n                                        <mml:mi>n</mml:mi>\r\n                                      </mml:msup>\r\n                                      <mml:mo>)</mml:mo>\r\n                                    </mml:mrow>\r\n                                  </mml:mrow>\r\n                                </mml:msub>\r\n                              </mml:mrow>\r\n                              <mml:mrow>\r\n                                <mml:mi>f</mml:mi>\r\n                                <mml:mo>(</mml:mo>\r\n                                <mml:mi>t</mml:mi>\r\n                                <mml:mo>)</mml:mo>\r\n                              </mml:mrow>\r\n                            </mml:mfrac>\r\n                            <mml:mo>=</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>and <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\limsup _{t\\rightarrow \\infty } \\frac{\\Vert u(\\cdot ,t)\\Vert _{L^\\infty (\\mathbb {R}^n)}}{g(t)} =\\infty . \\end{aligned}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n                          <mml:mrow>\r\n                            <mml:munder>\r\n                              <mml:mo>lim sup</mml:mo>\r\n                              <mml:mrow>\r\n                                <mml:mi>t</mml:mi>\r\n                                <mml:mo>→</mml:mo>\r\n                                <mml:mi>∞</mml:mi>\r\n                              </mml:mrow>\r\n                            </mml:munder>\r\n                            <mml:mfrac>\r\n                              <mml:msub>\r\n                                <mml:mrow>\r\n                                  <mml:mo>‖</mml:mo>\r\n                                  <mml:mi>u</mml:mi>\r\n                                  <mml:mrow>\r\n                                    <mml:mo>(</mml:mo>\r\n                                    <mml:mo>·</mml:mo>\r\n                                    <mml:mo>,</mml:mo>\r\n                                    <mml:mi>t</mml:mi>\r\n                                    <mml:mo>)</mml:mo>\r\n                                  </mml:mrow>\r\n                                  <mml:mo>‖</mml:mo>\r\n                                </mml:mrow>\r\n                                <mml:mrow>\r\n                                  <mml:msup>\r\n                                    <mml:mi>L</mml:mi>\r\n                                    <mml:mi>∞</mml:mi>\r\n                                  </mml:msup>\r\n                                  <mml:mrow>\r\n                                    <mml:mo>(</mml:mo>\r\n                                    <mml:msup>\r\n                                      <mml:mrow>\r\n                                        <mml:mi>R</mml:mi>\r\n                                      </mml:mrow>\r\n                                      <mml:mi>n</mml:mi>\r\n                                    </mml:msup>\r\n                                    <mml:mo>)</mml:mo>\r\n                                  </mml:mrow>\r\n                                </mml:mrow>\r\n                              </mml:msub>\r\n                              <mml:mrow>\r\n                                <mml:mi>g</mml:mi>\r\n                                <mml:mo>(</mml:mo>\r\n                                <mml:mi>t</mml:mi>\r\n                                <mml:mo>)</mml:mo>\r\n                              </mml:mrow>\r\n                            </mml:mfrac>\r\n                            <mml:mo>=</mml:mo>\r\n                            <mml:mi>∞</mml:mi>\r\n                            <mml:mo>.