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Boundedness and large-time behavior in a two-species doubly degenerate diffusion chemotaxis system with logistic proliferation 一类具有logistic扩散的两种双退化扩散趋化系统的有界性和大时行为
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-11-01 DOI: 10.1016/j.nonrwa.2025.104525
Yuting Xiang
<div><div>The two-species doubly degenerate nutrient taxis model with competitive kinetics<span><span><span><math><mtable><mtr><mtd><mrow><mo>{</mo><mtable><mtr><mtd><mrow><mrow></mrow><msub><mi>u</mi><mrow><mn>1</mn><mi>t</mi></mrow></msub></mrow></mtd><mtd><mrow><mo>=</mo><msub><mrow><mo>(</mo><msub><mi>u</mi><mn>1</mn></msub><mi>v</mi><msub><mi>u</mi><mrow><mn>1</mn><mi>x</mi></mrow></msub><mo>)</mo></mrow><mi>x</mi></msub><mo>−</mo><msub><mrow><mo>(</mo><msubsup><mi>u</mi><mn>1</mn><mn>2</mn></msubsup><mi>v</mi><msub><mi>v</mi><mi>x</mi></msub><mo>)</mo></mrow><mi>x</mi></msub><mo>+</mo><msub><mi>μ</mi><mn>1</mn></msub><msub><mi>u</mi><mn>1</mn></msub><mrow><mo>(</mo><mn>1</mn><mo>−</mo><msub><mi>u</mi><mn>1</mn></msub><mo>−</mo><msub><mi>a</mi><mn>1</mn></msub><msub><mi>u</mi><mn>2</mn></msub><mo>)</mo></mrow><mo>,</mo></mrow></mtd><mtd><mrow><mi>x</mi><mo>∈</mo><mstyle><mi>Ω</mi></mstyle><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mrow></mtd></mtr><mtr><mtd><msub><mi>u</mi><mrow><mn>2</mn><mi>t</mi></mrow></msub></mtd><mtd><mrow><mo>=</mo><msub><mrow><mo>(</mo><msub><mi>u</mi><mn>2</mn></msub><mi>v</mi><msub><mi>u</mi><mrow><mn>2</mn><mi>x</mi></mrow></msub><mo>)</mo></mrow><mi>x</mi></msub><mo>−</mo><msub><mrow><mo>(</mo><msubsup><mi>u</mi><mn>2</mn><mn>2</mn></msubsup><mi>v</mi><msub><mi>v</mi><mi>x</mi></msub><mo>)</mo></mrow><mi>x</mi></msub><mo>+</mo><msub><mi>μ</mi><mn>2</mn></msub><msub><mi>u</mi><mn>2</mn></msub><mrow><mo>(</mo><mn>1</mn><mo>−</mo><msub><mi>u</mi><mn>2</mn></msub><mo>−</mo><msub><mi>a</mi><mn>2</mn></msub><msub><mi>u</mi><mn>1</mn></msub><mo>)</mo></mrow><mo>,</mo></mrow></mtd><mtd><mrow><mi>x</mi><mo>∈</mo><mstyle><mi>Ω</mi></mstyle><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mrow></mtd></mtr><mtr><mtd><msub><mi>v</mi><mi>t</mi></msub></mtd><mtd><mrow><mo>=</mo><msub><mi>v</mi><mrow><mi>x</mi><mi>x</mi></mrow></msub><mo>−</mo><mrow><mo>(</mo><msub><mi>u</mi><mn>1</mn></msub><mo>+</mo><msub><mi>u</mi><mn>2</mn></msub><mo>)</mo></mrow><mi>v</mi><mo>,</mo></mrow></mtd><mtd><mrow><mi>x</mi><mo>∈</mo><mstyle><mi>Ω</mi></mstyle><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mrow></mtd></mtr></mtable></mrow></mtd></mtr></mtable></math></span></span></span>is considered under no-flux boundary conditions in an open bounded interval <span><math><mrow><mstyle><mi>Ω</mi></mstyle><mo>⊂</mo><mi>R</mi></mrow></math></span>, where <span><math><mrow><msub><mi>a</mi><mi>i</mi></msub><mo>></mo><mn>0</mn></mrow></math></span> and <span><math><mrow><msub><mi>μ</mi><mi>i</mi></msub><mo>></mo><mn>0</mn></mrow></math></span> for <span><math><mrow><mo>(</mo><mi>i</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></mrow></math></span>. It is shown that for all suitably regular nonnegative initial data <span><math><mrow><mo>(</mo><msub><mi>u</mi><mn>10</mn></msub><mo>,</mo><msub><mi>u</mi><mn>20</mn></msub><mo>,</mo><msub><mi>v</mi><mn>0</mn></msub><mo>)</mo></mrow></math></span>, where <span><math><ms
