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Dynamic bifurcation of nonautonomous evolution equations under Landesman–Lazer condition with cohomology methods 兰德斯曼-拉泽尔条件下非自治演化方程的动态分岔与同调方法
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-10-05 DOI: 10.1016/j.nonrwa.2024.104228
Chunqiu Li, Jintao Wang
In this article we study the dynamic bifurcation of nonautonomous evolution equations by using cohomology methods. First, we construct a homotopy equivalence relation between the nonautonomous system and a product flow. Then, we slightly extend some continuation theorems on bifurcations for autonomous equations, and prove some new cohomology consequences on the reduced singular groups. Based on this homotopy equivalence relation and these conclusions, we establish some typical results on the dynamic bifurcation from infinity of the abstract nonautonomous evolution equation. Finally, we consider the parabolic equation utΔu=λu+f(x,u)+g(x,t) associated with the Dirichlet boundary condition, where f(x,u) satisfies the appropriate Landesman–Lazer type condition. Some new results on the dynamical behaviors of this equation near resonance of the equation are derived.
本文利用同调方法研究了非自治演化方程的动态分岔。首先,我们构建了非自治系统与乘积流之间的同调等价关系。然后,我们略微扩展了一些关于自主方程分岔的延续定理,并证明了一些关于还原奇异群的新同调后果。基于这种同调等价关系和这些结论,我们建立了抽象非自治演化方程的无穷动态分岔的一些典型结果。最后,我们考虑了与迪里夏特边界条件相关的抛物方程 ut-Δu=λu+f(x,u)+g(x,t) ,其中 f(x,u) 满足适当的 Landesman-Lazer 类型条件。推导出了该方程在共振附近的动力学行为的一些新结果。
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引用次数: 0
Local Lipschitz continuity for energy integrals with slow growth and lower order terms 具有缓慢增长和低阶项的能量积分的局部 Lipschitz 连续性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-10-03 DOI: 10.1016/j.nonrwa.2024.104224
Michela Eleuteri , Stefania Perrotta , Giulia Treu
We consider integral functionals with slow growth and explicit dependence on u of the Lagrangian; this includes many relevant examples as, for instance, in elastoplastic torsion problems or in image restoration problems. Our aim is to prove that the local minimizers are locally Lipschitz continuous. The proof makes use of recent results concerning the Bounded Slope Conditions.
我们考虑的是增长缓慢且明确依赖于拉格朗日 u 的积分函数;这包括许多相关的例子,例如弹塑性扭转问题或图像复原问题。我们的目的是证明局部最小值是局部 Lipschitz 连续的。该证明利用了有关有界斜率条件的最新成果。
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引用次数: 0
New generalization of non-autonomous Bernfeld–Haddock conjecture and its proof 非自治伯恩费尔德-哈道克猜想的新概括及其证明
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-10-01 DOI: 10.1016/j.nonrwa.2024.104226
Chuangxia Huang , Xiaodan Ding
In this paper, the famous Bernfeld–Haddock conjecture is generalized to a broader form combining with a class of non-autonomous delay differential equations. With the help of differential inequality technique and Dini derivative theory, it is proved that each solution of the addressed equations has boundedness and tends to a constant without requiring the delay feedback function to be strictly increasing, which greatly refines and extends the corresponding results in the existing literature. In particular, an explanatory example is performed to substantiate the obtained analytical findings.
