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An improved version of a spectral inequality by Payne 佩恩谱不等式的改进版本
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-28 DOI: 10.1016/j.jde.2026.114138
Paolo Acampora , Emanuele Cristoforoni , Carlo Nitsch , Cristina Trombetti
A celebrated inequality by Payne relates the first eigenvalue of the Dirichlet Laplacian to the first eigenvalue of the buckling problem. Motivated by the goal of establishing a quantitative version of this inequality, we show that Payne's original estimate—which is not sharp—can in fact be improved. Our result provides a refined spectral bound and opens the way to further investigations into quantitative enhancements of classical inequalities in spectral theory.
佩恩的一个著名不等式将狄利克雷拉普拉斯函数的第一特征值与屈曲问题的第一特征值联系起来。在建立这个不等式的定量版本的目标的激励下,我们表明Payne的原始估计——它并不清晰——实际上可以改进。我们的结果提供了一个精细的谱界,并为进一步研究谱理论中经典不等式的定量增强开辟了道路。
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引用次数: 0
Hydrodynamic limit to the rarefaction wave for the Boltzmann equation 玻尔兹曼方程中稀疏波的水动力极限
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-30 DOI: 10.1016/j.jde.2026.114161
Guanghui Wang , Lingda Xu , Mingying Zhong
In this paper, we study the hydrodynamic limit for rarefaction wave from the Boltzmann equation to Euler equations. We obtain the convergence rate of ϵ in L norm on finite time interval [0,T], where ϵ>0 is the Knudsen number and T>0 is any fixed constant. This convergence rate coincides with Caflisch 1980, cf. [1], which studied the hydrodynamic limit for smooth Euler solutions. This rate improves the result of Xin-Zeng 2010, where the convergence rate is ϵ12 in L norm, cf. [25]. The result is obtained by a refined energy estimate and the better rates are obtained for the higher-order derivatives.
本文从玻尔兹曼方程到欧拉方程研究了稀疏波的水动力极限。我们得到了L∞范数在有限时间区间[0,T]上的收敛速率,其中ϵ>;0为Knudsen数,T >;0为任意固定常数。这一收敛速度与Caflisch 1980, cf.[1]研究光滑欧拉解的水动力极限相一致。该速率改进了Xin-Zeng 2010的结果,在L∞范数下收敛速率为ϵ12,参见[25]。通过改进的能量估计得到了结果,并对高阶导数得到了较好的速率。
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引用次数: 0
Averaging theory and catastrophes 平均理论和灾难
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-21 DOI: 10.1016/j.jde.2026.114126
Pedro C.C.R. Pereira , Mike R. Jeffrey , Douglas D. Novaes
When a dynamical system is subject to a periodic perturbation, the averaging method can be applied to obtain an autonomous leading order ‘guiding system’, placing the time dependence at higher orders. Recent research focused on investigating invariant structures in non-autonomous differential systems arising from hyperbolic structures in the guiding system, such as periodic orbits and invariant tori. Complementarily, the effect that bifurcations in the guiding system have on the original non-autonomous one has also been recently explored, albeit less frequently. This paper extends this study by providing a broader description of the dynamics that can emerge from non-hyperbolic structures of the guiding system. Specifically, we prove here that K-universal bifurcations in the guiding system ‘persist’ in the original non-autonomous one, while non-versal bifurcations, such as the transcritical and pitchfork, do not. We illustrate the results on examples of a fold, a transcritical, a pitchfork, and a saddle-focus.