考虑具有竞争动力学的两种双退化营养趋同模型{u1t=(u1vu1x)x−(u12vvx)x+μ1u1(1−u1−a1u2),x∈Ω,t>0,u2t=(u2vu2x)x−(u22vvx)x+μ2u2(1−u2−a2u1),x∈Ω,t>0,vt=vxx−(u1+u2)v,x∈Ω,t>0,在开放有界区间Ω∧R中的无流量边界条件下,其中(i=1,2)的ai>;0和μi>;0。证明了对于所有适当正则非负初始数据(u10,u20,v0),其中u10和u20为严格正,v0为正,上述系统至少存在一个全局弱解满足以下有界性∥u1(·,t)∥Lp(Ω)+∥u2(·,t)∥Lp(Ω)+∥v(·,t)∥W1,∞(Ω)≤C。此外,通过构造合适的能量泛函,我们建立了上述系统解的大时性,并证明了以下性质:•若a1,a2∈(0,1),则存在一个序列tk→∞,使得L2(Ω)中的全局弱解(u1,u2,v)(·,tk)→(1−a11−a1a2,1−a21−a1a2,0)为k→∞;•若a1≥1>;a2>0,则存在一个序列tk→∞,使得L2(Ω)上的整体弱解(u1,u2,v)(·,tk)→(0,1,0)为k→∞。
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kinetics&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msubsup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msubsup&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msubsup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msubsup&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;is considered under no-flux boundary conditions in an open bounded interval &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. It is shown that for all suitably regular nonnegative initial data &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mn&gt;20&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;span&gt;&lt;math&gt;&lt;ms","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"89 ","pages":"Article 104525"},"PeriodicalIF":1.8,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145418267","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
A note on the logistic damping effect to ensure the global solvability of the chemotaxis system with degenerate signal-dependent motility 关于保证具有退化信号依赖运动的趋化系统全局可解性的logistic阻尼效应的注释
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-10-21 DOI: 10.1016/j.nonrwa.2025.104520
Quanyong Zhao, Jinrong Wang
<div><div>This paper is devoted to investigating the logistic source damping effect of the following model<span><span><span><math><mtable><mtr><mtd><mrow><mo>{</mo><mtable><mtr><mtd><mrow><msub><mi>u</mi><mi>t</mi></msub><mo>=</mo><mi>∇</mi><mo>·</mo><mrow><mo>(</mo><mi>φ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mi>∇</mi><mi>u</mi><mo>)</mo></mrow><mo>−</mo><mi>∇</mi><mo>·</mo><mrow><mo>(</mo><mi>u</mi><mi>χ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mi>∇</mi><mi>v</mi><mo>)</mo></mrow><mo>+</mo><mi>r</mi><mi>u</mi><mo>−</mo><mi>μ</mi><msup><mi>u</mi><mi>α</mi></msup><mo>,</mo></mrow></mtd><mtd><mrow><mi>x</mi><mo>∈</mo><mstyle><mi>Ω</mi></mstyle><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mrow></mtd></mtr><mtr><mtd><mrow><msub><mi>v</mi><mi>t</mi></msub><mo>=</mo><mstyle><mi>Δ</mi></mstyle><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><mi>u</mi><mo>,</mo></mrow></mtd><mtd><mrow><mi>x</mi><mo>∈</mo><mstyle><mi>Ω</mi></mstyle><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mrow></mtd></mtr></mtable></mrow></mtd></mtr></mtable></math></span></span></span>under homogeneous Neumann boundary conditions in a smooth bounded domain <span><math><mrow><mstyle><mi>Ω</mi></mstyle><mo>⊂</mo><msup><mi>R</mi><mi>n</mi></msup></mrow></math></span>, where <span><math><mrow><mi>r</mi><mo>∈</mo><mi>R</mi><mo>,</mo><mi>μ</mi><mo>≥</mo><mn>0</mn></mrow></math></span> and <span><math><mrow><mi>α</mi><mo>></mo><mn>1</mn></mrow></math></span> are constants. For the case <span><math><mrow><mrow><mo>(</mo><mi>φ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow><mo>∈</mo><msup><mrow><mo>[</mo><msup><mi>C</mi><mn>2</mn></msup><mrow><mo>(</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>∞</mi><mo>)</mo></mrow><mo>)</mo></mrow><mo>]</mo></mrow><mn>2</mn></msup><mo>,</mo><mi>φ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>></mo><mn>0</mn><mspace></mspace><mtext>and</mtext><mspace></mspace><mfrac><msup><mrow><mo>|</mo><mi>χ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>|</mo></mrow><mn>2</mn></msup><mrow><mi>φ</mi><mo>(</mo><mi>v</mi><mo>)</mo></mrow></mfrac></mrow></math></span> is bounded on <span><math><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>∞</mi><mo>)</mo></mrow></math></span>, generating the prototypical choice given by <span><math><mrow><mi>φ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>=</mo><msup><mi>v</mi><mrow><mo>−</mo><mi>k</mi></mrow></msup></mrow></math></span> and <span><math><mrow><mi>χ</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>=</mo><mi>k</mi><msup><mi>v</mi><mrow><mo>−</mo><mi>k</mi><mo>−</mo><mn>1</mn></mrow></msup></mrow></math></span> with <span><math><mrow><mi>k</mi><mo>></mo><mn>0</mn></mrow></math></span>, it is shown that even with large initial data, the existence of the global classical solution to the above problem can be achieved when <span><math><mrow><mi>α</mi><mo>></mo><mn>3</mn><mo>−</mo><mfrac><mn>6</mn><mrow><mi>n</mi><mo>+</mo><mn>4</mn></mrow></mfrac></mrow></math></span> with <span><math><mrow
本文研究了光滑有界区域Ω∧Rn中齐次诺伊曼边界条件下模型{ut=∇·(φ(v)∇u) -∇·(uχ(v)∇v)+ru−μuα,x∈Ω,t>0,vt=Δv−v+u,x∈Ω,t>;0的logistic源阻尼效应,其中r∈r,μ≥0和α>;1是常数。对于(φ,χ)∈[C2((0,∞))]2,φ(v)>;0和|χ(v)|2φ(v)在(0,∞)上有界的情况,生成了φ(v)=v−k和χ(v)=kv−k−1在k>;0时给出的原型选择,证明了即使有较大的初始数据,α>;3−6n+4在μ>;0时也能得到上述问题的全局经典解的存在性,这优化了Lv和Wang (Proc. Roy)著作中使用的条件。Soc。爱丁堡教派151(2021)821-841),刘和高(苹果)。数学。左163(2025)109470)。对于奇异原型φ(v)=vk和χ(v)=−kvk−1,也研究了保证经典解全局存在的logistic阻尼强度。
{"title":"A note on the logistic damping effect to ensure the global solvability of the chemotaxis system with degenerate signal-dependent motility","authors":"Quanyong Zhao,&nbsp;Jinrong Wang","doi":"10.1016/j.nonrwa.2025.104520","DOIUrl":"10.1016/j.nonrwa.2025.104520","url":null,"abstract":"&lt;div&gt;&lt;div&gt;This paper is devoted to investigating the logistic source damping effect of the following model&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;φ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;msup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;/msup&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;under homogeneous Neumann boundary conditions in a smooth bounded domain &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mstyle&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; are constants. For the case &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;φ&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msup&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;φ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;and&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mfrac&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msup&gt;&lt;mrow&gt;&lt;mi&gt;φ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; is bounded on &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, generating the prototypical