本文将著名的伯恩费尔德-哈多克猜想推广到更广泛的形式,并与一类非自治延迟微分方程相结合。借助微分不等式技术和迪尼导数理论,证明了所涉及方程的每个解都有界且趋于常数,而不要求延迟反馈函数严格递增,这极大地完善和扩展了现有文献中的相应结果。特别是,通过一个解释性实例来证实所获得的分析结果。
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引用次数: 0
Bifurcation and dynamics of periodic solutions of MEMS model with squeeze film damping 带挤压膜阻尼的微机电系统模型周期解的分岔与动力学
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-27 DOI: 10.1016/j.nonrwa.2024.104229
Shiping Lu , Xingchen Yu , Zhuomo An
<div><div>In this paper, we study the oscillations of an idealized mass–spring model of micro-electro-mechanical system (MEMS) with squeeze film damping. The model consists of two parallel electrodes separated by a gap <span><math><mi>d</mi></math></span>: one of them is fixed, and another one is movable and attached to a linear spring with stiffness coefficient <span><math><mrow><mi>k</mi><mo>></mo><mn>0</mn></mrow></math></span>. The oscillation, under the influence of AC–DC voltage <span><math><mrow><mi>V</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>=</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>d</mi><mi>c</mi></mrow></msub><mo>+</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>a</mi><mi>c</mi></mrow></msub><mo>cos</mo><mfrac><mrow><mn>2</mn><mi>π</mi></mrow><mrow><mi>T</mi></mrow></mfrac><mi>t</mi></mrow></math></span>, is ruled by the following singular differential equation <span><span><span><math><mrow><mi>m</mi><msup><mrow><mi>y</mi></mrow><mrow><mo>′</mo><mo>′</mo></mrow></msup><mo>+</mo><mrow><mo>[</mo><mrow><mfrac><mrow><mi>A</mi></mrow><mrow><msup><mrow><mrow><mo>(</mo><mi>d</mi><mo>−</mo><mi>y</mi><mo>)</mo></mrow></mrow><mrow><mn>3</mn></mrow></msup></mrow></mfrac><mo>+</mo><mfrac><mrow><mi>A</mi></mrow><mrow><mi>d</mi><mo>−</mo><mi>y</mi></mrow></mfrac></mrow><mo>]</mo></mrow><msup><mrow><mi>y</mi></mrow><mrow><mo>′</mo></mrow></msup><mo>+</mo><mi>k</mi><mi>y</mi><mo>=</mo><mfrac><mrow><msub><mrow><mi>θ</mi></mrow><mrow><mn>0</mn></mrow></msub><mi>A</mi></mrow><mrow><mn>2</mn></mrow></mfrac><mfrac><mrow><msup><mrow><mi>V</mi></mrow><mrow><mn>2</mn></mrow></msup><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow><mrow><msup><mrow><mrow><mo>(</mo><mi>d</mi><mo>−</mo><mi>y</mi><mo>)</mo></mrow></mrow><mrow><mn>2</mn></mrow></msup></mrow></mfrac><mo>.</mo></mrow></math></span></span></span>Here, <span><math><mi>y</mi></math></span> is the vertical displacement of the moving plate (<span><math><mi>y</mi></math></span> is always assumed to be less than <span><math><mi>d</mi></math></span>), <span><math><mrow><mi>m</mi><mo>></mo><mn>0</mn></mrow></math></span> is its mass, <span><math><mrow><mi>A</mi><mo>></mo><mn>0</mn></mrow></math></span> is the electrode area, and <span><math><mrow><msub><mrow><mi>θ</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>></mo><mn>0</mn></mrow></math></span> is the absolute dielectric constant of vacuum. Taking <span><math><mi>d</mi></math></span> as the parameter, we show the existence of saddle–node bifurcation of <span><math><mi>T</mi></math></span>-periodic solutions to the equation in the parameter space. This answers, from certain point of view, the open problem proposed by Torres in his monograph, see Torres (2015, Open Problem 2.1, p. 18). Further, we prove that the equation has exactly two classes of <span><math><mi>T</mi></math></span>-periodic solutions: as <span><math><mi>d</mi></math></span> tends to <span><math><mrow><mo>+</mo><mi>∞</mi></mrow></math></span>, one of them uniformly tends t
本文研究了具有挤压膜阻尼的微机电系统(MEMS)理想化质量弹簧模型的振荡。该模型由两个平行电极组成,两电极之间有间隙 d:其中一个固定,另一个可移动,并连接到刚度系数为 k>0 的线性弹簧上。在交直流电压 V(t)=vdc+vaccos2πTt 的影响下,振荡受以下奇异微分方程 my′′+[A(d-y)3+Ad-y]y′+ky=θ0A2V2(t)(d-y)2 的支配。这里,y 是移动板的垂直位移(y 始终假定小于 d),m>0 是移动板的质量,A>0 是电极面积,θ0>0 是真空的绝对介电常数。以 d 为参数,我们证明了方程在参数空间中存在 T 周期解的鞍节点分岔。这从某种角度回答了托雷斯在其专著中提出的开放问题,见托雷斯(2015,开放问题 2.1,第 18 页)。此外,我们还证明了方程正好有两类 T 周期解:当 d 趋于 +∞ 时,其中一类以 d 的速率均匀地趋于 +∞,而第二类的最小值趋于或越过 0。
