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Global Fujita-Kato solutions for the incompressible Hall-MHD system 不可压缩Hall-MHD系统的全球富士通解决方案
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-19 DOI: 10.1016/j.na.2025.114007
Jin Tan
We show the global-in-time existence and uniqueness of solutions to the 3D incompressible Hall-magnetohydrodynamic (Hall-MHD) system with small initial data in critical Sobolev spaces. Our result works for general physical parameters, thus gives a full answer to the problem proposed by Chae and Lee in the Remark 2 of Chae and Lee (2014). Moreover, considering the so-called 212D flows for the Hall-MHD system (that is 3D flows independent of the vertical variable), we show that under the sole assumption that the initial magnetic field is small in the critical Sobolev space leads to a global unique solvability statement. Comparing with the classical MHD system, the new difficulties of proving such results come from the additional Hall term, which endows the magnetic equation with a quasi-linear character.
研究了临界Sobolev空间中初始数据较小的三维不可压缩霍尔-磁流体动力学(Hall-MHD)系统解的全局存在唯一性。我们的结果适用于一般物理参数,从而完整地回答了Chae和Lee在Chae和Lee(2014)的Remark 2中提出的问题。此外,考虑到所谓的Hall-MHD系统的212D流动(即独立于垂直变量的3D流动),我们表明,在临界Sobolev空间中初始磁场很小的唯一假设下,导致全局唯一可解性陈述。与经典MHD系统相比,证明这些结果的新困难来自于附加的霍尔项,它使磁方程具有拟线性特征。
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引用次数: 0
Weighted Orlicz-Sobolev and variable exponent Morrey regularity for fully nonlinear parabolic PDEs with oblique boundary conditions and applications 斜边界条件下全非线性抛物型偏微分方程的加权Orlicz-Sobolev和变指数Morrey正则性及其应用
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-14 DOI: 10.1016/j.na.2025.114017
Junior da S. Bessa , João Vitor da Silva , Maria N.B. Frederico , Gleydson C. Ricarte
<div><div>In this manuscript, we establish global weighted Orlicz-Sobolev and variable exponent Morrey–Sobolev estimates for viscosity solutions to fully nonlinear parabolic equations subject to oblique boundary conditions on a portion of the boundary, within the following framework: <span><math><mfenced><mrow><mtable><mtr><mtd><mi>F</mi><mrow><mo>(</mo><msup><mrow><mi>D</mi></mrow><mrow><mn>2</mn></mrow></msup><mi>u</mi><mo>,</mo><mi>D</mi><mi>u</mi><mo>,</mo><mi>u</mi><mo>,</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo></mrow><mo>−</mo><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub></mtd><mtd><mo>=</mo></mtd><mtd><mi>f</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo></mrow></mtd><mtd><mtext>in</mtext></mtd><mtd><msub><mrow><mi>Ω</mi></mrow><mrow><mi>T</mi></mrow></msub><mo>,</mo></mtd></mtr><mtr><mtd><mi>β</mi><mi>⋅</mi><mi>D</mi><mi>u</mi><mo>+</mo><mi>γ</mi><mi>u</mi></mtd><mtd><mo>=</mo></mtd><mtd><mi>g</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo></mrow></mtd><mtd><mtext>on</mtext></mtd><mtd><msub><mrow><mi>S</mi></mrow><mrow><mi>T</mi></mrow></msub><mo>,</mo></mtd></mtr><mtr><mtd><mi>u</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo></mrow></mtd><mtd><mo>=</mo></mtd><mtd><mn>0</mn></mtd><mtd><mtext>on</mtext></mtd><mtd><msub><mrow><mi>Ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo></mtd></mtr></mtable></mrow></mfenced></math></span> where <span><math><mrow><msub><mrow><mi>Ω</mi></mrow><mrow><mi>T</mi></mrow></msub><mo>=</mo><mi>Ω</mi><mo>×</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>T</mi><mo>)</mo></mrow></mrow></math></span> denotes the parabolic cylinder with spatial base <span><math><mi>Ω</mi></math></span> (a bounded domain in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span>, <span><math><mrow><mi>n</mi><mo>≥</mo><mn>2</mn></mrow></math></span>) and temporal height <span><math><mrow><mi>T</mi><mo>></mo><mn>0</mn></mrow></math></span>, <span><math><mrow><msub><mrow><mi>S</mi></mrow><mrow><mi>T</mi></mrow></msub><mo>=</mo><mi>∂</mi><mi>Ω</mi><mo>×</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>T</mi><mo>)</mo></mrow></mrow></math></span>, and <span><math><mrow><msub><mrow><mi>Ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><mi>Ω</mi><mo>×</mo><mrow><mo>{</mo><mn>0</mn><mo>}</mo></mrow></mrow></math></span>. Additionally, <span><math><mi>f</mi></math></span> represents