choice given by &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;φ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;msup&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, it is shown that even with large initial data, the existence of the global classical solution to the above problem can be achieved when &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mfrac&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mrow","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"89 ","pages":"Article 104520"},"PeriodicalIF":1.8,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145364267","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Global existence and optimal time-decay rates of the compressible Navier-Stokes-Poisson equations with Cattaneo heat conduction 具有Cattaneo热传导的可压缩Navier-Stokes-Poisson方程的全局存在性和最优时间衰减率
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-11-16 DOI: 10.1016/j.nonrwa.2025.104545
Fei Wu , Yakui Wu
Cattaneo heat conduction law is a hyperbolic type equation describing the finite speed of heat conduction. Compared to the classical Fourier heat conduction law, Cattaneo’s law provides a more accurate description of heat conduction in materials with high thermal conductivity and short time scales. In this paper, we study the global well-posedness and large-time behavior of the compressible Navier-Stokes-Poisson equations with Cattaneo heat conduction, which is from the dynamic of charged particles. We obtain the optimal time-decay rates of the high-order spatial derivatives of the solution. The decay rates of the solution reveal two conclusions: 1. due to the damping structure of Cattaneo’s law, the heat flux decays to the motionless state at a faster time-decay rate compared with velocity and temperature; 2. the decay rate of heat flux is same as that of density, and the latter has a faster decay rate because of the dispersion effect of the electric field. Finally, we also establish the convergence from the compressible Navier-Stokes-Poisson equations with Cattaneo heat conduction to the classical compressible Navier-Stokes-Poisson equations with Fourier heat conduction.
卡塔尼奥热传导定律是描述有限热传导速度的双曲型方程。与经典的傅立叶导热定律相比,Cattaneo定律更准确地描述了高导热性和短时间尺度材料的导热。本文从带电粒子动力学出发,研究了具有Cattaneo热传导的可压缩Navier-Stokes-Poisson方程的全局适定性和大时性。我们得到了解的高阶空间导数的最优时间衰减率。溶液的衰减速率揭示了两个结论:1。由于Cattaneo定律的阻尼结构,热流衰减到静止状态的时间衰减速率比速度和温度更快;2. 热通量的衰减速率与密度的衰减速率相同,但由于电场的色散效应,密度的衰减速率更快。最后,我们还建立了具有Cattaneo热传导的可压缩Navier-Stokes-Poisson方程到具有傅里叶热传导的经典可压缩Navier-Stokes-Poisson方程的收敛性。
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引用次数: 0
Global existence of weak solutions to a cell migration and (de)differentiation model with double haptotaxis in the context of tissue regeneration 在组织再生的背景下,具有双重趋向性的细胞迁移和(去)分化模型的弱解的全局存在
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-10-15 DOI: 10.1016/j.nonrwa.2025.104516
Nishith Mohan, Christina Surulescu
We study a model for the spread and (de)differentiation of mesenchymal stem cells and chondrocytes in a scaffold whose fibers are coated with hyaluron. The chondrocytes produce new extracellular matrix, which, together with hyaluron, serves as a haptotactic cue for the stem cell migration. We prove global existence of weak solutions of the corresponding cross-diffusion system with double haptotaxis.