当动力系统受到周期性扰动时,可以应用平均方法获得一个自主的超前阶“导向系统”,将时间依赖置于更高阶。近年来的研究主要集中在研究由导向系统中的双曲结构引起的非自治微分系统中的不变量结构,如周期轨道和不变量环面。与此相辅相成的是,指导系统的分叉对原来的非自治系统的影响最近也进行了探讨,尽管频率较低。本文通过提供从导向系统的非双曲结构中可能出现的动力学的更广泛的描述来扩展这一研究。具体地说,我们在这里证明了引导系统中的k -通用分岔“坚持”在原始的非自治分岔中,而非通用分岔,如跨临界和干草叉,则不会。我们举例说明了一个折叠,一个跨临界,一个干草叉,和一个鞍焦点的结果。
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引用次数: 0
Propagation properties of Fisher-KPP lattice equations with almost periodic coefficients 具有概周期系数的Fisher-KPP格方程的传播特性
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-26 DOI: 10.1016/j.jde.2026.114143
Hai Zhou, Tao Zhou
<div><div>In this paper, we investigate the properties of the spreading speeds for the following Fisher-KPP lattice system in the almost periodic media:<span><span><span>(⁎)</span><span><math><mrow><mo>{</mo><mtable><mtr><mtd></mtd><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>)</mo><mo>=</mo><msubsup><mrow><mi>d</mi></mrow><mrow><mi>i</mi></mrow><mrow><mo>′</mo></mrow></msubsup><mo>(</mo><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>+</mo><mn>1</mn><mo>)</mo><mo>−</mo><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>)</mo><mo>)</mo><mo>+</mo><msub><mrow><mi>d</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>(</mo><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>−</mo><mn>1</mn><mo>)</mo><mo>−</mo><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>)</mo><mo>)</mo><mo>+</mo><mi>f</mi><mo>(</mo><mi>i</mi><mo>,</mo><mi>u</mi><mo>(</mo><mi>t</mi><mo>,</mo><mi>i</mi><mo>)</mo><mo>)</mo><mo>,</mo></mtd></mtr><mtr><mtd></mtd><mtd><mi>u</mi><mo>(</mo><mn>0</mn><mo>,</mo><mi>i</mi><mo>)</mo><mo>=</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>i</mi><mo>)</mo><mo>∈</mo><mo>[</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>]</mo><mspace></mspace><mtext>is nonzero with compact support</mtext><mo>.</mo></mtd></mtr></mtable></mrow></math></span></span></span> First, we prove the existence of spreading speeds <span><math><msup><mrow><mi>ω</mi></mrow><mrow><mo>+</mo></mrow></msup></math></span> and <span><math><msup><mrow><mi>ω</mi></mrow><mrow><mo>−</mo></mrow></msup></math></span> of <span><span>(⁎)</span></span> in the positive and negative directions, respectively, without the “small drift” assumption. Moreover, the difference between the speeds on both sides (i.e., which is larger) is determined by a certain average of the left and right fluxes. Specifically,<span><span><span><math><mtext>sgn</mtext><mo>(</mo><msup><mrow><mi>ω</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>−</mo><msup><mrow><mi>ω</mi></mrow><mrow><mo>−</mo></mrow></msup><mo>)</mo><mo>=</mo><mtext>sgn</mtext><mo>(</mo><munder><mi>lim</mi><mrow><mi>n</mi><mo>→</mo><mo>∞</mo></mrow></munder><mo>⁡</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mi>n</mi></mrow></mfrac><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>n</mi></mrow></munderover><mi>ln</mi><mo>⁡</mo><mfrac><mrow><msubsup><mrow><mi>d</mi></mrow><mrow><mi>i</mi></mrow><mrow><mo>′</mo></mrow></msubsup></mrow><mrow><msub><mrow><mi>d</mi></mrow><mrow><mi>i</mi></mrow></msub></mrow></mfrac><mo>)</mo><mo>.</mo></math></span></span></span> We also prove the convergence of the average in the discrete case to that in the continuous case. Additionally, we demonstrate that, in the homogeneous case, any small perturbation of the 2-periodic drift reduces the expanding spread of the level set, i.e., the value <span><math><msup><mrow><mi>ω</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>+</mo><msup><mrow><mi>ω</mi></mrow><mrow><mo>−</mo
