[{"title":"Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions","date_created":"2025-12-18T17:21:21Z","publisher":"American Chemical Society (ACS)","year":"2022","issue":"28","quality_controlled":"1","language":[{"iso":"eng"}],"publication":"Analytical Chemistry","doi":"10.1021/acs.analchem.2c01763","volume":94,"author":[{"last_name":"Leppin","full_name":"Leppin, Christian","id":"117722","first_name":"Christian"},{"last_name":"Langhoff","full_name":"Langhoff, Arne","first_name":"Arne"},{"first_name":"Diethelm","last_name":"Johannsmann","full_name":"Johannsmann, Diethelm"}],"date_updated":"2025-12-18T17:38:07Z","page":"10227-10233","intvolume":"        94","citation":{"ama":"Leppin C, Langhoff A, Johannsmann D. Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions. <i>Analytical Chemistry</i>. 2022;94(28):10227-10233. doi:<a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">10.1021/acs.analchem.2c01763</a>","chicago":"Leppin, Christian, Arne Langhoff, and Diethelm Johannsmann. “Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions.” <i>Analytical Chemistry</i> 94, no. 28 (2022): 10227–33. <a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">https://doi.org/10.1021/acs.analchem.2c01763</a>.","ieee":"C. Leppin, A. Langhoff, and D. Johannsmann, “Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions,” <i>Analytical Chemistry</i>, vol. 94, no. 28, pp. 10227–10233, 2022, doi: <a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">10.1021/acs.analchem.2c01763</a>.","apa":"Leppin, C., Langhoff, A., &#38; Johannsmann, D. (2022). Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions. <i>Analytical Chemistry</i>, <i>94</i>(28), 10227–10233. <a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">https://doi.org/10.1021/acs.analchem.2c01763</a>","mla":"Leppin, Christian, et al. “Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions.” <i>Analytical Chemistry</i>, vol. 94, no. 28, American Chemical Society (ACS), 2022, pp. 10227–33, doi:<a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">10.1021/acs.analchem.2c01763</a>.","bibtex":"@article{Leppin_Langhoff_Johannsmann_2022, title={Square-Wave Electrogravimetry Combined with Voltammetry Reveals Reversible Submonolayer Adsorption of Redox-Active Ions}, volume={94}, DOI={<a href=\"https://doi.org/10.1021/acs.analchem.2c01763\">10.1021/acs.analchem.2c01763</a>}, number={28}, journal={Analytical Chemistry}, publisher={American Chemical Society (ACS)}, author={Leppin, Christian and Langhoff, Arne and Johannsmann, Diethelm}, year={2022}, pages={10227–10233} }","short":"C. Leppin, A. Langhoff, D. Johannsmann, Analytical Chemistry 94 (2022) 10227–10233."},"publication_identifier":{"issn":["0003-2700","1520-6882"]},"publication_status":"published","extern":"1","user_id":"117722","_id":"63233","status":"public","type":"journal_article"},{"publication_status":"published","publication_identifier":{"issn":["2169-0375"]},"issue":"1","year":"2022","citation":{"short":"M. Winkler, Advanced Nonlinear Studies 22 (2022) 88–117.","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} }","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>.","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>","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>","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>."},"intvolume":"        22","page":"88-117","publisher":"Walter de Gruyter GmbH","date_updated":"2025-12-18T20:05:30Z","author":[{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:29:40Z","volume":22,"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","type":"journal_article","publication":"Advanced Nonlinear Studies","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","_id":"63310","user_id":"31496","language":[{"iso":"eng"}]},{"language":[{"iso":"eng"}],"article_number":"108","user_id":"31496","_id":"63305","status":"public","abstract":[{"lang":"eng","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>"}],"publication":"Calculus of Variations and Partial Differential Equations","type":"journal_article","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","volume":61,"author":[{"last_name":"Winkler","id":"31496","full_name":"Winkler, Michael","first_name":"Michael"}],"date_created":"2025-12-18T19:26:32Z","date_updated":"2025-12-18T20:04:43Z","publisher":"Springer Science and Business Media LLC","intvolume":"        61","citation":{"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>","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>.","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>.","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).","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>"},"year":"2022","issue":"3","publication_identifier":{"issn":["0944-2669","1432-0835"]},"publication_status":"published"},{"_id":"63311","user_id":"31496","article_number":"47","language":[{"iso":"eng"}],"publication":"Partial Differential Equations and Applications","type":"journal_article","abstract":[{"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>","lang":"eng"}],"status":"public","date_updated":"2025-12-18T20:05:38Z","publisher":"Springer Science and Business Media LLC","volume":3,"date_created":"2025-12-18T19:30:04Z","author":[{"first_name":"Michael","id":"31496","full_name":"Winkler, Michael","last_name":"Winkler"}],"title":"Oscillatory decay in a degenerate parabolic equation","doi":"10.1007/s42985-022-00186-z","publication_identifier":{"issn":["2662-2963","2662-2971"]},"publication_status":"published","issue":"4","year":"2022","intvolume":"         3","citation":{"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>","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>.","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>","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>.","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} }"}},{"volume":27,"date_created":"2025-12-18T19:30:32Z","author":[{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"date_updated":"2025-12-18T20:05:47Z","publisher":"American Institute of Mathematical Sciences (AIMS)","doi":"10.3934/dcdsb.2022009","title":"Approaching logarithmic singularities in quasilinear chemotaxis-consumption systems with signal-dependent sensitivities","issue":"11","publication_identifier":{"issn":["1531-3492","1553-524X"]},"publication_status":"published","intvolume":"        27","citation":{"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>","short":"M. Winkler, Discrete and Continuous Dynamical Systems - B 27 (2022).","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>.","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} }","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>.","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>.","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>"},"year":"2022","user_id":"31496","_id":"63312","language":[{"iso":"eng"}],"article_number":"6565","publication":"Discrete and Continuous Dynamical Systems - B","type":"journal_article","status":"public","abstract":[{"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 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;.&lt;/p&gt;</jats:p>","lang":"eng"}]},{"publication":"Mathematische Nachrichten","type":"journal_article","status":"public","abstract":[{"text":"<jats:title>Abstract</jats:title><jats:p>This manuscript is concerned with the problem of efficiently estimating chemotactic gradients, as forming a ubiquitous issue of key importance in virtually any proof of boundedness features in Keller–Segel type systems. A strategy is proposed which at its core relies on bounds for such quantities, conditional in the sense of involving certain Lebesgue norms of solution components that explicitly influence the signal evolution.</jats:p><jats:p>Applications of this procedure firstly provide apparently novel boundedness results for two particular classes chemotaxis systems, and apart from that are shown to significantly condense proofs for basically well‐known statements on boundedness in two further Keller–Segel type problems.