我们研究了间充质干细胞和软骨细胞在纤维被透明质包裹的支架中的扩散和(去)分化模型。软骨细胞产生新的细胞外基质,其与透明质一起作为干细胞迁移的触致性线索。证明了具有双趋向性的交叉扩散系统弱解的整体存在性。
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引用次数: 0
Global existence and optimal time-decay rates of 3D non-isentropic compressible Navier-Stokes system with potential force 具有位势力的三维非等熵可压缩Navier-Stokes系统的全局存在性和最优时间衰减率
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-11-06 DOI: 10.1016/j.nonrwa.2025.104535
Wenwen Huo , Chao Zhang
This paper concerns the global existence and optimal time-decay rate for the higher-order spatial derivative of classical solutions for the three-dimensional viscous and heat-conductive fluids, which is governed by the compressible Navier-Stokes (CNS) system with an external potential force. We first establish the global existence of the non-isentropic CNS system with potential force when the initial data is a small perturbation near the equilibrium state. Subsequently, we show the upper and lower bounds of the optimal decay rates for the solution and its spatial derivatives based on energy estimate and low-high frequency decomposition.
本文研究了具有外部位力的可压缩Navier-Stokes (CNS)系统控制的三维粘性导热流体经典解的高阶空间导数的全局存在性和最优时间衰减率。在初始数据为接近平衡状态的小扰动时,首先建立了具有势力的非等熵CNS系统的全局存在性。随后,我们给出了基于能量估计和低高频分解的解及其空间导数的最优衰减率的上界和下界。
{"title":"Global existence and optimal time-decay rates of 3D non-isentropic compressible Navier-Stokes system with potential force","authors":"Wenwen Huo ,&nbsp;Chao Zhang","doi":"10.1016/j.nonrwa.2025.104535","DOIUrl":"10.1016/j.nonrwa.2025.104535","url":null,"abstract":"<div><div>This paper concerns the global existence and optimal time-decay rate for the higher-order spatial derivative of classical solutions for the three-dimensional viscous and heat-conductive fluids, which is governed by the compressible Navier-Stokes (CNS) system with an external potential force. We first establish the global existence of the non-isentropic CNS system with potential force when the initial data is a small perturbation near the equilibrium state. Subsequently, we show the upper and lower bounds of the optimal decay rates for the solution and its spatial derivatives based on energy estimate and low-high frequency decomposition.</div></div>","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"89 ","pages":"Article 104535"},"PeriodicalIF":1.8,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145474364","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Global strong solutions for 3-D immiscible and slightly compressible two-phase flow in porous media 多孔介质中三维非混相微可压缩两相流的全局强解
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-11-10 DOI: 10.1016/j.nonrwa.2025.104531
Lei Xu , Mengxue Du
In this paper, we consider the flow of two-phase slightly compressible and immiscible fluids in porous media. We focus on the case where the densities of phases follow exponential laws with small compressibility factors, the absolute permeability is linked to the porosity via a Kozeny-Carman relation, and source terms account for realistic injection and production rates. Under some realistic hypotheses based on the data, we establish the local existence and uniqueness of strong solutions for the regularized three-dimensional system. We further show that the solution is global under small assumptions for the system without source terms. This is the first high-dimensional result of the strong solution without any symmetric assumptions for immiscible two-phase flow systems in porous media.
本文考虑两相微可压缩非混相流体在多孔介质中的流动。我们关注的是这样的情况:相密度遵循指数定律,压缩系数较小,绝对渗透率通过Kozeny-Carman关系与孔隙度联系起来,源项考虑了实际的注入和生产速度。在一些基于数据的现实假设下,我们建立了正则化三维系统强解的局部存在唯一性。我们进一步证明,对于没有源项的系统,在较小的假设下,解是全局的。这是对多孔介质中非混相两相流系统,在没有任何对称假设的情况下,首次得到强溶液的高维结果。
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引用次数: 0
Spatial profiles of a diffusion-advection epidemic model with saturated incidence mechanism and birth-death effect 具有饱和发病机制和生-死效应的扩散-平流流行病模型的空间剖面
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-10-28 DOI: 10.1016/j.nonrwa.2025.104524
Xiaodan Chen, Renhao Cui
In this paper, we are concerned with a diffusion-advection SIS (susceptible-infected-susceptible) epidemic model with saturated incidence mechanism and birth-death effect. The basic reproduction number R0 has been derived through a variational expression and determined the threshold dynamics. We mainly investigate spatial profiles of endemic equilibrium with respect to large advection, small dispersal of susceptible/infected individuals and large saturation. These results may offer some prospective applications on disease control and prediction.