the source term of the parabolic equation, while the boundary data are given by <span><math><mi>β</mi></math></span>, <span><math><mi>γ</mi></math></span>, and <span><math><mi>g</mi></math></span>. Our first main result is a global weighted Orlicz–Sobolev estimate for the solution, obtained under asymptotic structural conditions on the differential operator and appropriate assumptions on the boundary data, assuming that the source term belongs to the corresponding weighted Orlicz space. Leveraging these estimates, we demonstrate several applications, including a density result
在本文中,我们在以下框架内建立了部分边界上受倾斜边界条件约束的全非线性抛物方程的粘度解的全局权重Orlicz-Sobolev和变指数Morrey-Sobolev估计:F(D2u,Du,u,x,t)−ut= F(x,t)inΩT,β·Du+γu=g(x,t)onST,u(x,0)=0onΩ0,其中ΩT=Ω×(0, t)表示空间基Ω (Rn, n≥2中的有界域)和时间高度T>;0的抛物线柱体,ST=∂Ω×(0, t), Ω0=Ω×{0}。此外,f表示抛物方程的源项,而边界数据由β, γ和g给出。我们的第一个主要结果是解的全局加权Orlicz - sobolev估计,该估计是在微分算子的渐近结构条件和对边界数据的适当假设下得到的,假设源项属于相应的加权Orlicz空间。利用这些估计,我们展示了几种应用,包括抛物方程基本类中的密度结果,相关障碍问题的正则性结果,以及解决方案的Hessian和时间导数的加权Orlicz-BMO估计。最后,我们通过外推技术推导出问题的可变指数Morrey-Sobolev估计,这是独立的数学兴趣。
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Ricarte","doi":"10.1016/j.na.2025.114017","DOIUrl":"10.1016/j.na.2025.114017","url":null,"abstract":"&lt;div&gt;&lt;div&gt;In this manuscript, we establish global weighted Orlicz-Sobolev and variable exponent Morrey–Sobolev estimates for viscosity solutions to fully nonlinear parabolic equations subject to oblique boundary conditions on a portion of the boundary, within the following framework: &lt;span&gt;&lt;math&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mi&gt;F&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&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;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mtext&gt;in&lt;/mtext&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mi&gt;⋅&lt;/mi&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mtext&gt;on&lt;/mtext&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mtext&gt;on&lt;/mtext&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Ω&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;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;/math&gt;&lt;/span&gt; where &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&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;T&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; denotes the parabolic cylinder with spatial base &lt;span&gt;&lt;math&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; (a bounded domain in &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) and temporal height &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;T&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;, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;Ω&lt;/mi&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;T&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Ω&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;=&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&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;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. Additionally, &lt;span&gt;&lt;math&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; represents the source term of the parabolic equation, while the boundary data are given by &lt;span&gt;&lt;math&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;. Our first main result is a global weighted Orlicz–Sobolev estimate for the solution, obtained under asymptotic structural conditions on the differential operator and appropriate assumptions on the boundary data, assuming that the source term belongs to the corresponding weighted Orlicz space. Leveraging these estimates, we demonstrate several applications, including a density result ","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 114017"},"PeriodicalIF":1.3,"publicationDate":"2025-11-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145520546","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 unique continuation from the edge of a crack with no star-shapedness condition 在没有星形条件的情况下,从裂纹边缘唯一延续的音符