</jats:p>","lang":"eng"}],"user_id":"31496","_id":"63309","language":[{"iso":"eng"}],"issue":"9","publication_identifier":{"issn":["0025-584X","1522-2616"]},"publication_status":"published","page":"1840-1862","intvolume":"       295","citation":{"short":"M. Winkler, Mathematische Nachrichten 295 (2022) 1840–1862.","mla":"Winkler, Michael. “A Unifying Approach toward Boundedness in Keller–Segel Type Cross‐diffusion Systems via Conditional L∞$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>.","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} }","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>","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":[{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","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"},{"status":"public","type":"journal_article","publication":"Indiana University Mathematics Journal","language":[{"iso":"eng"}],"user_id":"31496","_id":"63306","citation":{"short":"M. Winkler, Indiana University Mathematics Journal 71 (2022) 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>.","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} }","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>","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>","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>.","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>."},"intvolume":"        71","page":"1437-1465","year":"2022","issue":"4","publication_status":"published","publication_identifier":{"issn":["0022-2518"]},"doi":"10.1512/iumj.2022.71.9042","title":"A critical blow-up exponent for flux limiation in a Keller-Segel system","date_created":"2025-12-18T19:26:56Z","author":[{"first_name":"Michael","id":"31496","full_name":"Winkler, Michael","last_name":"Winkler"}],"volume":71,"publisher":"Indiana University Mathematics Journal","date_updated":"2025-12-18T20:04:53Z"},{"volume":13,"author":[{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:18:11Z","date_updated":"2025-12-18T20:07:05Z","publisher":"World Scientific Pub Co Pte Ltd","doi":"10.1142/s1664360722500126","title":"Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model","issue":"02","publication_identifier":{"issn":["1664-3607","1664-3615"]},"publication_status":"published","intvolume":"        13","citation":{"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>.","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>.","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>","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>","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} }","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>."},"year":"2022","user_id":"31496","_id":"63284","language":[{"iso":"eng"}],"article_number":"2250012","publication":"Bulletin of Mathematical Sciences","type":"journal_article","status":"public","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>"}]},{"year":"2022","intvolume":"       131","page":"33-57","citation":{"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>","short":"M. Winkler, Asymptotic Analysis 131 (2022) 33–57.","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} }","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>","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>."},"publication_identifier":{"issn":["0921-7134","1875-8576"]},"publication_status":"published","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","volume":131,"date_created":"2025-12-18T19:18:51Z","author":[{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"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","publication":"Asymptotic Analysis","type":"journal_article","language":[{"iso":"eng"}],"_id":"63286","user_id":"31496"},{"type":"journal_article","publication":"Discrete and Continuous Dynamical Systems","abstract":[{"lang":"eng","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>"}],"status":"public","_id":"63293","user_id":"31496","article_number":"5201","language":[{"iso":"eng"}],"publication_status":"published","publication_identifier":{"issn":["1078-0947","1553-5231"]},"issue":"11","year":"2022","citation":{"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).","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>.","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>","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","publisher":"American Institute of Mathematical Sciences (AIMS)","date_updated":"2025-12-18T20:08:21Z","author":[{"full_name":"Kang, Kyungkeun","last_name":"Kang","first_name":"Kyungkeun"},{"first_name":"Jihoon","full_name":"Lee, Jihoon","last_name":"Lee"},{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"date_created":"2025-12-18T19:22:04Z","volume":42,"title":"Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $","doi":"10.3934/dcds.2022091"},{"date_created":"2025-12-18T19:20:25Z","author":[{"last_name":"Bellomo","full_name":"Bellomo, N.","first_name":"N."},{"first_name":"N.","full_name":"Outada, N.","last_name":"Outada"},{"full_name":"Soler, J.","last_name":"Soler","first_name":"J."},{"full_name":"Tao, Y.","last_name":"Tao","first_name":"Y."},{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"volume":32,"date_updated":"2025-12-18T20:07:51Z","publisher":"World Scientific Pub Co Pte Ltd","doi":"10.1142/s0218202522500166","title":"Chemotaxis and cross-diffusion models in complex environments: Models and analytic problems toward a multiscale vision","issue":"04","publication_status":"published","publication_identifier":{"issn":["0218-2025","1793-6314"]},"citation":{"apa":"Bellomo, N., Outada, N., Soler, J., Tao, Y., &#38; Winkler, M. (2022). Chemotaxis and cross-diffusion models in complex environments: Models and analytic problems toward a multiscale vision. <i>Mathematical Models and Methods in Applied Sciences</i>, <i>32</i>(04), 713–792. <a href=\"https://doi.org/10.1142/s0218202522500166\">https://doi.org/10.1142/s0218202522500166</a>","bibtex":"@article{Bellomo_Outada_Soler_Tao_Winkler_2022, title={Chemotaxis and cross-diffusion models in complex environments: Models and analytic problems toward a multiscale vision}, volume={32}, DOI={<a href=\"https://doi.org/10.1142/s0218202522500166\">10.1142/s0218202522500166</a>}, number={04}, journal={Mathematical Models and Methods in Applied Sciences}, publisher={World Scientific Pub Co Pte Ltd}, author={Bellomo, N. and Outada, N. and Soler, J. and Tao, Y. and Winkler, Michael}, year={2022}, pages={713–792} }","short":"N. Bellomo, N. Outada, J. Soler, Y. Tao, M. Winkler, Mathematical Models and Methods in Applied Sciences 32 (2022) 713–792.","mla":"Bellomo, N., et al. “Chemotaxis and Cross-Diffusion Models in Complex Environments: Models and Analytic Problems toward a Multiscale Vision.” <i>Mathematical Models and Methods in Applied Sciences</i>, vol. 32, no. 04, World Scientific Pub Co Pte Ltd, 2022, pp. 713–92, doi:<a href=\"https://doi.org/10.1142/s0218202522500166\">10.1142/s0218202522500166</a>.","ama":"Bellomo N, Outada N, Soler J, Tao Y, Winkler M. Chemotaxis and cross-diffusion models in complex environments: Models and analytic problems toward a multiscale vision. <i>Mathematical Models and Methods in Applied Sciences</i>. 2022;32(04):713-792. doi:<a href=\"https://doi.org/10.1142/s0218202522500166\">10.1142/s0218202522500166</a>","chicago":"Bellomo, N., N. Outada, J. Soler, Y. Tao, and Michael Winkler. “Chemotaxis and Cross-Diffusion Models in Complex Environments: Models and Analytic Problems toward a Multiscale Vision.” <i>Mathematical Models and Methods in Applied Sciences</i> 32, no. 04 (2022): 713–92. <a href=\"https://doi.org/10.1142/s0218202522500166\">https://doi.org/10.1142/s0218202522500166</a>.","ieee":"N. Bellomo, N. Outada, J. Soler, Y. Tao, and M. Winkler, “Chemotaxis and cross-diffusion models in complex environments: Models and analytic problems toward a multiscale vision,” <i>Mathematical Models and Methods in Applied Sciences</i>, vol. 32, no. 04, pp. 713–792, 2022, doi: <a href=\"https://doi.org/10.1142/s0218202522500166\">10.1142/s0218202522500166</a>."