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The oscillation, under the influence of AC–DC voltage &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;cos&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;π&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, is ruled by the following singular differential equation &lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;′&lt;/mo&gt;&lt;mo&gt;′&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;′&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;θ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;Here, &lt;span&gt;&lt;math&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is the vertical displacement of the moving plate (&lt;span&gt;&lt;math&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is always assumed to be less than &lt;span&gt;&lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;), &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;m&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; is its mass, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;A&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; is the electrode area, and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;θ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&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; is the absolute dielectric constant of vacuum. Taking &lt;span&gt;&lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; as the parameter, we show the existence of saddle–node bifurcation of &lt;span&gt;&lt;math&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;-periodic solutions to the equation in the parameter space. This answers, from certain point of view, the open problem proposed by Torres in his monograph, see Torres (2015, Open Problem 2.1, p. 18). Further, we prove that the equation has exactly two classes of &lt;span&gt;&lt;math&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;-periodic solutions: as &lt;span&gt;&lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; tends to &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, one of them uniformly tends t","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"81 ","pages":"Article 104229"},"PeriodicalIF":1.8,"publicationDate":"2024-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142328262","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
On a planar equation involving (2,q)-Laplacian with zero mass and Trudinger–Moser nonlinearity 关于涉及零质量和特鲁丁格-莫泽非线性的 (2,q)- 拉普拉斯平面方程
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-25 DOI: 10.1016/j.nonrwa.2024.104227
J.A. Cardoso , J.C. de Albuquerque , J. Carvalho , G.M. Figueiredo
In this work, we study existence of positive solutions to a class of (2,q)-equations in the zero mass case in R2. We establish a weighted Sobolev embedding and we introduce a new Trudinger–Moser type inequality. Moreover, since we work on a suitable radial Sobolev space, we prove an appropriate version of the well-known Symmetric Criticality Principle by Palais. Finally, we study regularity of solutions applying Moser iteration scheme.
在这项工作中,我们研究了 R2 中零质量情况下一类 (2,q) -方程正解的存在性。我们建立了一个加权索波列夫嵌入,并引入了一个新的特鲁丁格-莫泽式不等式。此外,由于我们在合适的径向索波列夫空间上工作,我们证明了帕莱斯著名的对称临界原理的适当版本。最后,我们研究了应用 Moser 迭代方案求解的正则性。
{"title":"On a planar equation involving (2,q)-Laplacian with zero mass and Trudinger–Moser nonlinearity","authors":"J.A. Cardoso ,&nbsp;J.C. de Albuquerque ,&nbsp;J. Carvalho ,&nbsp;G.M. Figueiredo","doi":"10.1016/j.nonrwa.2024.104227","DOIUrl":"10.1016/j.nonrwa.2024.104227","url":null,"abstract":"<div><div>In this work, we study existence of positive solutions to a class of <span><math><mrow><mo>(</mo><mn>2</mn><mo>,</mo><mi>q</mi><mo>)</mo></mrow></math></span>-equations in the zero mass case in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span>. We establish a weighted Sobolev embedding and we introduce a new Trudinger–Moser type inequality. Moreover, since we work on a suitable radial Sobolev space, we prove an appropriate version of the well-known Symmetric Criticality Principle by Palais. Finally, we study regularity of solutions applying Moser iteration scheme.</div></div>","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"81 ","pages":"Article 104227"},"PeriodicalIF":1.8,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142318795","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