本文研究了具有饱和发病机制和生-死效应的扩散-平流SIS(易感-感染-易感)流行病模型。通过变分表达式导出了基本繁殖数R0,并确定了阈值动态。我们主要研究了大平流、小扩散和大饱和情况下地方性平衡的空间分布。这些结果可能在疾病控制和预测方面具有一定的应用前景。
{"title":"Spatial profiles of a diffusion-advection epidemic model with saturated incidence mechanism and birth-death effect","authors":"Xiaodan Chen,&nbsp;Renhao Cui","doi":"10.1016/j.nonrwa.2025.104524","DOIUrl":"10.1016/j.nonrwa.2025.104524","url":null,"abstract":"<div><div>In this paper, we are concerned with a diffusion-advection SIS (susceptible-infected-susceptible) epidemic model with saturated incidence mechanism and birth-death effect. The basic reproduction number <span><math><msub><mi>R</mi><mn>0</mn></msub></math></span> has been derived through a variational expression and determined the threshold dynamics. We mainly investigate spatial profiles of endemic equilibrium with respect to large advection, small dispersal of susceptible/infected individuals and large saturation. These results may offer some prospective applications on disease control and prediction.</div></div>","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"89 ","pages":"Article 104524"},"PeriodicalIF":1.8,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145424894","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Spreading speeds for a Lotva-Volterra competition system with advection in a periodic habitat 周期性栖息地中具有平流的Lotva-Volterra竞争系统的传播速度
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-11-05 DOI: 10.1016/j.nonrwa.2025.104528
Hong-Jie Wu, Bang-Sheng Han, Hong-Lei Wei, Yinghui Yang
The study investigates pulsating wave speeds in an advective two-species competition-diffusion system under periodic environments. Recent studies have confirmed the existence and characterized the qualitative dynamics of pulsating waves. In this paper, we determine pulsating wave speed’s signs with identical diffusion rates and characterize invasion dynamics of competing species in heterogeneous environments by comparing the reactions and competitions. Specifically, we first establish a criterion for zero-speed waves and derive sufficient conditions for strictly positive or negative speeds. Our framework extends previous studies (e.g., Ding and Liang, Math. Ann. 385 (2023), 1–36) by considering functional representation of periodic steady-state solutions and explicit inclusion of advection effects and extends (e.g., Du et al., Z. Angew. Math. Phys. 71 (2020), 27 pp.) by further considering the sign of the pulsating wave speed, determining the long-time behavior of two strongly competing species. Crucially, the presence of the advection term indeed exerts a certain influence on the long-time behavior of two strongly competing species: From the perspective of the proof process, the appearance of the advection term increased the difficulty and complexity of proving Lemmas 2.3 and 3.1; from the result perspective, the advection term necessitates specific structural conditions for definitive speed determination. These findings advance understanding of pattern selection mechanisms in flow-driven ecological systems.