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-12 DOI: 10.1016/j.na.2025.114006
Alessandra De Luca
In the present paper, which aims at representing an improvement of De Luca and Felli (2021), we prove the validity of the strong unique continuation property for solutions to some second order elliptic equations from the edge of a crack via a description of their local behaviour. In particular we relax the star-shapedness condition on the complement of the crack considered in De Luca and Felli (2021) by applying a suitable diffeomorphism which straightens the boundary of the crack before performing an approximation of the fractured domain needed to derive a monotonicity formula
在本文中,旨在表示De Luca和feli(2021)的改进,我们通过描述其局部行为证明了从裂纹边缘开始的一些二阶椭圆方程解的强唯一延拓性质的有效性。特别是,我们放宽了De Luca和feli(2021)中考虑的裂纹补上的星形条件,通过应用合适的微分同态,该微分同态在执行导出单调公式所需的断裂域近似之前使裂纹边界变直
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引用次数: 0
A new mechanism for producing degenerate centers in polynomial differential systems 多项式微分系统产生退化中心的新机制
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-12 DOI: 10.1016/j.na.2025.113981
Jaume Giné , Dmitry I. Sinelshchikov
It has been conjectured that the only mechanisms capable of producing a center – whether degenerate or not – at a singular point of a polynomial differential system are algebraic reducibility and Liouvillian integrability. In this work, we present an example that is algebraically reducible but neither orbitally reversible nor Liouvillian integrable. The construction of this example is based on a recently developed mechanism that establishes a necessary and sufficient condition for the existence of a center.
据推测,能够在多项式微分系统的奇点上产生中心(无论是否退化)的唯一机制是代数可约性和Liouvillian可积性。在这项工作中,我们提出了一个代数上可约,但既不是轨道可逆的,也不是柳维廉可积的例子。这个例子的构造是基于最近开发的一种机制,该机制建立了中心存在的充分必要条件。
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引用次数: 0
Random dynamics and invariant measures for a class of non-Newtonian fluids of differential type on 2D and 3D Poincaré domains 二维和三维庞卡罗区域上一类微分型非牛顿流体的随机动力学和不变测度
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-07 DOI: 10.1016/j.na.2025.114005
Kush Kinra , Fernanda Cipriano
In this article, we consider a class of incompressible stochastic third-grade fluids (non-Newtonian fluids) equations on two- as well as three-dimensional Poincaré domains O (which may be bounded or unbounded). Our aims are to study the well-posedness and asymptotic analysis for the solutions of the underlying system. Firstly, we prove that the underlying system defined on O has a unique weak solution (in the analytic sense) under Dirichlet boundary condition and it also generates random dynamical system Ψ. Secondly, we consider the underlying system on bounded domains. Using the compact Sobolev embedding H1(O)L2(O), we prove the existence of a unique random attractor for the underlying system on bounded domains with external forcing in H1(O). Thirdly, we consider the underlying system on unbounded Poincaré domains with external forcing in L2(O) and show the existence of a unique random attractor. In order to obtain the existence of a unique random attractor on unbounded domains, due to the lack of compact Sobolev embedding H1(O)L2(O), we use the uniform-tail estimates method which helps us to demonstrate the asymptotic compactness of Ψ. Note that due to the presence of several nonlinear terms in the underlying system, we are not able to use the energy equality method to obtain the asymptotic compactness of Ψ in unbounded domains, which makes the analysis of this work in unbounded domains more difficult and interesting. Finally, as a consequence of the existence of random attractors, we address the existence of invariant measures for underlying system. To the best of authors’ knowledge, this is the first work which consider a class of the 2D as well as 3D incompressible stochastic third-grade fluids equations and establish the existence of random attractor in bounded as well as unbounded domains. In addition, this is the first work which address the existence of invariant measures for underlying system on unbounded domains.
