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Spectral instability of peakons for the b-family of Novikov equations 诺维科夫方程 b 族的峰子谱不稳定性
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-25 DOI: 10.1016/j.jde.2024.09.031
Xijun Deng , Stéphane Lafortune
In this paper, we are concerned with a one-parameter family of peakon equations with cubic nonlinearity parametrized by a parameter usually denoted by the letter b. This family is called the “b-Novikov” since it reduces to the integrable Novikov equation in the case b=3. By extending the corresponding linearized operator defined on functions in H1(R) to one defined on weaker functions on L2(R), we prove spectral and linear instability on L2(R) of peakons in the b-Novikov equations for any b. We also consider the stability on H1(R) and show that the peakons are spectrally or linearly stable only in the case b=3.
在本文中,我们关注的是具有立方非线性参数的峰值子方程的一参数族,其参数通常用字母 b 表示。这个族被称为 "b-Novikov",因为它在 b=3 的情况下简化为可积分的 Novikov 方程。通过将定义在 H1(R) 中函数上的相应线性化算子扩展到定义在 L2(R) 上较弱函数上的算子,我们证明了 b-Novikov 方程中任何 b 的峰值子在 L2(R) 上的谱和线性不稳定性。
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引用次数: 0
An Lq(Lp)-regularity theory for parabolic equations with integro-differential operators having low intensity kernels 具有低强度核的积分微分算子抛物方程的 Lq(Lp)- 规则性理论
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.033
Jaehoon Kang , Daehan Park
<div><div>In this article, we present the existence, uniqueness, and regularity of solutions to parabolic equations with non-local operators<span><span><span><math><msub><mrow><mo>∂</mo></mrow><mrow><mi>t</mi></mrow></msub><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>x</mi><mo>)</mo><mo>=</mo><msup><mrow><mi>L</mi></mrow><mrow><mi>a</mi></mrow></msup><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>x</mi><mo>)</mo><mo>+</mo><mi>f</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>x</mi><mo>)</mo><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn></math></span></span></span> in <span><math><msub><mrow><mi>L</mi></mrow><mrow><mi>q</mi></mrow></msub><mo>(</mo><msub><mrow><mi>L</mi></mrow><mrow><mi>p</mi></mrow></msub><mo>)</mo></math></span> spaces. Our spatial operator <span><math><msup><mrow><mi>L</mi></mrow><mrow><mi>a</mi></mrow></msup></math></span> is an integro-differential operator of the form<span><span><span><math><munder><mo>∫</mo><mrow><msup><mrow><mi>R</mi></mrow><mrow><mi>d</mi></mrow></msup></mrow></munder><mrow><mo>(</mo><mi>u</mi><mo>(</mo><mi>x</mi><mo>+</mo><mi>y</mi><mo>)</mo><mo>−</mo><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mi>∇</mi><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>⋅</mo><mi>y</mi><msub><mrow><mn>1</mn></mrow><mrow><mo>|</mo><mi>y</mi><mo>|</mo><mo>≤</mo><mn>1</mn></mrow></msub><mo>)</mo></mrow><mi>a</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>y</mi><mo>)</mo><msub><mrow><mi>j</mi></mrow><mrow><mi>d</mi></mrow></msub><mo>(</mo><mo>|</mo><mi>y</mi><mo>|</mo><mo>)</mo><mi>d</mi><mi>y</mi><mo>.</mo></math></span></span></span> Here, <span><math><mi>a</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>y</mi><mo>)</mo></math></span> is a merely bounded measurable coefficient, and we employed the theory of additive process to handle it. We investigate conditions on <span><math><msub><mrow><mi>j</mi></mrow><mrow><mi>d</mi></mrow></msub><mo>(</mo><mi>r</mi><mo>)</mo></math></span> which yield <span><math><msub><mrow><mi>L</mi></mrow><mrow><mi>q</mi></mrow></msub><mo>(</mo><msub><mrow><mi>L</mi></mrow><mrow><mi>p</mi></mrow></msub><mo>)</mo></math></span>-regularity of solutions. Our assumptions on <span><math><msub><mrow><mi>j</mi></mrow><mrow><mi>d</mi></mrow></msub></math></span> are general so that <span><math><msub><mrow><mi>j</mi></mrow><mrow><mi>d</mi></mrow></msub><mo>(</mo><mi>r</mi><mo>)</mo></math></span> may be comparable to <span><math><msup><mrow><mi>r</mi></mrow><mrow><mo>−</mo><mi>d</mi></mrow></msup><mi>ℓ</mi><mo>(</mo><msup><mrow><mi>r</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mo>)</mo></math></span> for a function <em>ℓ</em> which is slowly varying at infinity. For example, we can take <span><math><mi>ℓ</mi><mo>(</mo><mi>r</mi><mo>)</mo><mo>=</mo><mi>log</mi><mo>⁡</mo><mo>(</mo><mn>1</mn><mo>+</mo><msup><mrow><mi>r</mi></mrow><mrow><mi>α</mi></mrow></msup><mo>)</mo></math></span> or <span><math><mi>ℓ</mi><mo>(</mo><mi>r</mi><mo>)</mo><mo>=</mo><mi>min</mi><mo>⁡</mo><mo>{</mo><msup><mrow><mi>r</mi></mrow><mrow><mi>α<
本文提出了 Lq(Lp) 空间中带有非局部算子∂tu(t,x)=Lau(t,x)+f(t,x),t>0 的抛物方程解的存在性、唯一性和正则性。我们的空间算子 La 是一个形式为∫Rd(u(x+y)-u(x)-∇u(x)⋅y1|y|≤1)a(t,y)jd(|y|)dy 的积分微分算子。这里,a(t,y) 只是一个有界的可测系数,我们用加法过程理论来处理它。我们研究了 jd(r) 的条件,这些条件产生了 Lq(Lp) 规则性解。我们对 jd 的假设是一般性的,因此对于在无穷远处缓慢变化的函数 ℓ 而言,jd(r) 可能与 r-dℓ(r-1)相当。例如,我们可以取 ℓ(r)=log(1+rα) 或 ℓ(r)=min{rα,1} (α∈(0,2)) 。事实上,我们的结果涵盖了傅里叶乘数ψ(ξ)对|ξ|≥1不存在任何缩放条件的算子。此外,我们还给出了一些算子的例子,这些算子无法被之前考虑了ψ的平滑性或缩放条件的结果所涵盖。