</mml:mo>\r\n                          </mml:mrow>\r\n                        </mml:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula></jats:p>"}],"type":"journal_article","publication":"Partial Differential Equations and Applications","language":[{"iso":"eng"}],"article_number":"47","user_id":"31496","_id":"63311"},{"issue":"11","publication_status":"published","publication_identifier":{"issn":["1531-3492","1553-524X"]},"citation":{"ama":"Winkler M. Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities. <i>Discrete and Continuous Dynamical Systems - B</i>. 2022;27(11). doi:<a href=\"https://doi.org/10.3934/dcdsb.2022009\">10.3934/dcdsb.2022009</a>","ieee":"M. Winkler, “Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities,” <i>Discrete and Continuous Dynamical Systems - B</i>, vol. 27, no. 11, Art. no. 6565, 2022, doi: <a href=\"https://doi.org/10.3934/dcdsb.2022009\">10.3934/dcdsb.2022009</a>.","chicago":"Winkler, Michael. “Approaching Logarithmic Singularities in Quasilinear Chemotaxis-Consumption Systems with Signal-Dependent Sensitivities.” <i>Discrete and Continuous Dynamical Systems - B</i> 27, no. 11 (2022). <a href=\"https://doi.org/10.3934/dcdsb.2022009\">https://doi.org/10.3934/dcdsb.2022009</a>.","mla":"Winkler, Michael. “Approaching Logarithmic Singularities in Quasilinear Chemotaxis-Consumption Systems with Signal-Dependent Sensitivities.” <i>Discrete and Continuous Dynamical Systems - B</i>, vol. 27, no. 11, 6565, American Institute of Mathematical Sciences (AIMS), 2022, doi:<a href=\"https://doi.org/10.3934/dcdsb.2022009\">10.3934/dcdsb.2022009</a>.","short":"M. Winkler, Discrete and Continuous Dynamical Systems - B 27 (2022).","bibtex":"@article{Winkler_2022, title={Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities}, volume={27}, DOI={<a href=\"https://doi.org/10.3934/dcdsb.2022009\">10.3934/dcdsb.2022009</a>}, number={116565}, journal={Discrete and Continuous Dynamical Systems - B}, publisher={American Institute of Mathematical Sciences (AIMS)}, author={Winkler, Michael}, year={2022} }","apa":"Winkler, M. (2022). Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities. <i>Discrete and Continuous Dynamical Systems - B</i>, <i>27</i>(11), Article 6565. <a href=\"https://doi.org/10.3934/dcdsb.2022009\">https://doi.org/10.3934/dcdsb.2022009</a>"},"intvolume":"        27","year":"2022","author":[{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:30:32Z","volume":27,"publisher":"American Institute of Mathematical Sciences (AIMS)","date_updated":"2025-12-18T20:05:47Z","doi":"10.3934/dcdsb.2022009","title":"Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities","type":"journal_article","publication":"Discrete and Continuous Dynamical Systems - B","status":"public","abstract":[{"lang":"eng","text":"<jats:p xml:lang=\"fr\">&lt;p style='text-indent:20px;'&gt;The chemotaxis system&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE1\"&gt; \\begin{document}$ \\begin{array}{l}\\left\\{ \\begin{array}{l} \tu_t = \\nabla \\cdot \\big( D(u) \\nabla u \\big) - \\nabla \\cdot \\big( uS(x, u, v)\\cdot \\nabla v\\big), \\\\ \tv_t = \\Delta v -uv, \\end{array} \\right. \\end{array} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;is considered in a bounded domain &lt;inline-formula&gt;&lt;tex-math id=\"M1\"&gt;\\begin{document}$ \\Omega\\subset \\mathbb{R}^n $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, &lt;inline-formula&gt;&lt;tex-math id=\"M2\"&gt;\\begin{document}$ n\\ge 2 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, with smooth boundary.