在这篇文章中,我们考虑了一类不可压缩的随机三阶流体(非牛顿流体)在二维和三维庞加莱格区域(可能是有界的或无界的)上的方程。我们的目的是研究底层系统解的适定性和渐近分析。首先,我们证明了定义在0上的底层系统在Dirichlet边界条件下具有唯一的弱解(解析意义上的),并生成随机动力系统Ψ。其次,我们考虑了有界域上的底层系统。利用紧凑Sobolev嵌入H1(O)“previous L2(O)”,证明了H−1(O)中具有外强迫的有界域上底层系统存在唯一随机吸引子。第三,我们考虑了L2(O)上具有外强迫的无界poincarcar区域上的基础系统,并证明了一个唯一随机吸引子的存在性。为了得到无界域上唯一随机吸引子的存在性,由于缺乏紧Sobolev嵌入H1(O)“previous L2(O)”,我们使用均匀尾估计方法证明了Ψ的渐近紧性。注意,由于底层系统中存在几个非线性项,我们无法使用能量相等方法来获得Ψ在无界域中的渐近紧性,这使得在无界域中分析这项工作变得更加困难和有趣。最后,作为随机吸引子存在的结果,我们讨论了底层系统不变测度的存在性。据作者所知,这是第一次考虑一类二维和三维不可压缩的随机三级流体方程,并在有界和无界区域中建立随机吸引子的存在性。此外,本文还首次讨论了无界域上底层系统的不变量测度的存在性。
{"title":"Random dynamics and invariant measures for a class of non-Newtonian fluids of differential type on 2D and 3D Poincaré domains","authors":"Kush Kinra ,&nbsp;Fernanda Cipriano","doi":"10.1016/j.na.2025.114005","DOIUrl":"10.1016/j.na.2025.114005","url":null,"abstract":"<div><div>In this article, we consider a class of incompressible stochastic third-grade fluids (non-Newtonian fluids) equations on two- as well as three-dimensional Poincaré domains <span><math><mi>O</mi></math></span> (which may be bounded or unbounded). Our aims are to study the well-posedness and asymptotic analysis for the solutions of the underlying system. Firstly, we prove that the underlying system defined on <span><math><mi>O</mi></math></span> has a unique weak solution (in the analytic sense) under Dirichlet boundary condition and it also generates random dynamical system <span><math><mi>Ψ</mi></math></span>. Secondly, we consider the underlying system on bounded domains. Using the compact Sobolev embedding <span><math><mrow><msup><mrow><mi>H</mi></mrow><mrow><mn>1</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow><mo>↪</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow></mrow></math></span>, we prove the existence of a unique random attractor for the underlying system on bounded domains with external forcing in <span><math><mrow><msup><mrow><mi>H</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow></mrow></math></span>. Thirdly, we consider the underlying system on unbounded Poincaré domains with external forcing in <span><math><mrow><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow></mrow></math></span> and show the existence of a unique random attractor. In order to obtain the existence of a unique random attractor on unbounded domains, due to the lack of compact Sobolev embedding <span><math><mrow><msup><mrow><mi>H</mi></mrow><mrow><mn>1</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow><mo>↪</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mrow><mo>(</mo><mi>O</mi><mo>)</mo></mrow></mrow></math></span>, we use the uniform-tail estimates method which helps us to demonstrate the asymptotic compactness of <span><math><mi>Ψ</mi></math></span>. Note that due to the presence of several nonlinear terms in the underlying system, we are not able to use the energy equality method to obtain the asymptotic compactness of <span><math><mi>Ψ</mi></math></span> in unbounded domains, which makes the analysis of this work in unbounded domains more difficult and interesting. Finally, as a consequence of the existence of random attractors, we address the existence of invariant measures for underlying system. To the best of authors’ knowledge, this is the first work which consider a class of the 2D as well as 3D incompressible stochastic third-grade fluids equations and establish the existence of random attractor in bounded as well as unbounded domains. In addition, this is the first work which address the existence of invariant measures for underlying system on unbounded domains.</div></div>","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 114005"},"PeriodicalIF":1.3,"publicationDate":"2025-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145467936","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 dimension stable spaces of measures 测度的维稳定空间
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-06 DOI: 10.1016/j.na.2025.113997
Daniel Spector , Dmitriy Stolyarov
In this paper, we define spaces of measures DSβ(Rd) with dimensional stability β(0,d). These spaces bridge between Mb(Rd), the space of finite Radon measures, and DSd(Rd)=H1(Rd), the real Hardy space. We show the spaces DSβ(Rd) support Sobolev inequalities for β(0,d], while for any β[0,d] we show that the lower Hausdorff dimension of an element of DSβ(Rd) is at least β.