{"title":"An Lq(Lp)-regularity theory for parabolic equations with integro-differential operators having low intensity kernels","authors":"Jaehoon Kang ,&nbsp;Daehan Park","doi":"10.1016/j.jde.2024.09.033","DOIUrl":"10.1016/j.jde.2024.09.033","url":null,"abstract":"&lt;div&gt;&lt;div&gt;In this article, we present the existence, uniqueness, and regularity of solutions to parabolic equations with non-local operators&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;∂&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; in &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; spaces. Our spatial operator &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; is an integro-differential operator of the form&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;munder&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/munder&gt;&lt;mrow&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;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&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;mo&gt;−&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&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;mo&gt;⋅&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; Here, &lt;span&gt;&lt;math&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is a merely bounded measurable coefficient, and we employed the theory of additive process to handle it. We investigate conditions on &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; which yield &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;-regularity of solutions. Our assumptions on &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; are general so that &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; may be comparable to &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;mo&gt;−&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; for a function &lt;em&gt;ℓ&lt;/em&gt; which is slowly varying at infinity. For example, we can take &lt;span&gt;&lt;math&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;log&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; or &lt;span&gt;&lt;math&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;min&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142315770","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
Limiting behavior of invariant foliations for SPDEs in singularly perturbed spaces 奇异扰动空间中 SPDEs 不变叶形的极限行为
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.039
Lin Shi
In this paper, we investigate a class of stochastic semilinear parabolic equations subjected to multiplicative noise within singularly perturbed phase spaces. We first establish the existence and smoothness of stable foliations. Then we prove that the long-term behavior of each solution is determined by a solution residing on the pseudo-unstable manifold via a leaf of the stable foliation. Finally, we present the convergence of C1 invariant foliations as the high dimensional region collapse to low dimensional region. In contrast to the convergence of pseudo-unstable manifolds, we introduce a novel technique to address challenges arising from the singularity of the stable term of hyperbolicity in the proof of convergence of stable manifolds and stable foliations as the space collapses.
在本文中,我们研究了一类在奇异扰动相空间内受乘法噪声影响的随机半线性抛物方程。我们首先确定了稳定对折的存在性和平滑性。然后,我们证明每个解的长期行为都是由驻留在伪不稳定流形上的解通过稳定叶子决定的。最后,我们提出了 C1 不变叶形在高维区域向低维区域坍缩时的收敛性。与伪不稳定流形的收敛性不同,我们引入了一种新技术,以解决在证明稳定流形和稳定叶状体在空间塌缩时的收敛性时,双曲线稳定项的奇异性所带来的挑战。
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引用次数: 0
Exponential stability of a diffuse interface model of incompressible two-phase flow with phase variable dependent viscosity and vacuum 具有相变粘度和真空的不可压缩两相流扩散界面模型的指数稳定性
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.036
Yinghua Li, Manrou Xie, Yuanxiang Yan
This paper is concerned with a simplified model for two-phase fluids with diffuse interface. The model couples the nonhomogeneous incompressible Navier-Stokes equations with the Allen-Cahn equation. The viscosity coefficient is allowed to depend both on the phase variable and on the density. Under some smallness assumptions on initial data, the global existence of unique strong solutions to the 3D Cauchy problem and the initial boundary value problem is established. Meanwhile, we obtain the exponential decay-in-time properties of the solutions. Here, the initial vacuum is allowed and no compatibility conditions are required for the initial data via time weighted techniques.