&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;It is shown that if &lt;inline-formula&gt;&lt;tex-math id=\"M3\"&gt;\\begin{document}$ D: [0, \\infty) \\to [0, \\infty) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; and &lt;inline-formula&gt;&lt;tex-math id=\"M4\"&gt;\\begin{document}$ S: \\overline{\\Omega}\\times [0, \\infty)\\times (0, \\infty)\\to \\mathbb{R}^{n\\times n} $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; are suitably smooth functions satisfying&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE2\"&gt; \\begin{document}$ \\begin{array}{l}D(u) \\ge k_D u^{m-1} \t\\qquad {\\rm{for\\; all}}\\; u\\ge 0 \\end{array} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;and&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE3\"&gt; \\begin{document}$ \\begin{array}{l}|S(x, u, v)| \\le \\frac{S_0(v)}{v^\\alpha} \\qquad {\\rm{for\\; all}}\\; (x, u, v)\\; \\in \\Omega\\times (0, \\infty)^2 \\end{array} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;with some&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE4\"&gt; \\begin{document}$ \\begin{array}{l}m&amp;gt;\\frac{3n-2}{2n} \t\\qquad {\\rm{and}}\\;\\alpha\\in [0, 1), \\end{array} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;and with some &lt;inline-formula&gt;&lt;tex-math id=\"M5\"&gt;\\begin{document}$ k_D&amp;gt;0 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; and nondecreasing &lt;inline-formula&gt;&lt;tex-math id=\"M6\"&gt;\\begin{document}$ S_0: (0, \\infty)\\to (0, \\infty) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, then for all suitably regular initial data a corresponding no-flux type initial-boundary value problem admits a global bounded weak solution which actually is smooth and classical if &lt;inline-formula&gt;&lt;tex-math id=\"M7\"&gt;\\begin{document}$ D(0)&amp;gt;0 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;.&lt;/p&gt;</jats:p>"}],"user_id":"31496","_id":"63312","language":[{"iso":"eng"}],"article_number":"6565"},{"issue":"9","publication_identifier":{"issn":["0025-584X","1522-2616"]},"publication_status":"published","intvolume":"       295","page":"1840-1862","citation":{"apa":"Winkler, M. (2022). A unifying approach toward boundedness in Keller–Segel type cross‐diffusion systems via conditional L∞$L^\\infty$ estimates for taxis gradients. <i>Mathematische Nachrichten</i>, <i>295</i>(9), 1840–1862. <a href=\"https://doi.org/10.1002/mana.202000403\">https://doi.org/10.1002/mana.202000403</a>","bibtex":"@article{Winkler_2022, title={A unifying approach toward boundedness in Keller–Segel type cross‐diffusion systems via conditional L∞$L^\\infty$ estimates for taxis gradients}, volume={295}, DOI={<a href=\"https://doi.org/10.1002/mana.202000403\">10.1002/mana.202000403</a>}, number={9}, journal={Mathematische Nachrichten}, publisher={Wiley}, author={Winkler, Michael}, year={2022}, pages={1840–1862} }","short":"M. Winkler, Mathematische Nachrichten 295 (2022) 1840–1862.","mla":"Winkler, Michael. “A Unifying Approach toward Boundedness in Keller–Segel Type Cross‐diffusion Systems via Conditional L∞$L^\\infty$ Estimates for Taxis Gradients.” <i>Mathematische Nachrichten</i>, vol. 295, no. 9, Wiley, 2022, pp. 1840–62, doi:<a href=\"https://doi.org/10.1002/mana.202000403\">10.1002/mana.202000403</a>.","chicago":"Winkler, Michael. “A Unifying Approach toward Boundedness in Keller–Segel Type Cross‐diffusion Systems via Conditional L∞$L^\\infty$ Estimates for Taxis Gradients.” <i>Mathematische Nachrichten</i> 295, no. 9 (2022): 1840–62. <a href=\"https://doi.org/10.1002/mana.202000403\">https://doi.org/10.1002/mana.202000403</a>.","ieee":"M. Winkler, “A unifying approach toward boundedness in Keller–Segel type cross‐diffusion systems via conditional L∞$L^\\infty$ estimates for taxis gradients,” <i>Mathematische Nachrichten</i>, vol. 295, no. 9, pp. 1840–1862, 2022, doi: <a href=\"https://doi.org/10.1002/mana.202000403\">10.1002/mana.202000403</a>.","ama":"Winkler M. A unifying approach toward boundedness in Keller–Segel type cross‐diffusion systems via conditional L∞$L^\\infty$ estimates for taxis gradients. <i>Mathematische Nachrichten</i>. 