研究了周期环境下平流两种竞争扩散系统的脉动波速度。近年来的研究证实了脉动波的存在,并定性地描述了脉动波的动力学特性。本文确定了具有相同扩散速率的脉动波速符号,并通过比较反应和竞争来表征异质环境中竞争物种的入侵动力学。具体地说,我们首先建立了零速度波的判据,并推导了严格正或负速度的充分条件。我们的框架扩展了以前的研究(例如,Ding和Liang, Math。Ann. 385(2023), 1-36)通过考虑周期稳态解的函数表示和明确包含平流效应和扩展(例如,Du等人,Z. Angew。数学。物理71(2020),27页)通过进一步考虑脉动波速度的标志,确定两个强烈竞争物种的长期行为。至关重要的是,平流项的存在确实对两个强竞争物种的长期行为产生了一定的影响:从证明过程来看,平流项的出现增加了证明引理2.3和3.1的难度和复杂性;从结果的角度来看,平流项需要特定的结构条件才能确定最终的速度。这些发现促进了对流量驱动型生态系统模式选择机制的理解。
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引用次数: 0
Time-delayed generalized Korteweg–de Vries-Burgers equation: Well-posedness and exponential decay 时滞广义Korteweg-de Vries-Burgers方程:适定性和指数衰减
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-10-21 DOI: 10.1016/j.nonrwa.2025.104519
Ibtissam Issa, Cristina Pignotti
This study explores the generalized Korteweg-de Vries-Burgers equation incorporating delay feedback and a damping term. Using semigroup arguments and Lyapunov functional techniques, we establish the existence of a global solution when the exponent of the nonlinear term satisfies some growth conditions. Furthermore, we prove exponential stability estimates under suitable assumptions: first in the case of a positive damping coefficient, then within a more comprehensive framework, accommodating sign changes in both coefficients, i.e. for the damping and the delay feedback. In both cases, we adopt refined conditions on the delay feedback’s coefficient, extending and enhancing existing results in the literature. In particular, our conditions are independent of the time delay size.
本文研究了包含延迟反馈和阻尼项的广义Korteweg-de Vries-Burgers方程。利用半群参数和Lyapunov泛函技术,建立了当非线性项的指数满足某些增长条件时全局解的存在性。此外,我们在适当的假设下证明了指数稳定性估计:首先在正阻尼系数的情况下,然后在更全面的框架内,容纳两个系数的符号变化,即对于阻尼和延迟反馈。在这两种情况下,我们对延迟反馈系数采用了改进的条件,扩展和增强了文献中已有的结果。特别是,我们的条件与时间延迟大小无关。
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引用次数: 0
Singularities of solutions to the non-Newtonian polytropic filtration 非牛顿多向过滤解的奇异性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-06-01 Epub Date: 2025-10-14 DOI: 10.1016/j.nonrwa.2025.104518
Meiling Zhou, Liangwei Wang, Jingxue Yin, Can Lu
In this paper, we study the non-Newtonian polytropic filtration equation utdiv(|um|p2um)=0 with a positive initial data on a smooth bounded domain ΩRn for n3, where 0<m<1, 2<p<1+1m, and in particular p<n(m+1)1+mn. To investigate the regularity of solutions to the Dirichlet problem for this equation when the initial data exhibit a singularity of the form u0(x)A|x|γ for xΩ{0} with A>0 and γ>0, we introduce a linear diffusion term in the regularization process. This addition ensures that the equation remains uniformly parabolic, thereby satisfying both the maximum principle and the comparison principle. The desired results are obtained provided that the coefficient of this regularization term converges to zero in the norm of the appropriate function space. This paper shows that the behavior of the solution depends critically on the value of the exponent γ in the initial data, leading to the following distinct cases: finite-time boundedness, infinite-time boundedness, singular stabilization, and infinite-time blow-up.
本文研究了光滑有界域Ω∧Rn上具有正初始数据的非牛顿多向滤波方程ut−div(|∇um|p−2∇um)=0,其中n≥3,0<m< 1,2 <p<1+1m,特别是p<;n(m+1)1+mn。为了研究该方程的Dirichlet问题解的正则性,当初始数据表现为形式为u0(x) ~ a |x|−γ的奇点时,对于x∈Ω∈{0},具有a >;0和γ>;0,我们在正则化过程中引入线性扩散项。这一补充保证了方程保持一致抛物,从而同时满足极大值原理和比较原理。当正则化项的系数在适当的函数空间范数内收敛于零时,得到了期望的结果。本文证明了解的行为严重依赖于初始数据中指数γ的值,从而导致以下不同的情况:有限时间有界性,无限时间有界性,奇异稳定和无限时间爆破。
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引用次数: 0
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Nonlinear Analysis-Real World Applications
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