本文涉及一种具有扩散界面的两相流体简化模型。该模型将非均质不可压缩纳维-斯托克斯方程与艾伦-卡恩方程耦合在一起。允许粘度系数同时取决于相变量和密度。在初始数据很小的假设条件下,建立了三维 Cauchy 问题和初始边界值问题的唯一强解的全局存在性。同时,我们还得到了解的时间指数衰减特性。在这里,通过时间加权技术,允许初始真空,且不要求初始数据的相容性条件。
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引用次数: 0
On the periodic solutions of switching scalar dynamical systems 论开关标量动力系统的周期解
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.032
Xuejun Pan , Hongying Shu , Lin Wang , Xiang-Sheng Wang , Jianshe Yu
In this paper, we investigate the existence and stability of periodic solutions of switching dynamical systems consisting of two sub-equations. We first establish a general criterion to determine the stability of periodic solutions; namely, we derive the conditions under which the periodic solution is locally asymptotically stable, globally asymptotically stable, or unstable. Next, we develop general theorems to count the number of periodic solutions and find the basins of attractions for the periodic solutions and the trivial solution, respectively. As applications, we analyze two biological models in recent literature. Our general theorems not only reproduce the existing results in a unified and simpler manner but also lead to new and complete dynamical results including bistability of the periodic solution and the trivial solution. Numerical examples are also given to illustrate our theoretical results.
在本文中,我们研究了由两个子方程组成的切换动力系统的周期解的存在性和稳定性。我们首先建立了确定周期解稳定性的一般标准,即推导出周期解局部渐近稳定、全局渐近稳定或不稳定的条件。接着,我们提出了计算周期解数量的一般定理,并分别找到了周期解和三解的吸引盆地。作为应用,我们分析了近期文献中的两个生物模型。我们的一般定理不仅以统一和更简单的方式重现了现有结果,而且还带来了新的和完整的动力学结果,包括周期解和三元解的双稳态性。我们还给出了数值例子来说明我们的理论结果。
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引用次数: 0
Maslov-type (L,P)-index and subharmonic P-symmetric brake solutions for Hamiltonian systems 哈密尔顿系统的马斯洛夫型(L,P)指数和亚谐波 P 对称制动解
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.037
Duanzhi Zhang , Zhihao Zhao
This paper introduces a novel iteration inequality for the Maslov-type (L,P)-index of iterated symplectic paths. Here, P is a fixed 2n-dimensional symplectic and orthogonal matrix satisfying Pm=I. These advancements in index theory are then applied to investigate the multiplicity of subharmonic solutions in Hamiltonian systems exhibiting dihedral equivariance with period . Notably, a criterion of geometric distinction is established for two subharmonic P-symmetric brake orbits with periods kmτ and lmτ within the set {kmτ|k1 (mod m)}. This criterion is based on a lower bound estimate for the ratio l/k. Specifically, for odd k, the lower bound must be not less than (12dimker(PI)+2)m+1, while for even k, it must be not less than (12dimker(PI)+n+2)m+1.
本文针对迭代交映路径的马斯洛夫型(L,P)指数提出了一种新的迭代不等式。这里,P 是一个固定的 2n 维交映和正交矩阵,满足 Pm=I。指数理论的这些进展随后被应用于研究哈密顿系统中的次谐波解的多重性,该系统表现出周期为 mτ 的二面等差性。值得注意的是,在{kmτ|k≡1 (mod m)}集合内,建立了周期分别为 kmτ 和 lmτ 的两个次谐波 P 对称制动轨道的几何区分标准。这一标准基于 l/k 比率的下限估计值。具体来说,对于奇数 k,下限必须不小于 (12dimker(P-I)+2)m+1,而对于偶数 k,下限必须不小于 (12dimker(P-I)+n+2)m+1。
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引用次数: 0
Stability and convergence of in time approximations of hyperbolic elastodynamics via stepwise minimization 通过逐步最小化实现双曲弹性力学及时近似的稳定性和收敛性
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-24 DOI: 10.1016/j.jde.2024.09.034
Antonín Češík , Sebastian Schwarzacher
We study step-wise time approximations of non-linear hyperbolic initial value problems. The technique used here is a generalization of the minimizing movements method, using two time-scales: one for velocity, the other (potentially much larger) for acceleration. The main applications are from elastodynamics, namely so-called generalized solids, undergoing large deformations. The evolution follows an underlying variational structure exploited by step-wise minimization. We show for a large family of (elastic) energies that the introduced scheme is stable; allowing for non-linearities of highest order. If the highest order can be assumed to be linear, we show that the limit solutions are regular and that the minimizing movements scheme converges with optimal linear rate. Thus this work extends numerical time-step minimization methods to the realm of hyperbolic problems.