2022;295(9):1840-1862. doi:<a href=\"https://doi.org/10.1002/mana.202000403\">10.1002/mana.202000403</a>"},"year":"2022","volume":295,"date_created":"2025-12-18T19:28:46Z","author":[{"last_name":"Winkler","full_name":"Winkler, Michael","id":"31496","first_name":"Michael"}],"publisher":"Wiley","date_updated":"2025-12-18T20:05:19Z","doi":"10.1002/mana.202000403","title":"A unifying approach toward boundedness in Keller–Segel type cross‐diffusion systems via conditional L∞$L^\\infty$ estimates for taxis gradients","publication":"Mathematische Nachrichten","type":"journal_article","status":"public","abstract":[{"text":"<jats:title>Abstract</jats:title><jats:p>This manuscript is concerned with the problem of efficiently estimating chemotactic gradients, as forming a ubiquitous issue of key importance in virtually any proof of boundedness features in Keller–Segel type systems. A strategy is proposed which at its core relies on bounds for such quantities, conditional in the sense of involving certain Lebesgue norms of solution components that explicitly influence the signal evolution.</jats:p><jats:p>Applications of this procedure firstly provide apparently novel boundedness results for two particular classes chemotaxis systems, and apart from that are shown to significantly condense proofs for basically well‐known statements on boundedness in two further Keller–Segel type problems.</jats:p>","lang":"eng"}],"user_id":"31496","_id":"63309","language":[{"iso":"eng"}]},{"date_created":"2025-12-18T19:26:56Z","author":[{"first_name":"Michael","last_name":"Winkler","id":"31496","full_name":"Winkler, Michael"}],"volume":71,"date_updated":"2025-12-18T20:04:53Z","publisher":"Indiana University Mathematics Journal","doi":"10.1512/iumj.2022.71.9042","title":"A critical blow-up exponent for flux limiation in a Keller-Segel system","issue":"4","publication_status":"published","publication_identifier":{"issn":["0022-2518"]},"citation":{"bibtex":"@article{Winkler_2022, title={A critical blow-up exponent for flux limiation in a Keller-Segel system}, volume={71}, DOI={<a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">10.1512/iumj.2022.71.9042</a>}, number={4}, journal={Indiana University Mathematics Journal}, publisher={Indiana University Mathematics Journal}, author={Winkler, Michael}, year={2022}, pages={1437–1465} }","mla":"Winkler, Michael. “A Critical Blow-up Exponent for Flux Limiation in a Keller-Segel System.” <i>Indiana University Mathematics Journal</i>, vol. 71, no. 4, Indiana University Mathematics Journal, 2022, pp. 1437–65, doi:<a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">10.1512/iumj.2022.71.9042</a>.","short":"M. Winkler, Indiana University Mathematics Journal 71 (2022) 1437–1465.","apa":"Winkler, M. (2022). A critical blow-up exponent for flux limiation in a Keller-Segel system. <i>Indiana University Mathematics Journal</i>, <i>71</i>(4), 1437–1465. <a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">https://doi.org/10.1512/iumj.2022.71.9042</a>","chicago":"Winkler, Michael. “A Critical Blow-up Exponent for Flux Limiation in a Keller-Segel System.” <i>Indiana University Mathematics Journal</i> 71, no. 4 (2022): 1437–65. <a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">https://doi.org/10.1512/iumj.2022.71.9042</a>.","ieee":"M. Winkler, “A critical blow-up exponent for flux limiation in a Keller-Segel system,” <i>Indiana University Mathematics Journal</i>, vol. 71, no. 4, pp. 1437–1465, 2022, doi: <a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">10.1512/iumj.2022.71.9042</a>.","ama":"Winkler M. A critical blow-up exponent for flux limiation in a Keller-Segel system. <i>Indiana University Mathematics Journal</i>. 