在本文中,我们定义了维度稳定性β∈(0,d)的测度空间DSβ(Rd)。这些空间连接了有限Radon测度空间Mb(Rd)和实Hardy空间DSd(Rd)=H1(Rd)。我们证明了空间DSβ(Rd)对于β∈(0,d)支持Sobolev不等式,而对于任何β∈[0,d],我们证明了DSβ(Rd)的元素的下Hausdorff维数至少为β。
{"title":"On dimension stable spaces of measures","authors":"Daniel Spector ,&nbsp;Dmitriy Stolyarov","doi":"10.1016/j.na.2025.113997","DOIUrl":"10.1016/j.na.2025.113997","url":null,"abstract":"<div><div>In this paper, we define spaces of measures <span><math><mrow><mi>D</mi><msub><mrow><mi>S</mi></mrow><mrow><mi>β</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow></mrow></math></span> with dimensional stability <span><math><mrow><mi>β</mi><mo>∈</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>d</mi><mo>)</mo></mrow></mrow></math></span>. These spaces bridge between <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mi>b</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow></mrow></math></span>, the space of finite Radon measures, and <span><math><mrow><mi>D</mi><msub><mrow><mi>S</mi></mrow><mrow><mi>d</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow><mo>=</mo><msup><mrow><mi>H</mi></mrow><mrow><mn>1</mn></mrow></msup><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow></mrow></math></span>, the real Hardy space. We show the spaces <span><math><mrow><mi>D</mi><msub><mrow><mi>S</mi></mrow><mrow><mi>β</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow></mrow></math></span> support Sobolev inequalities for <span><math><mrow><mi>β</mi><mo>∈</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>d</mi><mo>]</mo></mrow></mrow></math></span>, while for any <span><math><mrow><mi>β</mi><mo>∈</mo><mrow><mo>[</mo><mn>0</mn><mo>,</mo><mi>d</mi><mo>]</mo></mrow></mrow></math></span> we show that the lower Hausdorff dimension of an element of <span><math><mrow><mi>D</mi><msub><mrow><mi>S</mi></mrow><mrow><mi>β</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></mrow></mrow></math></span> is at least <span><math><mi>β</mi></math></span>.</div></div>","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 113997"},"PeriodicalIF":1.3,"publicationDate":"2025-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145467932","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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
Large global bounded solutions for the parabolic–elliptic Keller–Segel system via a framework of sum-closed frequency sets 基于和闭频率集框架的抛物-椭圆型Keller-Segel系统的大全局有界解
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-05 DOI: 10.1016/j.na.2025.114000
V. Angulo-Castillo , L.C.F. Ferreira , E.J. Villamizar-Roa
This paper addresses the n-dimensional elliptic–parabolic Keller–Segel system by employing a Fourier-based framework. This approach allows to consider a new class of L-initial data for the associated Cauchy problem, which can be arbitrarily large in norm. More specifically, our main result establishes global-in-time well-posedness for initial data belonging to a space of tempered distributions whose Fourier transform is a Radon measure supported on sum-closed frequency sets at a distance δ>0 from the origin. The construction of large solutions can be carried out by taking the distance δ sufficiently large, a feasible condition that can be handled in practice through suitable translations in Fourier variables. The initial class includes, in particular, data of non-decaying type as |x|, as well as periodic and almost periodic functions.