Singular non-autonomous (p,q)-equations with competing nonlinearities 具有竞争非线性的奇异非自治 (p,q) -方程
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-23 DOI: 10.1016/j.nonrwa.2024.104225
Nikolaos S. Papageorgiou , Dongdong Qin , Vicenţiu D. Rădulescu
We consider a parametric non-autonomous (p,q)-equation with a singular term and competing nonlinearities, a parametric concave term and a Carathéodory perturbation. We consider the cases where the perturbation is (p1)-linear and where it is (p1)-superlinear (but without the use of the Ambrosetti–Rabinowitz condition). We prove an existence and multiplicity result which is global in the parameter λ>0 (a bifurcation type result). Also, we show the existence of a smallest positive solution and show that it is strictly increasing as a function of the parameter. Finally, we examine the set of positive solutions as a function of the parameter (solution multifunction). First, we show that the solution set is compact in C01(Ω̄) and then we show that the solution multifunction is Vietoris continuous and also Hausdorff continuous as a multifunction of the parameter.
我们考虑的是一个参数非自治 (p,q) -方程,它包含一个奇异项和相互竞争的非线性、一个参数凹项和一个卡拉瑟奥多里扰动。我们考虑了扰动为 (p-1)- 线性和 (p-1)- 超线性(但不使用 Ambrosetti-Rabinowitz 条件)的情况。我们证明了参数 λ>0 全局性的存在性和多重性结果(分岔类型结果)。此外,我们还证明了一个最小正解的存在,并证明它作为参数的函数是严格递增的。最后,我们研究了作为参数函数的正解集(解的多重函数)。首先,我们证明解集在 C01(Ω̄) 中是紧凑的,然后我们证明解的多重函数是 Vietoris 连续的,并且作为参数的多重函数也是 Hausdorff 连续的。
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引用次数: 0
Stability of inertial manifolds for semilinear parabolic equations under Lipschitz perturbations 半线性抛物方程的惯性流形在 Lipschitz 摄动下的稳定性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-23 DOI: 10.1016/j.nonrwa.2024.104219
Jihoon Lee , Thanhnguyen Nguyen
In this paper we study the stability and continuity of inertial manifolds for semilinear parabolic equations. More precisely, we prove the continuity of inertial manifolds and the Gromov–Hausdorff stability of dynamical systems on inertial manifolds for reaction diffusion equations under Lipschitz perturbations of the domain and equation, using a nontrivial generalization of ODE approach discussed in Romanov (1994).
本文研究了半线性抛物方程惯性流形的稳定性和连续性。更确切地说,我们利用 Romanov (1994) 中讨论的 ODE 方法的非微观概括,证明了惯性流形的连续性以及反应扩散方程惯性流形上动力系统在域和方程的 Lipschitz 摄动下的 Gromov-Hausdorff 稳定性。
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引用次数: 0
Existence of periodic and solitary waves of a Boussinesq equation under perturbations 扰动下布西内斯克方程周期波和孤波的存在性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-19 DOI: 10.1016/j.nonrwa.2024.104223
Minzhi Wei , Feiting Fan , Xingwu Chen

In this paper, we consider a Boussinesq equation containing weak backward diffusion, delay in the convection term, dissipation and Marangoni effect. By applying geometric singular perturbation theory, a locally invariant manifold diffeomorphic to the critical manifold is established. For Boussinesq equation with delay and weak backward diffusion, the monotonicity of ratio of Abelian integrals is analyzed by utilizing the Picard–Fuchs equation. The conditions on existence of a unique periodic wave and solitary waves are obtained as well as the bound of wave speed. For Boussinesq equation with weak backward diffusion, dissipation and Marangoni effect, the corresponding Melnikov function containing three generic elements is given. The parametric conditions on existence of a unique and two periodic waves are derived respectively. Furthermore, the existence of a unique solitary wave is proved under some parametric conditions.