},"page":"713-792","intvolume":"        32","year":"2022","user_id":"31496","_id":"63290","language":[{"iso":"eng"}],"type":"journal_article","publication":"Mathematical Models and Methods in Applied Sciences","status":"public","abstract":[{"lang":"eng","text":"<jats:p> This paper proposes a review focused on exotic chemotaxis and cross-diffusion models in complex environments. The term exotic is used to denote the dynamics of models interacting with a time-evolving external system and, specifically, models derived with the aim of describing the dynamics of living systems. The presentation first, considers the derivation of phenomenological models of chemotaxis and cross-diffusion models with particular attention on nonlinear characteristics. Then, a variety of exotic models is presented with some hints toward the derivation of new models, by accounting for a critical analysis looking ahead to perspectives. The second part of the paper is devoted to a survey of analytical problems concerning the application of models to the study of real world dynamics. Finally, the focus shifts to research perspectives within the framework of a multiscale vision, where different paths are examined to move from the dynamics at the microscopic scale to collective behaviors at the macroscopic scale. </jats:p>"}]},{"year":"2022","intvolume":"        22","citation":{"short":"J. Lankeit, M. Winkler, Journal of Evolution Equations 22 (2022).","mla":"Lankeit, Johannes, and Michael Winkler. “Global Existence in Reaction–Diffusion Systems with Mass Control under Relaxed Assumptions Merely Referring to Cross-Absorptive Effects.” <i>Journal of Evolution Equations</i>, vol. 22, no. 1, 14, Springer Science and Business Media LLC, 2022, doi:<a href=\"https://doi.org/10.1007/s00028-022-00768-9\">10.1007/s00028-022-00768-9</a>.","bibtex":"@article{Lankeit_Winkler_2022, title={Global existence in reaction–diffusion systems with mass control under relaxed assumptions merely referring to cross-absorptive effects}, volume={22}, DOI={<a href=\"https://doi.org/10.1007/s00028-022-00768-9\">10.1007/s00028-022-00768-9</a>}, number={114}, journal={Journal of Evolution Equations}, publisher={Springer Science and Business Media LLC}, author={Lankeit, Johannes and Winkler, Michael}, year={2022} }","apa":"Lankeit, J., &#38; Winkler, M. (2022). Global existence in reaction–diffusion systems with mass control under relaxed assumptions merely referring to cross-absorptive effects. <i>Journal of Evolution Equations</i>, <i>22</i>(1), Article 14. <a href=\"https://doi.org/10.1007/s00028-022-00768-9\">https://doi.org/10.1007/s00028-022-00768-9</a>","ama":"Lankeit J, Winkler M. Global existence in reaction–diffusion systems with mass control under relaxed assumptions merely referring to cross-absorptive effects. <i>Journal of Evolution Equations</i>. 2022;22(1). doi:<a href=\"https://doi.org/10.1007/s00028-022-00768-9\">10.1007/s00028-022-00768-9</a>","ieee":"J. Lankeit and M. Winkler, “Global existence in reaction–diffusion systems with mass control under relaxed assumptions merely referring to cross-absorptive effects,” <i>Journal of Evolution Equations</i>, vol. 22, no. 1, Art. no. 14, 2022, doi: <a href=\"https://doi.org/10.1007/s00028-022-00768-9\">10.1007/s00028-022-00768-9</a>.","chicago":"Lankeit, Johannes, and Michael Winkler. “Global Existence in Reaction–Diffusion Systems with Mass Control under Relaxed Assumptions Merely Referring to Cross-Absorptive Effects.” <i>Journal of Evolution Equations</i> 22, no. 1 (2022). <a href=\"https://doi.org/10.1007/s00028-022-00768-9\">https://doi.org/10.1007/s00028-022-00768-9</a>."},"publication_identifier":{"issn":["1424-3199","1424-3202"]},"publication_status":"published","issue":"1","title":"Global existence in reaction–diffusion systems with mass control under relaxed assumptions merely referring to cross-absorptive effects","doi":"10.1007/s00028-022-00768-9","publisher":"Springer Science and Business Media LLC","date_updated":"2025-12-18T20:08:35Z","volume":22,"author":[{"first_name":"Johannes","full_name":"Lankeit, Johannes","last_name":"Lankeit"},{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:22:46Z","abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title><jats:p>We introduce a generalized concept of solutions for reaction–diffusion systems and prove their global existence. The only restriction on the reaction function beyond regularity, quasipositivity and mass control is special in that it merely controls the growth of cross-absorptive terms. The result covers nonlinear diffusion and does not rely on an entropy estimate.</jats:p>"}],"status":"public","publication":"Journal of Evolution Equations","type":"journal_article","article_number":"14","language":[{"iso":"eng"}],"_id":"63295","user_id":"31496"},{"date_updated":"2025-12-18T20:09:05Z","publisher":"Society for Industrial & Applied Mathematics (SIAM)","volume":54,"author":[{"first_name":"Youshan","full_name":"Tao, Youshan","last_name":"Tao"},{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"date_created":"2025-12-18T19:24:16Z","title":"Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System","doi":"10.1137/21m1449841","publication_identifier":{"issn":["0036-1410","1095-7154"]},"publication_status":"published","issue":"4","year":"2022","page":"4806-4864","intvolume":"        54","citation":{"apa":"Tao, Y., &#38; Winkler, M. (2022). Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System. <i>SIAM Journal on Mathematical Analysis</i>, <i>54</i>(4), 4806–4864. <a href=\"https://doi.org/10.1137/21m1449841\">https://doi.org/10.1137/21m1449841</a>","mla":"Tao, Youshan, and Michael Winkler. “Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System.” <i>SIAM Journal on Mathematical Analysis</i>, vol. 54, no. 4, Society for Industrial &#38; Applied Mathematics (SIAM), 2022, pp. 4806–64, doi:<a href=\"https://doi.org/10.1137/21m1449841\">10.1137/21m1449841</a>.","short":"Y. Tao, M. Winkler, SIAM Journal on Mathematical Analysis 54 (2022) 4806–4864.","bibtex":"@article{Tao_Winkler_2022, title={Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System}, volume={54}, DOI={<a href=\"https://doi.org/10.1137/21m1449841\">10.1137/21m1449841</a>}, number={4}, journal={SIAM Journal on Mathematical Analysis}, publisher={Society for Industrial &#38; Applied Mathematics (SIAM)}, author={Tao, Youshan and Winkler, Michael}, year={2022}, pages={4806–4864} }","chicago":"Tao, Youshan, and Michael Winkler. “Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System.” <i>SIAM Journal on Mathematical Analysis</i> 54, no. 4 (2022): 4806–64. <a href=\"https://doi.org/10.1137/21m1449841\">https://doi.org/10.1137/21m1449841</a>.","ieee":"Y. Tao and M. Winkler, “Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System,” <i>SIAM Journal on Mathematical Analysis</i>, vol. 54, no. 4, pp. 4806–4864, 2022, doi: <a href=\"https://doi.org/10.1137/21m1449841\">10.1137/21m1449841</a>.","ama":"Tao Y, Winkler M. Existence Theory and Qualitative Analysis for a Fully Cross-Diffusive Predator-Prey System. <i>SIAM Journal on Mathematical Analysis</i>. 