本文研究了近似周期介质上的一类Fisher-KPP格系统的扩展速度的性质:(f){ut(t,i)=di ' (u(t,i+1) - u(t,i))+di(u(t,i - 1) - u(t,i))+f(i,u(t,i)),u(0,i)=u0(i)∈[0,1]是非零的紧支撑。首先,在不存在“小漂移”假设的情况下,证明了()在正、负方向上分别存在扩展速度ω+和ω−。此外,两边的速度之差(即哪个更大)是由左右通量的一定平均值决定的。具体来说,胡志明市(ω+−ω−)=胡志明市(描写→∞⁡1 n∑我= 1 nln⁡di 'di)。我们还证明了离散情况下的均值收敛于连续情况下的均值。此外,我们证明,在齐次情况下,任何2周期漂移的小扰动都会减小水平集的扩展范围,即值ω++ω−。这种行为不同于连续情况下的行为。
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Moreover, the difference between the speeds on both sides (i.e., which is larger) is determined by a certain average of the left and right fluxes. Specifically,&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mtext&gt;sgn&lt;/mtext&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;ω&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;msup&gt;&lt;mrow&gt;&lt;mi&gt;ω&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;mo&gt;=&lt;/mo&gt;&lt;mtext&gt;sgn&lt;/mtext&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;munder&gt;&lt;mi&gt;lim&lt;/mi&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;→&lt;/mo&gt;&lt;mo&gt;∞&lt;/mo&gt;&lt;/mrow&gt;&lt;/munder&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;munderover&gt;&lt;mo&gt;∑&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/munderover&gt;&lt;mi&gt;ln&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;′&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; We also prove the convergence of the average in the discrete case to that in the continuous case. Additionally, we demonstrate that, in the homogeneous case, any small perturbation of the 2-periodic drift reduces the expanding spread of the level set, i.e., the value &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;ω&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;msup&gt;&lt;mrow&gt;&lt;mi&gt;ω&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":"461 ","pages":"Article 114143"},"PeriodicalIF":2.3,"publicationDate":"2026-04-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146074313","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
Stability of 2D tropical climate system with partial dissipations near Couette flow Couette流附近部分耗散的二维热带气候系统的稳定性
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-28 DOI: 10.1016/j.jde.2026.114148
Dongjuan Niu , Huiru Wu , Jiahong Wu , Xiaojing Xu
The Tropical Climate Model (TCM) is a simplified system that captures key aspects of equatorial atmospheric dynamics through the interaction of barotropic and baroclinic velocity modes with temperature fields. This study focuses on the nonlinear stability of Couette flow in a two-dimensional TCM with only partial dissipation. Two main difficulties arise: the absence of full dissipation, and the lack of a divergence-free condition for the baroclinic velocity. To address these challenges, we develop a refined Fourier multiplier approach that captures enhanced dissipation via the interaction between the shear-induced mixing term and vertical viscosity. Furthermore, this paper introduces new techniques to handle terms involving non-divergence-free components and exploits key couplings within the system to control potentially unstable linear terms. Under appropriate smallness conditions on the initial perturbations in anisotropic Sobolev spaces, we rigorously establish the nonlinear stability of the Couette flow and identify a possible precise transition threshold for stability.