2022;71(4):1437-1465. doi:<a href=\"https://doi.org/10.1512/iumj.2022.71.9042\">10.1512/iumj.2022.71.9042</a>"},"intvolume":"        71","page":"1437-1465","year":"2022","user_id":"31496","_id":"63306","language":[{"iso":"eng"}],"type":"journal_article","publication":"Indiana University Mathematics Journal","status":"public"},{"publication_identifier":{"issn":["1664-3607","1664-3615"]},"publication_status":"published","issue":"02","year":"2022","intvolume":"        13","citation":{"chicago":"Winkler, Michael. “Application of the Moser–Trudinger Inequality in the Construction of Global Solutions to a Strongly Degenerate Migration Model.” <i>Bulletin of Mathematical Sciences</i> 13, no. 02 (2022). <a href=\"https://doi.org/10.1142/s1664360722500126\">https://doi.org/10.1142/s1664360722500126</a>.","ieee":"M. Winkler, “Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model,” <i>Bulletin of Mathematical Sciences</i>, vol. 13, no. 02, Art. no. 2250012, 2022, doi: <a href=\"https://doi.org/10.1142/s1664360722500126\">10.1142/s1664360722500126</a>.","ama":"Winkler M. Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model. <i>Bulletin of Mathematical Sciences</i>. 2022;13(02). doi:<a href=\"https://doi.org/10.1142/s1664360722500126\">10.1142/s1664360722500126</a>","short":"M. Winkler, Bulletin of Mathematical Sciences 13 (2022).","mla":"Winkler, Michael. “Application of the Moser–Trudinger Inequality in the Construction of Global Solutions to a Strongly Degenerate Migration Model.” <i>Bulletin of Mathematical Sciences</i>, vol. 13, no. 02, 2250012, World Scientific Pub Co Pte Ltd, 2022, doi:<a href=\"https://doi.org/10.1142/s1664360722500126\">10.1142/s1664360722500126</a>.","bibtex":"@article{Winkler_2022, title={Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model}, volume={13}, DOI={<a href=\"https://doi.org/10.1142/s1664360722500126\">10.1142/s1664360722500126</a>}, number={022250012}, journal={Bulletin of Mathematical Sciences}, publisher={World Scientific Pub Co Pte Ltd}, author={Winkler, Michael}, year={2022} }","apa":"Winkler, M. (2022). Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model. <i>Bulletin of Mathematical Sciences</i>, <i>13</i>(02), Article 2250012. <a href=\"https://doi.org/10.1142/s1664360722500126\">https://doi.org/10.1142/s1664360722500126</a>"},"date_updated":"2025-12-18T20:07:05Z","publisher":"World Scientific Pub Co Pte Ltd","volume":13,"author":[{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:18:11Z","title":"Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model","doi":"10.1142/s1664360722500126","publication":"Bulletin of Mathematical Sciences","type":"journal_article","abstract":[{"lang":"eng","text":"<jats:p> A no-flux initial-boundary value problem for the cross-diffusion system [Formula: see text] is considered in smoothly bounded domains [Formula: see text] with [Formula: see text]. It is shown that whenever [Formula: see text] is positive on [Formula: see text] and such that [Formula: see text] for some [Formula: see text], for all suitably regular positive initial data a global very weak solution, particularly preserving mass in its first component, can be constructed. This extends previous results which either concentrate on non-degenerate analogs, or are restricted to the special case [Formula: see text]. </jats:p><jats:p> To appropriately cope with the considerably stronger cross-degeneracies thus allowed through [Formula: see text] when [Formula: see text] is large, in its core part the analysis relies on the use of the Moser–Trudinger inequality in controlling the respective diffusion rates [Formula: see text] from below. </jats:p>"}],"status":"public","_id":"63284","user_id":"31496","article_number":"2250012","language":[{"iso":"eng"}]},{"year":"2022","citation":{"chicago":"Winkler, Michael. “Exponential Grow-up Rates in a Quasilinear Keller–Segel System.” <i>Asymptotic Analysis</i> 131, no. 1 (2022): 33–57. <a href=\"https://doi.org/10.3233/asy-221765\">https://doi.org/10.3233/asy-221765</a>.","ieee":"M. Winkler, “Exponential grow-up rates in a quasilinear Keller–Segel system,” <i>Asymptotic Analysis</i>, vol. 131, no. 1, pp. 33–57, 2022, doi: <a href=\"https://doi.org/10.3233/asy-221765\">10.3233/asy-221765</a>.","ama":"Winkler M. Exponential grow-up rates in a quasilinear Keller–Segel system. <i>Asymptotic Analysis</i>. 