我们研究非线性双曲初值问题的分步时间逼近。这里使用的技术是最小化运动法的一般化,使用两个时间尺度:一个用于速度,另一个(可能更大)用于加速度。主要应用于弹性动力学,即发生大变形的所谓广义固体。其演化过程遵循一种潜在的变分结构,并通过逐步最小化的方式加以利用。我们针对大量(弹性)能量证明,引入的方案是稳定的;允许最高阶的非线性。如果可以假定最高阶为线性,我们将证明极限解是有规律的,最小化运动方案将以最佳线性速率收敛。因此,这项工作将数值时间步最小化方法扩展到了双曲问题领域。
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引用次数: 0
Study on the behaviors of rupture solutions for a class of elliptic MEMS equations in R2 R2 中一类椭圆 MEMS 方程的破裂解行为研究
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-23 DOI: 10.1016/j.jde.2024.09.035
Qing Li , Yanyan Zhang
This study examines nonnegative solutions to the problem{Δu=λ|x|αup inR2{0},u(0)=0andu>0 inR2{0}, where λ>0, α>2, and p>0 are constants. The possible asymptotic behaviors of u(x) at |x|=0 and |x|= are classified according to (α,p). In particular, the results show that for some (α,p), u(x) exhibits only “isotropic” behavior at |x|=0 and |x|=. However, in other cases, u(x) may exhibit the “anisotropic” behavior at |x|=0 or |x|=. Furthermore, the relation between the limit at |x|=0 and the limit at |x|= for a global solution is investigated.
本研究探讨了问题{Δu=λ|x|αup inR2∖{0},u(0)=0andu>0 inR2∖{0}的非负解,其中λ>0,α>-2,p>0为常数。根据 (α,p) 对 u(x) 在 |x|=0 和 |x|=∞ 时的可能渐近行为进行了分类。结果特别表明,对于某些 (α,p) 情况,u(x) 只在|x|=0 和 |x|=∞时表现出 "各向同性 "行为。然而,在其他情况下,u(x) 可能会在|x|=0 或 |x|=∞处表现出 "各向异性 "行为。此外,还研究了全局解在 |x|=0 时的极限与 |x|=∞ 时的极限之间的关系。
{"title":"Study on the behaviors of rupture solutions for a class of elliptic MEMS equations in R2","authors":"Qing Li ,&nbsp;Yanyan Zhang","doi":"10.1016/j.jde.2024.09.035","DOIUrl":"10.1016/j.jde.2024.09.035","url":null,"abstract":"<div><div>This study examines nonnegative solutions to the problem<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><mi>Δ</mi><mi>u</mi><mo>=</mo><mfrac><mrow><mi>λ</mi><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>α</mi></mrow></msup></mrow><mrow><msup><mrow><mi>u</mi></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac><mspace></mspace></mtd><mtd><mtext> in</mtext><mspace></mspace><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo><mo>,</mo></mtd></mtr><mtr><mtd><mi>u</mi><mo>(</mo><mn>0</mn><mo>)</mo><mo>=</mo><mn>0</mn><mspace></mspace><mtext>and</mtext><mspace></mspace><mi>u</mi><mo>&gt;</mo><mn>0</mn><mspace></mspace></mtd><mtd><mtext> in</mtext><mspace></mspace><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> where <span><math><mi>λ</mi><mo>&gt;</mo><mn>0</mn></math></span>, <span><math><mi>α</mi><mo>&gt;</mo><mo>−</mo><mn>2</mn></math></span>, and <span><math><mi>p</mi><mo>&gt;</mo><mn>0</mn></math></span> are constants. The possible asymptotic behaviors of <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span> are classified according to <span><math><mo>(</mo><mi>α</mi><mo>,</mo><mi>p</mi><mo>)</mo></math></span>. In particular, the results show that for some <span><math><mo>(</mo><mi>α</mi><mo>,</mo><mi>p</mi><mo>)</mo></math></span>, <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> exhibits only “isotropic” behavior at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span>. However, in other cases, <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> may exhibit the “anisotropic” behavior at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> or <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span>. Furthermore, the relation between the limit at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and the limit at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span> for a global solution is investigated.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142312203","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
Global dynamics for a two-species chemotaxis-competition system with loop and nonlocal kinetics 具有循环和非局部动力学的双物种趋化竞争系统的全局动力学
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-23 DOI: 10.1016/j.jde.2024.09.027