热带气候模式(TCM)是一个简化的系统,它通过正压和斜压速度模式与温度场的相互作用来捕捉赤道大气动力学的关键方面。本文研究了仅部分耗散的二维TCM中Couette流的非线性稳定性。出现了两个主要困难:缺乏充分耗散,以及缺乏斜压速度的无散度条件。为了解决这些挑战,我们开发了一种改进的傅立叶乘数方法,通过剪切诱导的混合项和垂直粘度之间的相互作用来捕获增强的耗散。此外,本文还介绍了处理涉及非无散度分量的项的新技术,并利用系统内的关键耦合来控制潜在不稳定的线性项。在各向异性Sobolev空间初始扰动较小的条件下,我们严格地建立了Couette流的非线性稳定性,并确定了可能的精确过渡阈值。
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引用次数: 0
Complex spatiotemporal dynamics in a diffusive intraguild predation model with digestion delay 具有消化延迟的扩散性捕食模型的复杂时空动力学
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-16 DOI: 10.1016/j.jde.2026.114107
Wanxiao Xu , Hongying Shu , Lin Wang , Xiang-Sheng Wang , Jianshe Yu
Incorporating spatial diffusion and digestion delay into an intraguild predation (IGP) model, this work demonstrates rich spatiotemporal dynamics governing biological invasions. We derive criteria for the successful invasion of the intraguild predator and identify a critical diffusion threshold that eliminates spatially heterogeneous steady states. The digestion delay induces stability switches, resulting in a finite number of stability intervals, and causing abrupt shifts in coexistence patterns as the delay crosses critical thresholds. Through steady state bifurcation analysis, we rigorously establish the emergence of spatially heterogeneous coexistence states. We further derive Turing instability conditions for Hopf-bifurcating periodic solutions in a general three-dimensional delayed diffusive system. Our results reveal multiple coexistence mechanisms, including homogeneous steady states, periodic oscillations, and complex spatiotemporal patterns, highlighting the intricate interplay between time delay and spatial heterogeneity in biological invasions.
将空间扩散和消化延迟纳入到一个种群内捕食(IGP)模型中,这项工作展示了控制生物入侵的丰富时空动态。我们推导了野生捕食者成功入侵的标准,并确定了消除空间异质稳态的关键扩散阈值。消化延迟诱导稳定开关,导致有限数量的稳定间隔,并在延迟超过临界阈值时引起共存模式的突变。通过稳态分岔分析,我们严格地建立了空间异质共存状态的出现。在此基础上,进一步导出了一类广义三维延迟扩散系统hopf分岔周期解的图灵不稳定性条件。我们的研究结果揭示了生物入侵的多重共存机制,包括均匀的稳态、周期振荡和复杂的时空模式,突出了生物入侵的时间延迟和空间异质性之间复杂的相互作用。
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引用次数: 0
Global smooth solutions of compressible Navier–Stokes equations with degenerate viscosity and vacuum 具有退化黏度和真空的可压缩Navier-Stokes方程的全局光滑解
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-16 DOI: 10.1016/j.jde.2026.114112
Andrew Yang , Xu Zhao , Wenshu Zhou
We study free boundary problem of the one dimensional compressible isentropic Navier–Stokes equations with density–dependent viscosity when the initial density connects to the vacuum states continuously and is either of compact or infinite support. Precisely, the pressure and the viscosity coefficient are assumed to be proportional to ργ and ρθ respectively, where ρ is the density, and γ and θ are positive constants. We prove the global existence of smooth solutions with large initial data when θ>0 and γ1+θ. Since the power θ of the previous results on this topic does not exceed 2, the result of this paper fills at least the gap for large θ. The result includes also the case of the infinite support of the initial density, which just corresponds to the one when 0<θ1. Notice that two key estimates of the proof are the uniform lower bound of the density and the uniform L bound of the velocity with respect to the construction of the approximate solutions. In contrast to the traditional techniques relying on weighted energy estimates, they are proved independently by the comparison principle and the maximal principle, respectively. Moreover, we obtain some results on regularity up to boundary and uniqueness of solutions. The results of this paper cover some important models, for instance, the viscous Saint–Venant model for the motion of shallow water, i.e., θ=1 and γ=2.