本文采用基于傅里叶的框架讨论了n维椭圆-抛物型Keller-Segel系统。这种方法允许考虑一类新的L∞初始数据的相关柯西问题,它可以是任意大范数。更具体地说,我们的主要结果建立了属于缓和分布空间的初始数据的全局时间适定性,其傅里叶变换是在距离原点δ>;0的和闭频率集上支持的Radon测度。大解的构造可以通过取足够大的距离δ来实现,这是一个可行的条件,可以通过在傅里叶变量中适当的平移来处理。初始类特别包括|x|→∞的非衰减型数据,以及周期函数和概周期函数。
{"title":"Large global bounded solutions for the parabolic–elliptic Keller–Segel system via a framework of sum-closed frequency sets","authors":"V. Angulo-Castillo ,&nbsp;L.C.F. Ferreira ,&nbsp;E.J. Villamizar-Roa","doi":"10.1016/j.na.2025.114000","DOIUrl":"10.1016/j.na.2025.114000","url":null,"abstract":"<div><div>This paper addresses the <span><math><mi>n</mi></math></span>-dimensional elliptic–parabolic Keller–Segel system by employing a Fourier-based framework. This approach allows to consider a new class of <span><math><msup><mrow><mi>L</mi></mrow><mrow><mi>∞</mi></mrow></msup></math></span>-initial data for the associated Cauchy problem, which can be arbitrarily large in norm. More specifically, our main result establishes global-in-time well-posedness for initial data belonging to a space of tempered distributions whose Fourier transform is a Radon measure supported on sum-closed frequency sets at a distance <span><math><mrow><mi>δ</mi><mo>&gt;</mo><mn>0</mn></mrow></math></span> from the origin. The construction of large solutions can be carried out by taking the distance <span><math><mi>δ</mi></math></span> sufficiently large, a feasible condition that can be handled in practice through suitable translations in Fourier variables. The initial class includes, in particular, data of non-decaying type as <span><math><mrow><mo>|</mo><mi>x</mi><mo>|</mo><mo>→</mo><mi>∞</mi><mo>,</mo></mrow></math></span> as well as periodic and almost periodic functions.</div></div>","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 114000"},"PeriodicalIF":1.3,"publicationDate":"2025-11-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145467930","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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
Fully nonlinear parabolic fixed transmission problems 全非线性抛物型固定传输问题
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-05 DOI: 10.1016/j.na.2025.114004
David Jesus , María Soria-Carro
We consider transmission problems for parabolic equations governed by distinct fully nonlinear operators on each side of a time-dependent interface. We prove that if the interface is C1,α, in the parabolic sense, then viscosity solutions are piecewise C1,α up to the interface. As byproducts, we obtain a new ABP–Krylov–Tso estimate, and establish existence, uniqueness, a comparison principle, and regularity results for the flat interface problem.
研究了一类抛物型方程的传输问题,该方程由时变界面两侧不同的完全非线性算子控制。我们证明了如果界面是C1,α,在抛物线意义上,那么粘度解是分段的C1,α直到界面。作为副产物,我们得到了一个新的ABP-Krylov-Tso估计,并建立了平面界面问题的存在性、唯一性、比较原理和正则性结果。
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引用次数: 0
Geometric rigidity for incompatible fields in the multi-well case and an application to strain-gradient plasticity 几何刚度不兼容的字段在多井的情况下,应用应变梯度塑性
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-05 DOI: 10.1016/j.na.2025.113998
Stefano Almi , Dario Reggiani , Francesco Solombrino
We derive a quantitative rigidity estimate for a multiwell problem in nonlinear elasticity with dislocations. Precisely, we show that the L1-distance of a possibly incompatible strain field β from a single well is controlled in terms of the L1-distance from a finite set of wells, of curlβ, and of divβ. As a consequence, we derive a strain-gradient plasticity model as Γ-limit of a nonlinear finite dislocation model, containing a singular perturbation term accounting for the divergence of the strain field. This can also be seen as a generalization of the result of Alicandro et al. (2018) to the case of incompatible vector fields.