2022;54(4):4806-4864. doi:<a href=\"https://doi.org/10.1137/21m1449841\">10.1137/21m1449841</a>"},"_id":"63299","user_id":"31496","language":[{"iso":"eng"}],"publication":"SIAM Journal on Mathematical Analysis","type":"journal_article","status":"public"},{"title":"Taxis-driven persistent localization in a degenerate Keller-Segel system","doi":"10.1080/03605302.2022.2122836","date_updated":"2025-12-18T20:08:58Z","publisher":"Informa UK Limited","volume":47,"date_created":"2025-12-18T19:23:52Z","author":[{"first_name":"Angela","full_name":"Stevens, Angela","last_name":"Stevens"},{"first_name":"Michael","last_name":"Winkler","id":"31496","full_name":"Winkler, Michael"}],"year":"2022","page":"2341-2362","intvolume":"        47","citation":{"mla":"Stevens, Angela, and Michael Winkler. “Taxis-Driven Persistent Localization in a Degenerate Keller-Segel System.” <i>Communications in Partial Differential Equations</i>, vol. 47, no. 12, Informa UK Limited, 2022, pp. 2341–62, doi:<a href=\"https://doi.org/10.1080/03605302.2022.2122836\">10.1080/03605302.2022.2122836</a>.","short":"A. Stevens, M. Winkler, Communications in Partial Differential Equations 47 (2022) 2341–2362.","bibtex":"@article{Stevens_Winkler_2022, title={Taxis-driven persistent localization in a degenerate Keller-Segel system}, volume={47}, DOI={<a href=\"https://doi.org/10.1080/03605302.2022.2122836\">10.1080/03605302.2022.2122836</a>}, number={12}, journal={Communications in Partial Differential Equations}, publisher={Informa UK Limited}, author={Stevens, Angela and Winkler, Michael}, year={2022}, pages={2341–2362} }","apa":"Stevens, A., &#38; Winkler, M. (2022). Taxis-driven persistent localization in a degenerate Keller-Segel system. <i>Communications in Partial Differential Equations</i>, <i>47</i>(12), 2341–2362. <a href=\"https://doi.org/10.1080/03605302.2022.2122836\">https://doi.org/10.1080/03605302.2022.2122836</a>","ama":"Stevens A, Winkler M. Taxis-driven persistent localization in a degenerate Keller-Segel system. <i>Communications in Partial Differential Equations</i>. 2022;47(12):2341-2362. doi:<a href=\"https://doi.org/10.1080/03605302.2022.2122836\">10.1080/03605302.2022.2122836</a>","ieee":"A. Stevens and M. Winkler, “Taxis-driven persistent localization in a degenerate Keller-Segel system,” <i>Communications in Partial Differential Equations</i>, vol. 47, no. 12, pp. 2341–2362, 2022, doi: <a href=\"https://doi.org/10.1080/03605302.2022.2122836\">10.1080/03605302.2022.2122836</a>.","chicago":"Stevens, Angela, and Michael Winkler. “Taxis-Driven Persistent Localization in a Degenerate Keller-Segel System.” <i>Communications in Partial Differential Equations</i> 47, no. 12 (2022): 2341–62. <a href=\"https://doi.org/10.1080/03605302.2022.2122836\">https://doi.org/10.1080/03605302.2022.2122836</a>."},"publication_identifier":{"issn":["0360-5302","1532-4133"]},"publication_status":"published","issue":"12","language":[{"iso":"eng"}],"_id":"63298","user_id":"31496","status":"public","publication":"Communications in Partial Differential Equations","type":"journal_article"},{"citation":{"ama":"Winkler M. Slow Grow-up in a Quasilinear Keller–Segel System. <i>Journal of Dynamics and Differential Equations</i>. 2022;36(2):1677-1702. doi:<a href=\"https://doi.org/10.1007/s10884-022-10167-w\">10.1007/s10884-022-10167-w</a>","ieee":"M. Winkler, “Slow Grow-up in a Quasilinear Keller–Segel System,” <i>Journal of Dynamics and Differential Equations</i>, vol. 36, no. 2, pp. 1677–1702, 2022, doi: <a href=\"https://doi.org/10.1007/s10884-022-10167-w\">10.1007/s10884-022-10167-w</a>.","chicago":"Winkler, Michael. “Slow Grow-up in a Quasilinear Keller–Segel System.” <i>Journal of Dynamics and Differential Equations</i> 36, no. 2 (2022): 1677–1702. <a href=\"https://doi.org/10.1007/s10884-022-10167-w\">https://doi.org/10.1007/s10884-022-10167-w</a>.","apa":"Winkler, M. (2022). Slow Grow-up in a Quasilinear Keller–Segel System. <i>Journal of Dynamics and Differential Equations</i>, <i>36</i>(2), 1677–1702. <a href=\"https://doi.org/10.1007/s10884-022-10167-w\">https://doi.org/10.1007/s10884-022-10167-w</a>","short":"M. Winkler, Journal of Dynamics and Differential Equations 36 (2022) 1677–1702.","mla":"Winkler, Michael. “Slow Grow-up in a Quasilinear Keller–Segel System.” <i>Journal of Dynamics and Differential Equations</i>, vol. 36, no. 2, Springer Science and Business Media LLC, 2022, pp. 1677–702, doi:<a href=\"https://doi.org/10.1007/s10884-022-10167-w\">10.1007/s10884-022-10167-w</a>.","bibtex":"@article{Winkler_2022, title={Slow Grow-up in a Quasilinear Keller–Segel System}, volume={36}, DOI={<a href=\"https://doi.org/10.1007/s10884-022-10167-w\">10.1007/s10884-022-10167-w</a>}, number={2}, journal={Journal of Dynamics and Differential Equations}, publisher={Springer Science and Business Media LLC}, author={Winkler, Michael}, year={2022}, pages={1677–1702} }"},"page":"1677-1702","intvolume":"        36","year":"2022","issue":"2","publication_status":"published","publication_identifier":{"issn":["1040-7294","1572-9222"]},"doi":"10.1007/s10884-022-10167-w","title":"Slow Grow-up in a Quasilinear Keller–Segel System","author":[{"last_name":"Winkler","full_name":"Winkler, Michael","id":"31496","first_name":"Michael"}],"date_created":"2025-12-18T19:10:32Z","volume":36,"publisher":"Springer Science and Business Media LLC","date_updated":"2025-12-18T20:10:14Z","status":"public","abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title><jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\Omega =B_R(0)\\subset \\mathbb {R}^n$$</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:msub>\r\n                      <mml:mi>B</mml:mi>\r\n                      <mml:mi>R</mml:mi>\r\n                    </mml:msub>\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: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:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$n\\ge 2$$</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>2</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, the chemotaxis system <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\left\\{ \\begin{array}{l}u_t = \\nabla \\cdot \\big ( D(u) \\nabla u \\big ) - \\nabla \\cdot \\big ( uS(u)\\nabla v\\big ), \\\\ 0 = \\Delta v - \\mu + u, \\qquad \\mu =\\frac{1}{|\\Omega |} \\int _\\Omega u, \\end{array} \\right. \\qquad \\qquad (\\star ) \\end{aligned}$$</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>D</mml:mi>\r\n                                        <mml:mrow>\r\n                                          <mml:mo>(</mml:mo>\r\n                                          <mml:mi>u</mml:mi>\r\n                                          <mml:mo>)</mml:mo>\r\n                                        </mml:mrow>\r\n                                        <mml:mi>∇</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>∇</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>S</mml:mi>\r\n                                        <mml:mrow>\r\n                                          <mml:mo>(</mml:mo>\r\n                                          <mml:mi>u</mml:mi>\r\n                                          <mml:mo>)</mml:mo>\r\n                                        </mml:mrow>\r\n                                        <mml:mi>∇</mml:mi>\r\n                                        <mml:mi>v</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: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:mn>0</mml:mn>\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>μ</mml:mi>\r\n                                        <mml:mo>+</mml:mo>\r\n                                        <mml:mi>u</mml:mi>\r\n                                        <mml:mo>,</mml:mo>\r\n                                        <mml:mspace/>\r\n                                        <mml:mi>μ</mml:mi>\r\n                                        <mml:mo>=</mml:mo>\r\n                                        <mml:mfrac>\r\n                                          <mml:mn>1</mml:mn>\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:mfrac>\r\n                                        <mml:msub>\r\n                                          <mml:mo>∫</mml:mo>\r\n                                          <mml:mi>Ω</mml:mi>\r\n                                        </mml:msub>\r\n                                        <mml:mi>u</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 under no-flux boundary conditions, with a focus on nonlinearities <jats:inline-formula><jats:alternatives><jats:tex-math>$$S\\in C^2([0,\\infty ))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>S</mml:mi>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mn>2</mml:mn>\r\n                    </mml:msup>\r\n                    <mml: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> which exhibit super-algebraically fast decay in the sense that with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_S&gt;0, \\beta \\in [0,1)$$</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>K</mml:mi>\r\n                      <mml:mi>S</mml:mi>\r\n                    </mml:msub>\r\n                    <mml:mo>&gt;</mml:mo>\r\n                    <mml:mn>0</mml:mn>\r\n                    <mml:mo>,</mml:mo>\r\n                    <mml:mi>β</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:mn>1</mml:mn>\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>$$\\xi _0&gt;0$$</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>ξ</mml:mi>\r\n                      <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n                    <mml:mo>&gt;</mml:mo>\r\n                    <mml:mn>0</mml:mn>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} S(\\xi )&gt;0 \\quad \\text{ and } \\quad S'(\\xi ) \\le -K_S\\xi ^{-\\beta } S(\\xi ) \\qquad \\text{ for } \\text{ all } \\xi \\ge \\xi _0. \\end{aligned}$$</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:mi>S</mml:mi>\r\n                            <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n                            <mml:mo>&gt;</mml:mo>\r\n                            <mml:mn>0</mml:mn>\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:msup>\r\n                              <mml:mi>S</mml:mi>\r\n                              <mml:mo>′</mml:mo>\r\n                            </mml:msup>\r\n                            <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n                            <mml:mo>≤</mml:mo>\r\n                            <mml:mo>-</mml:mo>\r\n                            <mml:msub>\r\n                              <mml:mi>K</mml:mi>\r\n                              <mml:mi>S</mml:mi>\r\n                            </mml:msub>\r\n                            <mml:msup>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mrow>\r\n                                <mml:mo>-</mml:mo>\r\n                                <mml:mi>β</mml:mi>\r\n                              </mml:mrow>\r\n                            </mml:msup>\r\n                            <mml:mi>S</mml:mi>\r\n                            <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>for</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>all</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mi>ξ</mml:mi>\r\n                            <mml:mo>≥</mml:mo>\r\n                            <mml:msub>\r\n                              <mml:mi>ξ</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:mtd>\r\n                      </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:disp-formula>It is, inter alia, shown that if furthermore <jats:inline-formula><jats:alternatives><jats:tex-math>$$D\\in C^2((0,\\infty ))$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>D</mml:mi>\r\n                    <mml:mo>∈</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mn>2</mml:mn>\r\n                    </mml:msup>\r\n                    <mml: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> is positive and suitably small in relation to <jats:italic>S</jats:italic> by satisfying <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\frac{\\xi S(\\xi )}{D(\\xi )} \\ge K_{SD}\\xi ^\\lambda \\qquad \\text{ for } \\text{ all } \\xi \\ge \\xi _0 \\end{aligned}$$</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:mfrac>\r\n                              <mml:mrow>\r\n                                <mml:mi>ξ</mml:mi>\r\n                                <mml:mi>S</mml:mi>\r\n                                <mml:mo>(</mml:mo>\r\n                                <mml:mi>ξ</mml:mi>\r\n                                <mml:mo>)</mml:mo>\r\n                              </mml:mrow>\r\n                              <mml:mrow>\r\n                                <mml:mi>D</mml:mi>\r\n                                <mml:mo>(</mml:mo>\r\n                                <mml:mi>ξ</mml:mi>\r\n                                <mml:mo>)</mml:mo>\r\n                              </mml:mrow>\r\n                            </mml:mfrac>\r\n                            <mml:mo>≥</mml:mo>\r\n                            <mml:msub>\r\n                              <mml:mi>K</mml:mi>\r\n                              <mml:mrow>\r\n                                <mml:mi>SD</mml:mi>\r\n                              </mml:mrow>\r\n                            </mml:msub>\r\n                            <mml:msup>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mi>λ</mml:mi>\r\n                            </mml:msup>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>for</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>all</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mi>ξ</mml:mi>\r\n                            <mml:mo>≥</mml:mo>\r\n                            <mml:msub>\r\n                              <mml:mi>ξ</mml:mi>\r\n                              <mml:mn>0</mml:mn>\r\n                            </mml:msub>\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>with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_{SD}&gt;0$$</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>K</mml:mi>\r\n                      <mml:mrow>\r\n                        <mml:mi>SD</mml:mi>\r\n                      </mml:mrow>\r\n                    </mml:msub>\r\n                    <mml:mo>&gt;</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>$$\\lambda &gt;\\frac{2}{n}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>λ</mml:mi>\r\n                    <mml:mo>&gt;</mml:mo>\r\n                    <mml:mfrac>\r\n                      <mml:mn>2</mml:mn>\r\n                      <mml:mi>n</mml:mi>\r\n                    </mml:mfrac>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>, then throughout a considerably large set of initial data, (<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 global classical solutions (<jats:italic>u</jats:italic>, <jats:italic>v</jats:italic>) fulfilling <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\frac{z(t)}{C} \\le \\Vert u(\\cdot ,t)\\Vert _{L^\\infty (\\Omega )} \\le Cz(t) \\qquad \\text{ for } \\text{ all } t&gt;0, \\end{aligned}$$</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:mfrac>\r\n                              <mml:mrow>\r\n                                <mml:mi>z</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:mi>C</mml:mi>\r\n                            </mml:mfrac>\r\n                            <mml:mo>≤</mml:mo>\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: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>≤</mml:mo>\r\n                            <mml:mi>C</mml:mi>\r\n                            <mml:mi>z</mml:mi>\r\n                            <mml:mrow>\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:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>for</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mspace/>\r\n                            <mml:mtext>all</mml:mtext>\r\n                            <mml:mspace/>\r\n                            <mml:mi>t</mml:mi>\r\n                            <mml:mo>&gt;</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n                            <mml:mo>,</mml:mo>\r\n                          </mml: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>with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$C=C^{(u,v)}\\ge 1$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>C</mml:mi>\r\n                    <mml:mo>=</mml:mo>\r\n                    <mml:msup>\r\n                      <mml:mi>C</mml:mi>\r\n                      <mml:mrow>\r\n                        <mml:mo>(</mml:mo>\r\n                        <mml:mi>u</mml:mi>\r\n                        <mml:mo>,</mml:mo>\r\n                        <mml:mi>v</mml:mi>\r\n                        <mml:mo>)</mml:mo>\r\n                      </mml:mrow>\r\n                    </mml:msup>\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>, where <jats:italic>z</jats:italic> denotes the solution of <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned} \\left\\{ \\begin{array}{l}z'(t) = z^2(t) \\cdot S\\big ( z(t)\\big ), \\qquad t&gt;0, \\\\ z(0)=\\xi _0, \\end{array} \\right. \\end{aligned}$$</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:mfenced>\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>z</mml:mi>\r\n                                        <mml:mo>′</mml:mo>\r\n                                      </mml:msup>\r\n                                      <mml:mrow>\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:msup>\r\n                                        <mml:mi>z</mml:mi>\r\n                                        <mml:mn>2</mml:mn>\r\n                                      </mml:msup>\r\n                                      <mml:mrow>\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:mi>S</mml:mi>\r\n                                      <mml:mrow>\r\n                                        <mml:mo>(</mml:mo>\r\n                                      </mml:mrow>\r\n                                      <mml:mi>z</mml:mi>\r\n                                      <mml:mrow>\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:mrow>\r\n                                        <mml:mo>)</mml:mo>\r\n                                      </mml:mrow>\r\n                                      <mml:mo>,</mml:mo>\r\n                                      <mml:mspace/>\r\n                                      <mml:mi>t</mml:mi>\r\n                                      <mml:mo>&gt;</mml:mo>\r\n                                      <mml:mn>0</mml:mn>\r\n                                      <mml:mo>,</mml:mo>\r\n                                    </mml: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:mi>z</mml:mi>\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:mrow>\r\n                                      <mml:mo>=</mml:mo>\r\n                                      <mml:msub>\r\n                                        <mml:mi>ξ</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:mtd>\r\n                                </mml:mtr>\r\n                              </mml:mtable>\r\n                            </mml:mrow>\r\n                          </mml:mfenced>\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>which is seen to exist globally, and to satisfy <jats:inline-formula><jats:alternatives><jats:tex-math>$$z(t)\\rightarrow +\\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n                    <mml:mi>z</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:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula> as <jats:inline-formula><jats:alternatives><jats:tex-math>$$t\\rightarrow \\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\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:math></jats:alternatives></jats:inline-formula>. As particular examples, exponentially and doubly exponentially decaying <jats:italic>S</jats:italic> are found to imply corresponding infinite-time blow-up properties 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>) at logarithmic and doubly logarithmic rates, respectively.</jats:p>"}],"type":"journal_article","publication":"Journal of Dynamics and Differential Equations","language":[{"iso":"eng"}],"user_id":"31496","_id":"63266"},{"publication_status":"published","publication_identifier":{"issn":["0022-0396"]},"citation":{"ama":"Tao Y, Winkler M. Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension. <i>Journal of Differential Equations</i>. 2022;343:390-418. doi:<a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">10.1016/j.jde.2022.10.022</a>","chicago":"Tao, Youshan, and Michael Winkler. “Global Solutions to a Keller-Segel-Consumption System Involving Singularly Signal-Dependent Motilities in Domains of Arbitrary Dimension.” <i>Journal of Differential Equations</i> 343 (2022): 390–418. <a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">https://doi.org/10.1016/j.jde.2022.10.022</a>.","ieee":"Y. Tao and M. Winkler, “Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension,” <i>Journal of Differential Equations</i>, vol. 343, pp. 390–418, 2022, doi: <a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">10.1016/j.jde.2022.10.022</a>.","bibtex":"@article{Tao_Winkler_2022, title={Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension}, volume={343}, DOI={<a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">10.1016/j.jde.2022.10.022</a>}, journal={Journal of Differential Equations}, publisher={Elsevier BV}, author={Tao, Youshan and Winkler, Michael}, year={2022}, pages={390–418} }","mla":"Tao, Youshan, and Michael Winkler. “Global Solutions to a Keller-Segel-Consumption System Involving Singularly Signal-Dependent Motilities in Domains of Arbitrary Dimension.” <i>Journal of Differential Equations</i>, vol. 343, Elsevier BV, 2022, pp. 390–418, doi:<a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">10.1016/j.jde.2022.10.022</a>.","short":"Y. Tao, M. Winkler, Journal of Differential Equations 343 (2022) 390–418.","apa":"Tao, Y., &#38; Winkler, M. (2022). Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension. <i>Journal of Differential Equations</i>, <i>343</i>, 390–418. <a href=\"https://doi.org/10.1016/j.jde.2022.10.022\">https://doi.org/10.1016/j.jde.2022.10.022</a>"},"page":"390-418","intvolume":"       343","year":"2022","date_created":"2025-12-18T19:13:04Z","author":[{"full_name":"Tao, Youshan","last_name":"Tao","first_name":"Youshan"},{"first_name":"Michael","last_name":"Winkler","id":"31496","full_name":"Winkler, Michael"}],"volume":343,"publisher":"Elsevier BV","date_updated":"2025-12-18T20:11:02Z","doi":"10.1016/j.jde.2022.10.022","title":"Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension","type":"journal_article","publication":"Journal of Differential Equations","status":"public","user_id":"31496","_id":"63272","language":[{"iso":"eng"}]},{"doi":"10.1016/j.na.2022.113153","title":"Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing","date_created":"2025-12-18T19:11:16Z","author":[{"last_name":"Desvillettes","full_name":"Desvillettes, Laurent","first_name":"Laurent"},{"last_name":"Laurençot","full_name":"Laurençot, Philippe","first_name":"Philippe"},{"full_name":"Trescases, Ariane","last_name":"Trescases","first_name":"Ariane"},{"first_name":"Michael","last_name":"Winkler","full_name":"Winkler, Michael","id":"31496"}],"volume":226,"publisher":"Elsevier BV","date_updated":"2025-12-18T20:10:32Z","citation":{"ieee":"L. Desvillettes, P. Laurençot, A. Trescases, and M. Winkler, “Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing,” <i>Nonlinear Analysis</i>, vol. 226, Art. no. 113153, 2022, doi: <a href=\"https://doi.org/10.1016/j.na.2022.113153\">10.1016/j.na.2022.113153</a>.","chicago":"Desvillettes, Laurent, Philippe Laurençot, Ariane Trescases, and Michael Winkler. “Weak Solutions to Triangular Cross Diffusion Systems Modeling Chemotaxis with Local Sensing.” <i>Nonlinear Analysis</i> 226 (2022). <a href=\"https://doi.org/10.1016/j.na.2022.113153\">https://doi.org/10.1016/j.na.2022.113153</a>.","ama":"Desvillettes L, Laurençot P, Trescases A, Winkler M. Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing. <i>Nonlinear Analysis</i>. 2022;226. doi:<a href=\"https://doi.org/10.1016/j.na.2022.113153\">10.1016/j.na.2022.113153</a>","short":"L. Desvillettes, P. Laurençot, A. Trescases, M. Winkler, Nonlinear Analysis 226 (2022).","bibtex":"@article{Desvillettes_Laurençot_Trescases_Winkler_2022, title={Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing}, volume={226}, DOI={<a href=\"https://doi.org/10.1016/j.na.2022.113153\">10.1016/j.na.2022.113153</a>}, number={113153}, journal={Nonlinear Analysis}, publisher={Elsevier BV}, author={Desvillettes, Laurent and Laurençot, Philippe and Trescases, Ariane and Winkler, Michael}, year={2022} }","mla":"Desvillettes, Laurent, et al. “Weak Solutions to Triangular Cross Diffusion Systems Modeling Chemotaxis with Local Sensing.” <i>Nonlinear Analysis</i>, vol. 226, 113153, Elsevier BV, 2022, doi:<a href=\"https://doi.org/10.1016/j.na.2022.113153\">10.1016/j.na.2022.113153</a>.","apa":"Desvillettes, L., Laurençot, P., Trescases, A., &#38; Winkler, M. (2022). Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing. <i>Nonlinear Analysis</i>, <i>226</i>, Article 113153. <a href=\"https://doi.org/10.1016/j.na.2022.113153\">https://doi.org/10.1016/j.na.2022.113153</a>"},"intvolume":"       226","year":"2022","publication_status":"published","publication_identifier":{"issn":["0362-546X"]},"language":[{"iso":"eng"}],"article_number":"113153","user_id":"31496","_id":"63268","status":"public","type":"journal_article","publication":"Nonlinear Analysis"},{"language":[{"iso":"eng"}],"_id":"63278","user_id":"31496","abstract":[{"lang":"eng","text":"<jats:title>Abstract</jats:title>\r\n               <jats:p>The Neumann problem for (0.1)$$ \\begin{align}&amp; V_t = \\Delta V-aV+f(x,t) \\end{align}$$is considered in bounded domains $\\Omega \\subset {\\mathbb {R}}^n$ with smooth boundary, where $n\\ge 1$ and $a\\in {\\mathbb {R}}$. By means of a variational approach, a statement on boundedness of the quantities $$ \\begin{eqnarray*} \\sup_{t\\in (0,T)} \\int_\\Omega \\big|\\nabla V(\\cdot,t)\\big|^p L^{\\frac{n+p}{n+2}} \\Big( \\big|\\nabla V(\\cdot,t)\\big| \\Big) \\end{eqnarray*}$$in dependence on the expressions (0.2)$$ \\begin{align}&amp; \\sup_{t\\in (0,T-\\tau)} \\int_t^{t+\\tau} \\int_\\Omega |f|^{\\frac{(n+2)p}{n+p}} L\\big( |f|\\big) \\end{align}$$is derived for $p\\ge 2$, $\\tau&amp;gt;0$, and $T\\ge 2\\tau $, provided that $L\\in C^0([0,\\infty ))$ is positive, strictly increasing, unbounded, and slowly growing in the sense that $\\limsup _{s\\to \\infty } \\frac {L(s^{\\lambda _0})}{L(s)} &amp;lt;\\infty $ for some $\\lambda _0&amp;gt;1$. In the particular case when $p=n\\ge 2$, an additional condition on growth of $L$, particularly satisfied by $L(\\xi ):=\\ln ^\\alpha (\\xi +b)$ whenever $b&amp;gt;0$ and $\\alpha&amp;gt;\\frac {(n+2)(n-1)}{2n}$, is identified as sufficient to ensure that as a consequence of the above, bounds for theintegrals in (0.2) even imply estimates for the spatio-temporal modulus of continuity of solutions to (0.1). A subsequent application to the Keller–Segel system $$ \\begin{eqnarray*} \\left\\{ \\begin{array}{l} u_t = \\nabla \\cdot \\big( D(v)\\nabla u\\big) - \\nabla \\cdot \\big( uS(v)\\nabla v\\big) + ru - \\mu u^2, \\\\[1mm] v_t = \\Delta v-v+u, \\end{array} \\right. \\end{eqnarray*}$$shows that when $n=2$, $r\\in {\\mathbb {R}}$, $0&amp;lt;D\\in C^2([0,\\infty ))$, and $S\\in C^2([0,\\infty )) \\cap W^{1,\\infty }((0,\\infty ))$ and thus especially in the presence of arbitrarily strong diffusion degeneracies implied by rapid decay of $D$, any choice of $\\mu&amp;gt;0$ excludes blowup in the sense that for all suitably regular nonnegative initial data, an associated initial-boundary value problem admits a global bounded classical solution.</jats:p>"}],"status":"public","publication":"International Mathematics Research Notices","type":"journal_article","title":"A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System","doi":"10.1093/imrn/rnac286","publisher":"Oxford University Press (OUP)","date_updated":"2025-12-18T20:11:43Z","volume":2023,"date_created":"2025-12-18T19:15:52Z","author":[{"first_name":"Michael","last_name":"Winkler","full_name":"Winkler, Michael","id":"31496"}],"year":"2022","intvolume":"      2023","page":"16336-16393","citation":{"apa":"Winkler, M. (2022). A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System. <i>International Mathematics Research Notices</i>, <i>2023</i>(19), 16336–16393. <a href=\"https://doi.org/10.1093/imrn/rnac286\">https://doi.org/10.1093/imrn/rnac286</a>","short":"M. Winkler, International Mathematics Research Notices 2023 (2022) 16336–16393.","bibtex":"@article{Winkler_2022, title={A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System}, volume={2023}, DOI={<a href=\"https://doi.org/10.1093/imrn/rnac286\">10.1093/imrn/rnac286</a>}, number={19}, journal={International Mathematics Research Notices}, publisher={Oxford University Press (OUP)}, author={Winkler, Michael}, year={2022}, pages={16336–16393} }","mla":"Winkler, Michael. “A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System.” <i>International Mathematics Research Notices</i>, vol. 2023, no. 19, Oxford University Press (OUP), 2022, pp. 16336–93, doi:<a href=\"https://doi.org/10.1093/imrn/rnac286\">10.1093/imrn/rnac286</a>.","ama":"Winkler M. A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System. <i>International Mathematics Research Notices</i>. 2022;2023(19):16336-16393. doi:<a href=\"https://doi.org/10.1093/imrn/rnac286\">10.1093/imrn/rnac286</a>","chicago":"Winkler, Michael. “A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System.” <i>International Mathematics Research Notices</i> 2023, no. 19 (2022): 16336–93. <a href=\"https://doi.org/10.1093/imrn/rnac286\">https://doi.org/10.1093/imrn/rnac286</a>.","ieee":"M. Winkler, “A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System,” <i>International Mathematics Research Notices</i>, vol. 2023, no. 19, pp. 16336–16393, 2022, doi: <a href=\"https://doi.org/10.1093/imrn/rnac286\">10.1093/imrn/rnac286</a>."},"publication_identifier":{"issn":["1073-7928","1687-0247"]},"publication_status":"published","issue":"19"},{"publisher":"European Mathematical Society - EMS - Publishing House GmbH","date_updated":"2025-12-18T20:11:51Z","author":[{"full_name":"Winkler, Michael","id":"31496","last_name":"Winkler","first_name":"Michael"}],"date_created":"2025-12-18T19:16:13Z","volume":25,"title":"Does Leray’s structure theorem withstand buoyancy-driven chemotaxis-fluid interaction?","doi":"10.4171/jems/1226","publication_status":"published","publication_identifier":{"issn":["1435-9855","1435-9863"]},"issue":"4","year":"2022","citation":{"apa":"Winkler, M. (2022). Does Leray’s structure theorem withstand buoyancy-driven chemotaxis-fluid interaction? <i>Journal of the European Mathematical Society</i>, <i>25</i>(4), 1423–1456. <a href=\"https://doi.org/10.4171/jems/1226\">https://doi.org/10.4171/jems/1226</a>","bibtex":"@article{Winkler_2022, title={Does Leray’s structure theorem withstand buoyancy-driven chemotaxis-fluid interaction?}, volume={25}, DOI={<a href=\"https://doi.org/10.4171/jems/1226\">10.4171/jems/1226</a>}, number={4}, journal={Journal of the European Mathematical Society}, publisher={European Mathematical Society - EMS - Publishing House GmbH}, author={Winkler, Michael}, year={2022}, pages={1423–1456} }","short":"M. Winkler, Journal of the European Mathematical Society 25 (2022) 1423–1456.","mla":"Winkler, Michael. “Does Leray’s Structure Theorem Withstand Buoyancy-Driven Chemotaxis-Fluid Interaction?” <i>Journal of the European Mathematical Society</i>, vol. 25, no. 4, European Mathematical Society - EMS - Publishing House GmbH, 2022, pp. 1423–56, doi:<a href=\"https://doi.org/10.4171/jems/1226\">10.4171/jems/1226</a>.","chicago":"Winkler, Michael. “Does Leray’s Structure Theorem Withstand Buoyancy-Driven Chemotaxis-Fluid Interaction?” <i>Journal of the European Mathematical Society</i> 25, no. 4 (2022): 1423–56. <a href=\"https://doi.org/10.4171/jems/1226\">https://doi.org/10.4171/jems/1226</a>.","ieee":"M. Winkler, “Does Leray’s structure theorem withstand buoyancy-driven chemotaxis-fluid interaction?,” <i>Journal of the European Mathematical Society</i>, vol. 25, no. 4, pp. 1423–1456, 2022, doi: <a href=\"https://doi.org/10.4171/jems/1226\">10.4171/jems/1226</a>.","ama":"Winkler M. Does Leray’s structure theorem withstand buoyancy-driven chemotaxis-fluid interaction? <i>Journal of the European Mathematical Society</i>. 