{"title":"具有间接信号、密度抑制运动和广义logistic源的趋化系统有界解的非线性生成指标","authors":"Quanyong Zhao, Jinrong Wang","doi":"10.1016/j.jmaa.2025.129290","DOIUrl":null,"url":null,"abstract":"<div><div>In this paper, we study the following chemotaxis-growth system with density-suppressed motility<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd></mtd><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mo>(</mo><mi>u</mi><mi>γ</mi><mo>(</mo><mi>v</mi><mo>)</mo><mo>)</mo><mo>+</mo><mi>r</mi><mi>u</mi><mo>−</mo><mi>μ</mi><msup><mrow><mi>u</mi></mrow><mrow><mi>α</mi></mrow></msup><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd></mtd><mtd><msub><mrow><mi>v</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><msup><mrow><mi>w</mi></mrow><mrow><mi>β</mi></mrow></msup><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd></mtd><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mo>−</mo><mi>δ</mi><mi>w</mi><mo>+</mo><mi>u</mi><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> under homogeneous Neumann boundary conditions in a bounded domain <span><math><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>(</mo><mi>n</mi><mo>≥</mo><mn>2</mn><mo>)</mo></math></span> with smooth boundary, where <span><math><mi>r</mi><mo>∈</mo><mi>R</mi></math></span>, <em>μ</em>, <em>δ</em>, <span><math><mi>β</mi><mo>></mo><mn>0</mn></math></span>, <span><math><mi>α</mi><mo>></mo><mn>1</mn></math></span>, and the positive motility function <span><math><mi>γ</mi><mo>∈</mo><msup><mrow><mi>C</mi></mrow><mrow><mn>3</mn></mrow></msup><mo>(</mo><mo>[</mo><mn>0</mn><mo>,</mo><mo>∞</mo><mo>)</mo><mo>)</mo></math></span> satisfies <span><math><msup><mrow><mi>γ</mi></mrow><mrow><mo>′</mo></mrow></msup><mo>(</mo><mi>s</mi><mo>)</mo><mo>≤</mo><mn>0</mn></math></span> for all <span><math><mi>s</mi><mo>≥</mo><mn>0</mn></math></span>. The main purpose of this paper is to establish the global boundedness and stabilization of classical solutions for such kind of chemotaxis system. More precisely, we showed that if <span><math><mi>β</mi><mo><</mo><mfrac><mrow><mn>2</mn><mi>α</mi></mrow><mrow><mi>n</mi></mrow></mfrac></math></span>, the system possesses a globally bounded classical solution, and further, if <em>γ</em> also fulfills the additional assumption that <span><math><mfrac><mrow><msup><mrow><mi>γ</mi></mrow><mrow><mo>′</mo></mrow></msup></mrow><mrow><mi>γ</mi></mrow></mfrac></math></span> is bounded on <span><math><mo>[</mo><mn>0</mn><mo>,</mo><mo>∞</mo><mo>)</mo></math></span>, then for <span><math><mi>α</mi><mo>></mo><mfrac><mrow><mi>n</mi></mrow><mrow><mi>n</mi><mo>−</mo><mn>2</mn></mrow></mfrac></math></span>, the above restriction can be optimized as <span><math><mi>β</mi><mo><</mo><mfrac><mrow><mo>(</mo><mi>n</mi><mo>+</mo><mn>2</mn><mo>)</mo><mi>α</mi><mo>−</mo><mi>n</mi></mrow><mrow><mn>2</mn><mi>n</mi></mrow></mfrac></math></span>. Furthermore, we obtained that the solution will converge to the equilibrium <span><math><mo>(</mo><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mi>δ</mi></mrow><mrow><mi>β</mi></mrow></msup></mrow></mfrac><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mi>β</mi></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mi>δ</mi></mrow></mfrac><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>)</mo></math></span> with an exponential decay rate in <span><math><msup><mrow><mo>(</mo><msup><mrow><mi>L</mi></mrow><mrow><mo>∞</mo></mrow></msup><mo>(</mo><mi>Ω</mi><mo>)</mo><mo>)</mo></mrow><mrow><mn>3</mn></mrow></msup></math></span>, where <span><math><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub><mo>:</mo><mo>=</mo><mi>max</mi><mo></mo><mo>{</mo><mi>r</mi><mo>,</mo><mn>0</mn><mo>}</mo></math></span>.</div></div>","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"547 1","pages":"Article 129290"},"PeriodicalIF":1.2000,"publicationDate":"2025-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Nonlinear generation index of bounded solutions in a chemotaxis system with indirect signal, density-suppressed motility and generalized logistic source\",\"authors\":\"Quanyong Zhao, Jinrong Wang\",\"doi\":\"10.1016/j.jmaa.2025.129290\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>In this paper, we study the following chemotaxis-growth system with density-suppressed motility<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd></mtd><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mo>(</mo><mi>u</mi><mi>γ</mi><mo>(</mo><mi>v</mi><mo>)</mo><mo>)</mo><mo>+</mo><mi>r</mi><mi>u</mi><mo>−</mo><mi>μ</mi><msup><mrow><mi>u</mi></mrow><mrow><mi>α</mi></mrow></msup><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd></mtd><mtd><msub><mrow><mi>v</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><msup><mrow><mi>w</mi></mrow><mrow><mi>β</mi></mrow></msup><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd></mtd><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mo>−</mo><mi>δ</mi><mi>w</mi><mo>+</mo><mi>u</mi><mo>,</mo></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> under