研究了初始密度与真空状态连续连接且为紧支撑或无限支撑时,具有密度依赖黏度的一维可压缩等熵Navier-Stokes方程的自由边界问题。精确地说,假设压力和粘度系数分别与ργ和ρθ成正比,其中ρ为密度,γ和θ为正常数。证明了当θ>;0和γ≥1+θ时具有大初始数据的光滑解的整体存在性。由于这一主题的先前结果的幂θ不超过2,因此本文的结果至少填补了大θ的空白。结果还包括初始密度的无限支撑情况,它正好对应于0<;θ≤1时的情况。注意,证明的两个关键估计是密度的均匀下界和速度的均匀L∞界,这是关于近似解的构造的。与传统的依赖加权能量估计的方法不同,它们分别通过比较原理和极大值原理进行独立证明。此外,我们还得到了解在边界处的正则性和唯一性的一些结果。本文的结果涵盖了一些重要的模型,如浅水运动的粘性Saint-Venant模型,即θ=1, γ=2。
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引用次数: 0
On the Nirenberg problem on spheres: Arbitrarily many solutions in a perturbative setting 关于球上的Nirenberg问题:摄动环境下的任意多解
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-19 DOI: 10.1016/j.jde.2026.114105
Mohameden Ahmedou , Mohamed Ben Ayed , Khalil El Mehdi
Given a smooth positive function K on the standard sphere (Sn,g0), we use Morse theoretical methods and counting index formulae to prove that, under generic conditions on the function K, there are arbitrarily many metrics g conformally equivalent to g0 and whose scalar curvature is given by the function K provided that the function is sufficiently close to the scalar curvature of g0. Our approach leverages a comprehensive characterization of blowing-up solutions of a subcritical approximation, along with various Morse relations involving their indices. Notably, this multiplicity result is achieved without relying on any symmetry or periodicity assumptions about the function K.
给定标准球面(Sn,g0)上的光滑正函数K,利用莫尔斯理论方法和计数指标公式证明了在函数K的一般条件下,存在任意多个与g0共形等价的度量g,其标量曲率由函数K给出,只要该函数足够接近g0的标量曲率。我们的方法利用了亚临界近似的爆破解的综合表征,以及涉及其指标的各种莫尔斯关系。值得注意的是,这个多重性结果是在不依赖于关于函数K的任何对称性或周期性假设的情况下实现的。
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引用次数: 0
Blow-up solutions for general Toda systems on Riemann surfaces 黎曼曲面上一般Toda系统的爆破解
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-28 DOI: 10.1016/j.jde.2026.114145
Zhengni Hu, Miaomiao Zhu
In this paper, we study general Toda systems with homogeneous Neumann boundary conditions on Riemann surfaces. Assuming the surface satisfies the “k-symmetric” condition, we construct a family of bubbling solutions using singular perturbation methods, where the concentration rates of different components occur in distinct orders. In particular, we establish the existence of asymmetric blow-up solutions for the SU(3) Toda system. Furthermore, the blow-up points are precisely located at the “k-symmetric” centers of the surface.
本文研究了黎曼曲面上具有齐次诺伊曼边界条件的一般Toda系统。假设表面满足“k对称”条件,我们用奇异摄动方法构造了一组冒泡解,其中不同组分的浓度率以不同的顺序出现。特别地,我们建立了SU(3) Toda系统的不对称爆破解的存在性。此外,爆炸点精确地位于表面的“k对称”中心。
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引用次数: 0
Polynomial stability of non-linearly damped contraction semigroups 非线性阻尼收缩半群的多项式稳定性
IF 2.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-04-25 Epub Date: 2026-01-20 DOI: 10.1016/j.jde.2026.114129
Lassi Paunonen , David Seifert
We investigate the stability properties of an abstract class of semi-linear systems. Our main result establishes rational rates of decay for classical solutions assuming a certain non-uniform observability estimate for the linear part and suitable conditions on the non-linearity. We illustrate the strength of our abstract results by applying them to a one-dimensional wave equation with weak non-linear damping and to an Euler–Bernoulli beam with a tip mass subject to non-linear damping.
研究一类抽象的半线性系统的稳定性。我们的主要结果建立了经典解的合理衰减率,假设线性部分有一定的非均匀可观测性估计和非线性的适当条件。我们通过将抽象结果应用于具有弱非线性阻尼的一维波动方程和具有非线性阻尼的尖端质量的欧拉-伯努利梁来说明其强度。
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引用次数: 0
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Journal of Differential Equations
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