Shuyan Qiu , Li Luo , Xinyu Tu
<div><div>In this paper, we consider the two-species chemotaxis-competition system with loop and nonlocal kinetics<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>u</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>11</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>12</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>w</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>21</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>22</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>z</mi><mo>−</mo><mi>z</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> subject to homogeneous Neumann boundary conditions in a smooth 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>1</mn><mo>)</mo></math></span>, where <span><math><msub><mrow><mi>χ</mi></mrow><mrow><mi>i</mi><mi>j</mi></mrow></msub><mo>></mo><mn>0</mn><mo>(</mo><mi>i</mi><mo>,</mo><mi>j</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></math></span>, <span><math><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>=</mo><mi>u</mi><mrow><mo>(</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mi>u</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>2</mn></mrow></msub><mi>w</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>3</mn></mrow></msub><msub><mrow><mo>∫</mo></mrow><mrow><mi>Ω</mi></mrow></msub><mi>u</mi><mi>d</mi><mi>
本文考虑了具有循环和非局部动力学的双物种趋化-竞争系统{ut=Δu-χ11∇⋅(u∇v)-χ12∇⋅(u∇z)+f1(u,w),x∈Ω,t>;0,0=Δv-v+u+w,x∈Ω,t>0,wt=Δw-χ21∇⋅(w∇v)-χ22∇⋅(w∇z)+f2(u,w),x∈Ω,t>;0,0=Δz-z+u+w,x∈Ω,t>0,在光滑有界域Ω⊂Rn(n≥1)中服从均质 Neumann 边界条件,其中 χij>;0(i,j=1,2),f1(u,w)=u(a0-a1u-a2w-a3∫Ωudx-a4∫Ωwdx),f2(u,w)=w(b0-b1u-b2w-b3∫Ωudx-b4∫Ωwdx),其中 ai,bi>0(i=0,1,2),aj,bj∈R(j=3,4)。研究表明,如果参数满足某些条件,那么相应的初始边界值问题在任何空间维度上都有唯一的全局时间经典解,且该解均匀有界。此外,基于合适能量函数的构造,还考虑了共存和半共存稳态的全局渐近稳定问题。我们的结果概括并改进了之前文献中的一些结果。
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subject to homogeneous Neumann boundary conditions in a smooth bounded domain &lt;span&gt;&lt;math&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;⊂&lt;/mo&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;mo&gt;(&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&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;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;a&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&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;/msub&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142310593","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 the locally self-similar blowup for the generalized SQG equation 论广义 SQG方程的局部自相似膨胀
IF 2.4 2区 数学 Q1 MATHEMATICS Pub Date : 2024-09-23 DOI: 10.1016/j.jde.2024.09.025
Anne Bronzi , Ricardo Guimarães , Cecilia Mondaini
We analyze finite-time blowup scenarios of locally self-similar type for the inviscid generalized surface quasi-geostrophic equation (gSQG) in R2. Under an Lr growth assumption on the self-similar profile and its gradient, we identify appropriate ranges of the self-similar parameter where the profile is either identically zero, and hence blowup cannot occur, or its Lp asymptotic behavior can be characterized, for suitable r,p. Our results extend the work by Xue [38] regarding the SQG equation, and also partially recover the results proved by Cannone and Xue [3] concerning globally self-similar solutions of the gSQG equation.
我们分析了 R2 中不粘性广义表面准地转方程(gSQG)的局部自相似型有限时间炸裂情形。在自相似剖面及其梯度的 Lr 增长假设下,我们确定了自相似参数的适当范围,在这些范围内,对于合适的 r,p,剖面要么为完全相同的零,因此不会发生炸裂,要么可以描述其 Lp 渐近行为。我们的结果扩展了 Xue [38] 关于 SQG 方程的研究,也部分恢复了 Cannone 和 Xue [3] 关于 gSQG 方程全局自相似解的结果。
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引用次数: 0
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Journal of Differential Equations
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