2022;131(1):33-57. doi:<a href=\"https://doi.org/10.3233/asy-221765\">10.3233/asy-221765</a>","apa":"Winkler, M. (2022). Exponential grow-up rates in a quasilinear Keller–Segel system. <i>Asymptotic Analysis</i>, <i>131</i>(1), 33–57. <a href=\"https://doi.org/10.3233/asy-221765\">https://doi.org/10.3233/asy-221765</a>","mla":"Winkler, Michael. “Exponential Grow-up Rates in a Quasilinear Keller–Segel System.” <i>Asymptotic Analysis</i>, vol. 131, no. 1, SAGE Publications, 2022, pp. 33–57, doi:<a href=\"https://doi.org/10.3233/asy-221765\">10.3233/asy-221765</a>.","bibtex":"@article{Winkler_2022, title={Exponential grow-up rates in a quasilinear Keller–Segel system}, volume={131}, DOI={<a href=\"https://doi.org/10.3233/asy-221765\">10.3233/asy-221765</a>}, number={1}, journal={Asymptotic Analysis}, publisher={SAGE Publications}, author={Winkler, Michael}, year={2022}, pages={33–57} }","short":"M. Winkler, Asymptotic Analysis 131 (2022) 33–57."},"intvolume":"       131","page":"33-57","publication_status":"published","publication_identifier":{"issn":["0921-7134","1875-8576"]},"issue":"1","title":"Exponential grow-up rates in a quasilinear Keller–Segel system","doi":"10.3233/asy-221765","date_updated":"2025-12-18T20:07:19Z","publisher":"SAGE Publications","author":[{"first_name":"Michael","last_name":"Winkler","full_name":"Winkler, Michael","id":"31496"}],"date_created":"2025-12-18T19:18:51Z","volume":131,"abstract":[{"lang":"eng","text":"<jats:p> The chemotaxis system [Formula: see text] is considered in a ball [Formula: see text]. </jats:p><jats:p> It is shown that if [Formula: see text] suitably generalizes the prototype given by [Formula: see text] with some [Formula: see text], and if diffusion is suitably weak in the sense that [Formula: see text] is such that there exist [Formula: see text] and [Formula: see text] fulfilling [Formula: see text] then for appropriate choices of sufficiently concentrated initial data, an associated no-flux initial-boundary value problem admits a global classical solution [Formula: see text] which blows up in infinite time and satisfies [Formula: see text] A major part of the proof is based on a comparison argument involving explicitly constructed subsolutions to a scalar parabolic problem satisfied by mass accumulation functions corresponding to solutions of ( ⋆ ). </jats:p>"}],"status":"public","type":"journal_article","publication":"Asymptotic Analysis","language":[{"iso":"eng"}],"_id":"63286","user_id":"31496"},{"year":"2022","citation":{"apa":"Kang, K., Lee, J., &#38; Winkler, M. (2022). Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $. <i>Discrete and Continuous Dynamical Systems</i>, <i>42</i>(11), Article 5201. <a href=\"https://doi.org/10.3934/dcds.2022091\">https://doi.org/10.3934/dcds.2022091</a>","mla":"Kang, Kyungkeun, et al. “Global Weak Solutions to a Chemotaxis-Navier-Stokes System in $  \\mathbb{R}^3 $.” <i>Discrete and Continuous Dynamical Systems</i>, vol. 42, no. 11, 5201, American Institute of Mathematical Sciences (AIMS), 2022, doi:<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>.","bibtex":"@article{Kang_Lee_Winkler_2022, title={Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $}, volume={42}, DOI={<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>}, number={115201}, journal={Discrete and Continuous Dynamical Systems}, publisher={American Institute of Mathematical Sciences (AIMS)}, author={Kang, Kyungkeun and Lee, Jihoon and Winkler, Michael}, year={2022} }","short":"K. Kang, J. Lee, M. Winkler, Discrete and Continuous Dynamical Systems 42 (2022).","ama":"Kang K, Lee J, Winkler M. Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $. <i>Discrete and Continuous Dynamical Systems</i>. 2022;42(11). doi:<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>","ieee":"K. Kang, J. Lee, and M. Winkler, “Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $,” <i>Discrete and Continuous Dynamical Systems</i>, vol. 42, no. 11, Art. no. 5201, 2022, doi: <a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>.","chicago":"Kang, Kyungkeun, Jihoon Lee, and Michael Winkler. “Global Weak Solutions to a Chemotaxis-Navier-Stokes System in $  \\mathbb{R}^3 $.” <i>Discrete and Continuous Dynamical Systems</i> 42, no. 11 (2022). <a href=\"https://doi.org/10.3934/dcds.2022091\">https://doi.org/10.3934/dcds.2022091</a>."},"intvolume":"        42","publication_status":"published","publication_identifier":{"issn":["1078-0947","1553-5231"]},"issue":"11","title":"Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $","doi":"10.3934/dcds.2022091","date_updated":"2025-12-18T20:08:21Z","publisher":"American Institute of Mathematical Sciences (AIMS)","date_created":"2025-12-18T19:22:04Z","author":[{"first_name":"Kyungkeun","last_name":"Kang","full_name":"Kang, Kyungkeun"},{"first_name":"Jihoon","last_name":"Lee","full_name":"Lee, Jihoon"},{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"volume":42,"abstract":[{"text":"<jats:p xml:lang=\"fr\">&lt;p style='text-indent:20px;'&gt;The Cauchy problem in &lt;inline-formula&gt;&lt;tex-math id=\"M2\"&gt;\\begin{document}$  \\mathbb{R}^3 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; for the chemotaxis-Navier–Stokes system&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE1\"&gt; \\begin{document}$ \\begin{eqnarray*} \\left\\{ \\begin{array}{l}      n_t + u\\cdot\\nabla n = \\Delta n - \\nabla \\cdot (n\\nabla c), \\\\\tc_t + u\\cdot\\nabla c = \\Delta c - nc, \\\\ \tu_t + (u\\cdot\\nabla) u = \\Delta u + \\nabla P + n\\nabla\\phi, \\qquad \\nabla \\cdot u = 0, \\ \t\\end{array} \\right. \\end{eqnarray*} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;is considered. Under suitable conditions on the initial data &lt;inline-formula&gt;&lt;tex-math id=\"M3\"&gt;\\begin{document}$ (n_0, c_0, u_0) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, with regard to the crucial first component requiring that &lt;inline-formula&gt;&lt;tex-math id=\"M4\"&gt;\\begin{document}$ n_0\\in L^1( \\mathbb{R}^3) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; be nonnegative and such that &lt;inline-formula&gt;&lt;tex-math id=\"M5\"&gt;\\begin{document}$ (n_0+1)\\ln (n_0+1) \\in L^1( \\mathbb{R}^3) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, a globally defined weak solution with &lt;inline-formula&gt;&lt;tex-math id=\"M6\"&gt;\\begin{document}$ (n, c, u)|_{t = 0} = (n_0, c_0, u_0) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; is constructed. Apart from that, assuming that moreover &lt;inline-formula&gt;&lt;tex-math id=\"M7\"&gt;\\begin{document}$ \\int_{ \\mathbb{R}^3} n_0(x) \\ln (1+|x|^2) dx $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; is finite, it is shown that a weak solution exists which enjoys further regularity features and preserves mass in an appropriate sense.&lt;/p&gt;</jats:p>","lang":"eng"}],"status":"public","type":"journal_article","publication":"Discrete and Continuous Dynamical Systems","article_number":"5201","language":[{"iso":"eng"}],"_id":"63293","user_id":"31496"}]