本文导出了含位错的非线性弹性多井问题的定量刚度估计。准确地说,我们证明了可能不相容的应变场β到单井的L1 *距离是由到有限井集、curlβ和divβ的L1 *距离来控制的。因此,我们推导了一个非线性有限位错模型的应变梯度塑性模型Γ-limit,该模型包含一个奇异扰动项,用于解释应变场的散度。这也可以看作是Alicandro等人(2018)对不相容向量场的结果的概括。
{"title":"Geometric rigidity for incompatible fields in the multi-well case and an application to strain-gradient plasticity","authors":"Stefano Almi ,&nbsp;Dario Reggiani ,&nbsp;Francesco Solombrino","doi":"10.1016/j.na.2025.113998","DOIUrl":"10.1016/j.na.2025.113998","url":null,"abstract":"<div><div>We derive a quantitative rigidity estimate for a multiwell problem in nonlinear elasticity with dislocations. Precisely, we show that the <span><math><msup><mrow><mi>L</mi></mrow><mrow><msup><mrow><mn>1</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></msup></math></span>-distance of a possibly incompatible strain field <span><math><mi>β</mi></math></span> from a single well is controlled in terms of the <span><math><msup><mrow><mi>L</mi></mrow><mrow><msup><mrow><mn>1</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></msup></math></span>-distance from a finite set of wells, of <span><math><mrow><mi>curl</mi><mi>β</mi></mrow></math></span>, and of <span><math><mrow><mi>div</mi><mi>β</mi></mrow></math></span>. As a consequence, we derive a strain-gradient plasticity model as <span><math><mi>Γ</mi></math></span>-limit of a nonlinear finite dislocation model, containing a singular perturbation term accounting for the divergence of the strain field. This can also be seen as a generalization of the result of Alicandro et al. (2018) to the case of incompatible vector fields.</div></div>","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 113998"},"PeriodicalIF":1.3,"publicationDate":"2025-11-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145467934","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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
Asymptotic behavior of positive solutions for a degenerate logistic equation with mixed local and non-local diffusion 一类具有混合局部和非局部扩散的退化logistic方程正解的渐近性质
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2025-11-05 DOI: 10.1016/j.na.2025.114003
Willian Cintra , Cristian Morales-Rodrigo , Antonio Suárez
In this work, we analyze a stationary degenerate logistic equation with both local and non-local diffusion. Primarily employing bifurcation results, sub- and supersolution methods, and maximum principles, we establish results regarding the existence, non-existence, and uniqueness of positive solutions. Additionally, using appropriate large solutions, we conduct a detailed study of the asymptotic behavior of the solutions with respect to one of the equation’s parameters, showing that the presence of the non-local diffusion can drastically change this pointwise behavior when compared with the local case.
本文分析了一类具有局部扩散和非局部扩散的平稳退化logistic方程。主要利用分岔结果、子解和上解方法以及极大值原理,建立了正解的存在性、不存在性和唯一性的结果。此外,使用适当的大解,我们对解相对于方程参数之一的渐近行为进行了详细的研究,表明与局部情况相比,非局部扩散的存在可以极大地改变这种点态行为。
{"title":"Asymptotic behavior of positive solutions for a degenerate logistic equation with mixed local and non-local diffusion","authors":"Willian Cintra ,&nbsp;Cristian Morales-Rodrigo ,&nbsp;Antonio Suárez","doi":"10.1016/j.na.2025.114003","DOIUrl":"10.1016/j.na.2025.114003","url":null,"abstract":"<div><div>In this work, we analyze a stationary degenerate logistic equation with both local and non-local diffusion. Primarily employing bifurcation results, sub- and supersolution methods, and maximum principles, we establish results regarding the existence, non-existence, and uniqueness of positive solutions. Additionally, using appropriate large solutions, we conduct a detailed study of the asymptotic behavior of the solutions with respect to one of the equation’s parameters, showing that the presence of the non-local diffusion can drastically change this pointwise behavior when compared with the local case.</div></div>","PeriodicalId":49749,"journal":{"name":"Nonlinear Analysis-Theory Methods & Applications","volume":"264 ","pages":"Article 114003"},"PeriodicalIF":1.3,"publicationDate":"2025-11-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145467933","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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
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Nonlinear Analysis-Theory Methods & Applications
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