在本文中,我们考虑了一个包含弱后向扩散、对流项延迟、耗散和马兰戈尼效应的布森斯克方程。通过应用几何奇异扰动理论,建立了与临界流形同构的局部不变流形。对于具有延迟和弱后向扩散的布森斯克方程,利用皮卡尔-富克斯方程分析了阿贝尔积分比率的单调性。获得了唯一周期波和孤波的存在条件以及波速约束。对于具有弱后向扩散、耗散和马兰戈尼效应的布森斯克方程,给出了包含三个一般元素的相应梅利尼科夫函数。分别导出了唯一周期波和两个周期波存在的参数条件。此外,还在一些参数条件下证明了唯一孤波的存在。
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引用次数: 0
Cocycles for equations with infinite delay and hyperbolicity 具有无限延迟和双曲性的方程的循环
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-17 DOI: 10.1016/j.nonrwa.2024.104221
Luís Barreira , Matheus G.C. Cunha , Claudia Valls

We show that the hyperbolicity of a linear delay-difference equation with infinite delay, expressed in terms of the existence of an exponential dichotomy, can be completely characterized by the hyperbolicity of a linear cocycle obtained from the solutions of the equation. As an application of this characterization, we obtain several consequences: the extension of hyperbolicity to all equations in the invariant hull; the robustness of the existence of hyperbolicity for all equations in this hull under sufficiently small linear perturbations; the equality of all spectra in the invariant hull; and a characterization of hyperbolicity for all equations in the invariant hull in terms of an admissibility property taking bounded perturbations to bounded solutions.

我们证明,用指数二分法的存在性来表示具有无限延迟的线性延迟-差分方程的双曲性,完全可以用从方程的解中得到的线性环的双曲性来表征。作为对这一特征的应用,我们得到了几个结果:将双曲性扩展到不变簇中的所有方程;在足够小的线性扰动下,不变簇中所有方程的双曲性存在的稳健性;不变簇中所有谱的相等性;以及从有界扰动到有界解的可接受性特征来描述不变簇中所有方程的双曲性。
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引用次数: 0
On the global well-posedness for the incompressible four-component chemotaxis-Navier–Stokes equations with gradient-dependent flux limitation in R2 关于 R2 中具有梯度通量限制的不可压缩四成分趋化-纳维尔-斯托克斯方程的全局良好拟合问题
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-09-17 DOI: 10.1016/j.nonrwa.2024.104222
He Bao, Yaoning Jia, Qian Zhang

We consider the four-component chemotaxis-Navier–Stokes system in R2: nt+un=Δn(nf(|c|2)c)nm,ct+uc=Δcc+m,mt+um=Δmnm,ut+(u)u+P=Δu+(n+m)ϕ,u=0.Utilizing the Fourier localization technique alongside the inherent structure of the equations, we achieve global well-posedness for a class of rough initial data in the context of the 2D incompressible four-component chemotaxis-Navier–Stokes equations with gradient-dependent flux limitation f(ζ)=Kf(1+ζ)α2 for α>0.

我们考虑 R2 中的四分量化合-纳维尔-斯托克斯系统:nt+u⋅∇n=Δn-∇⋅(nf(|∇c|2)∇c)-nm,ct+u⋅∇c=Δc-c+m,mt+u⋅∇m=Δm-nm,ut+(u⋅∇)u+∇P=Δu+(n+m)∇j,∇⋅u=0。利用傅立叶局部化技术和方程的固有结构,我们在二维不可压缩的四分量趋化-纳维尔-斯托克斯方程的背景下,对一类粗糙初始数据实现了全局良好求解,该方程具有梯度依赖通量限制 f(ζ)=Kf⋅(1+ζ)-α2 for α>0。
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引用次数: 0
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Nonlinear Analysis-Real World Applications
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