2022;25(4):1423-1456. doi:<a href=\"https://doi.org/10.4171/jems/1226\">10.4171/jems/1226</a>"},"intvolume":"        25","page":"1423-1456","_id":"63279","user_id":"31496","language":[{"iso":"eng"}],"type":"journal_article","publication":"Journal of the European Mathematical Society","abstract":[{"lang":"eng","text":"<jats:p>\r\n                    In a smoothly bounded convex domain\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>\\Omega \\subset \\mathbb{R}^3</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    , we consider the chemotaxis-Navier–Stokes model\r\n                  </jats:p>\r\n                  <jats:p>\r\n                    <jats:disp-formula>\r\n                      <jats:tex-math>\\begin{cases} n_t + u\\cdot\\nabla n = \\Delta n - \\nabla \\cdot (n\\nabla c), &amp; x\\in \\Omega, \\, t&gt;0, \\\\ c_t + u\\cdot\\nabla c = \\Delta c -nc, &amp; x\\in \\Omega, \\, t&gt;0, \\\\ u_t + (u\\cdot\\nabla) u = \\Delta u + \\nabla P + n\\nabla\\Phi, \\quad \\nabla\\cdot u=0, &amp; x\\in \\Omega, \\, t&gt;0, \\end{cases} \\quad (\\star)</jats:tex-math>\r\n                    </jats:disp-formula>\r\n                  </jats:p>\r\n                  <jats:p>\r\n                    proposed by Goldstein et al. to describe pattern formation in populations of aerobic bacteria interacting with their liquid environment via transport and buoyancy. Known results have asserted that under appropriate regularity assumptions on\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>\\Phi</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    and the initial data, a corresponding no-flux/no-flux/Dirichlet initial-boundary value problem is globally solvable in a framework of so-called weak energy solutions, and that any such solution eventually becomes smooth and classical.\r\n                  </jats:p>\r\n                  <jats:p>\r\n                    Going beyond this, the present work focuses on the possible extent of unboundedness phenomena also on short timescales, and hence investigates in more detail the set of times in\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>(0,\\infty)</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    at which solutions may develop singularities. The main results in this direction reveal the existence of a global weak energy solution which coincides with a smooth function throughout\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>\\overline{\\Omega}\\times E</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    , where\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>E</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    denotes a countable union of open intervals which is such that\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>|(0,\\infty)\\setminus E|=0</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    . In particular, this indicates that a similar feature of the unperturbed Navie–Stokes equations, known as Leray’s structure theorem, persists even in the presence of the coupling to the attractive and hence potentially destabilizing cross-diffusive mechanism in the full system (\r\n                    <jats:inline-formula>\r\n                      <jats:tex-math>\\star</jats:tex-math>\r\n                    </jats:inline-formula>\r\n                    ).\r\n                  </jats:p>"}],"status":"public"},{"language":[{"iso":"eng"}],"_id":"63274","user_id":"31496","abstract":[{"lang":"eng","text":"<jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega \\subset \\mathbb {R}^{n}$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline1.png\" /></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$n\\ge 2$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline2.png\" /></jats:alternatives></jats:inline-formula>, the chemotaxis system\r\n<jats:disp-formula><jats:alternatives><jats:tex-math>\\[ \\left\\{ \\begin{array}{@{}l} u_t = \\nabla \\cdot \\big( D(u)\\nabla u\\big) + \\nabla\\cdot \\big(\\dfrac{u}{v} \\nabla v\\big), \\\\ 0=\\Delta v - uv \\end{array} \\right. \\]</jats:tex-math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" position=\"float\" xlink:href=\"S0308210522000397_eqnU1.png\" /></jats:alternatives></jats:disp-formula>is considered along with no-flux boundary conditions for <jats:inline-formula><jats:alternatives><jats:tex-math>$u$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline3.png\" /></jats:alternatives></jats:inline-formula> and with prescribed constant positive Dirichlet boundary data for <jats:inline-formula><jats:alternatives><jats:tex-math>$v$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline4.png\" /></jats:alternatives></jats:inline-formula>. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$D\\in C^{3}([0,\\infty ))$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline5.png\" /></jats:alternatives></jats:inline-formula> is such that <jats:inline-formula><jats:alternatives><jats:tex-math>$0&lt; D(\\xi ) \\le {K_D} (\\xi +1)^{-\\alpha }$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline6.png\" /></jats:alternatives></jats:inline-formula> for all <jats:inline-formula><jats:alternatives><jats:tex-math>$\\xi &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline7.png\" /></jats:alternatives></jats:inline-formula> with some <jats:inline-formula><jats:alternatives><jats:tex-math>${K_D}&gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline8.png\" /></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$\\alpha &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline9.png\" /></jats:alternatives></jats:inline-formula>, then for all initial data from a considerably large set of radial functions on <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline10.png\" /></jats:alternatives></jats:inline-formula>, the corresponding initial-boundary value problem admits a solution blowing up in finite time.</jats:p>"}],"status":"public","publication":"Proceedings of the Royal Society of Edinburgh: Section A Mathematics","type":"journal_article","title":"Finite-time blow-up in a repulsive chemotaxis-consumption system","doi":"10.1017/prm.2022.39","date_updated":"2025-12-18T20:11:15Z","publisher":"Cambridge University Press (CUP)","volume":153,"date_created":"2025-12-18T19:14:20Z","author":[{"full_name":"Wang, Yulan","last_name":"Wang","first_name":"Yulan"},{"first_name":"Michael","full_name":"Winkler, Michael","id":"31496","last_name":"Winkler"}],"year":"2022","page":"1150-1166","intvolume":"       153","citation":{"bibtex":"@article{Wang_Winkler_2022, title={Finite-time blow-up in a repulsive chemotaxis-consumption system}, volume={153}, DOI={<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>}, number={4}, journal={Proceedings of the Royal Society of Edinburgh: Section A Mathematics}, publisher={Cambridge University Press (CUP)}, author={Wang, Yulan and Winkler, Michael}, year={2022}, pages={1150–1166} }","mla":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, Cambridge University Press (CUP), 2022, pp. 1150–66, doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>.","short":"Y. Wang, M. Winkler, Proceedings of the Royal Society of Edinburgh: Section A Mathematics 153 (2022) 1150–1166.","apa":"Wang, Y., &#38; Winkler, M. (2022). Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, <i>153</i>(4), 1150–1166. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>","ieee":"Y. Wang and M. Winkler, “Finite-time blow-up in a repulsive chemotaxis-consumption system,” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, pp. 1150–1166, 2022, doi: <a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>.","chicago":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i> 153, no. 4 (2022): 1150–66. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>.","ama":"Wang Y, Winkler M. Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>. 2022;153(4):1150-1166. doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>"},"publication_identifier":{"issn":["0308-2105","1473-7124"]},"publication_status":"published","issue":"4"}]