homogeneous Neumann boundary conditions in a bounded domain <span><math><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>(</mo><mi>n</mi><mo>≥</mo><mn>2</mn><mo>)</mo></math></span> with smooth boundary, where <span><math><mi>r</mi><mo>∈</mo><mi>R</mi></math></span>, <em>μ</em>, <em>δ</em>, <span><math><mi>β</mi><mo>></mo><mn>0</mn></math></span>, <span><math><mi>α</mi><mo>></mo><mn>1</mn></math></span>, and the positive motility function <span><math><mi>γ</mi><mo>∈</mo><msup><mrow><mi>C</mi></mrow><mrow><mn>3</mn></mrow></msup><mo>(</mo><mo>[</mo><mn>0</mn><mo>,</mo><mo>∞</mo><mo>)</mo><mo>)</mo></math></span> satisfies <span><math><msup><mrow><mi>γ</mi></mrow><mrow><mo>′</mo></mrow></msup><mo>(</mo><mi>s</mi><mo>)</mo><mo>≤</mo><mn>0</mn></math></span> for all <span><math><mi>s</mi><mo>≥</mo><mn>0</mn></math></span>. The main purpose of this paper is to establish the global boundedness and stabilization of classical solutions for such kind of chemotaxis system. More precisely, we showed that if <span><math><mi>β</mi><mo><</mo><mfrac><mrow><mn>2</mn><mi>α</mi></mrow><mrow><mi>n</mi></mrow></mfrac></math></span>, the system possesses a globally bounded classical solution, and further, if <em>γ</em> also fulfills the additional assumption that <span><math><mfrac><mrow><msup><mrow><mi>γ</mi></mrow><mrow><mo>′</mo></mrow></msup></mrow><mrow><mi>γ</mi></mrow></mfrac></math></span> is bounded on <span><math><mo>[</mo><mn>0</mn><mo>,</mo><mo>∞</mo><mo>)</mo></math></span>, then for <span><math><mi>α</mi><mo>></mo><mfrac><mrow><mi>n</mi></mrow><mrow><mi>n</mi><mo>−</mo><mn>2</mn></mrow></mfrac></math></span>, the above restriction can be optimized as <span><math><mi>β</mi><mo><</mo><mfrac><mrow><mo>(</mo><mi>n</mi><mo>+</mo><mn>2</mn><mo>)</mo><mi>α</mi><mo>−</mo><mi>n</mi></mrow><mrow><mn>2</mn><mi>n</mi></mrow></mfrac></math></span>. Furthermore, we obtained that the solution will converge to the equilibrium <span><math><mo>(</mo><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mi>δ</mi></mrow><mrow><mi>β</mi></mrow></msup></mrow></mfrac><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mi>β</mi></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>,</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mi>δ</mi></mrow></mfrac><msup><mrow><mo>(</mo><mfrac><mrow><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub></mrow><mrow><mi>μ</mi></mrow></mfrac><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mo>)</mo></math></span> with an exponential decay rate in <span><math><msup><mrow><mo>(</mo><msup><mrow><mi>L</mi></mrow><mrow><mo>∞</mo></mrow></msup><mo>(</mo><mi>Ω</mi><mo>)</mo><mo>)</mo></mrow><mrow><mn>3</mn></mrow></msup></math></span>, where <span><math><msub><mrow><mi>r</mi></mrow><mrow><mo>+</mo></mrow></msub><mo>:</mo><mo>=</mo><mi>max</mi><mo></mo><mo>{</mo><mi>r</mi><mo>,</mo><mn>0</mn><mo>}</mo></math></span>.</div></div>\",\"PeriodicalId\":50147,\"journal\":{\"name\":\"Journal of Mathematical Analysis and Applications\",\"volume\":\"547 1\",\"pages\":\"Article 129290\"},\"PeriodicalIF\":1.2000,\"publicationDate\":\"2025-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Mathematical Analysis and Applications\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0022247X2500071X\",\"RegionNum\":3,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2025/1/21 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q1\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Mathematical Analysis and Applications","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022247X2500071X","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/1/21 0:00:00","PubModel":"Epub","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
Nonlinear generation index of bounded solutions in a chemotaxis system with indirect signal, density-suppressed motility and generalized logistic source
In this paper, we study the following chemotaxis-growth system with density-suppressed motility under homogeneous Neumann boundary conditions in a bounded domain with smooth boundary, where , μ, δ, , , and the positive motility function satisfies for all . The main purpose of this paper is to establish the global boundedness and stabilization of classical solutions for such kind of chemotaxis system. More precisely, we showed that if , the system possesses a globally bounded classical solution, and further, if γ also fulfills the additional assumption that is bounded on , then for , the above restriction can be optimized as . Furthermore, we obtained that the solution will converge to the equilibrium with an exponential decay rate in , where .
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