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Measurable solutions of an alternative functional equation 可选泛函方程的可测解
IF 0.7 3区 数学 Q2 MATHEMATICS Pub Date : 2026-01-14 DOI: 10.1007/s00010-026-01263-z
Péter Tóth

In this paper we investigate the functional equation

$$begin{aligned} varphi left( frac{x+y}{2} right) left( psi _1(x) - psi _2(y) right) = 0 quad left( hbox { for all } x in I_1 hbox { and } y in I_2 right) end{aligned}$$

where ( I_1 , I_2 ) are open intervals of ( mathbb {R}), ( J = frac{1}{2} left( I_1 + I_2 right) ) moreover ( psi _1: I_1 rightarrow mathbb {R}), ( psi _2: I_2 rightarrow mathbb {R}) and ( varphi : J rightarrow mathbb {R}) are unknown functions. We describe the structure of the possible solutions assuming that ( varphi ) is measurable. In the case when ( varphi ) is a derivative, we give a complete characterization of the solutions. Furthermore, we present an example of a solution consisting of irregular Darboux functions. This provides the answer to an open problem proposed during the 59th International Symposium on Functional Equations.

本文研究了泛函方程$$begin{aligned} varphi left( frac{x+y}{2} right) left( psi _1(x) - psi _2(y) right) = 0 quad left( hbox { for all } x in I_1 hbox { and } y in I_2 right) end{aligned}$$,其中( I_1 , I_2 )为( mathbb {R})、( J = frac{1}{2} left( I_1 + I_2 right) )的开区间,( psi _1: I_1 rightarrow mathbb {R})、( psi _2: I_2 rightarrow mathbb {R})、( varphi : J rightarrow mathbb {R})为未知函数。假设( varphi )是可测量的,我们描述可能解的结构。当( varphi )为导数时,给出了解的完整表征。此外,我们还给出了一个由不规则达布函数组成的解的例子。这为第59届泛函方程国际研讨会上提出的一个开放性问题提供了答案。
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引用次数: 0
Petal-like vortex solitons with fractional angular momentum in Bessel optical lattices 贝塞尔光学晶格中具有分数角动量的花瓣状涡旋孤子
IF 5.6 1区 数学 Q1 MATHEMATICS, INTERDISCIPLINARY APPLICATIONS Pub Date : 2026-01-14 DOI: 10.1016/j.chaos.2026.117893
Lifen Yan, Mingfeng Wang, Dong Zhang, Haiyong Zhu
We predict the existence of petal-like vortex solitons (PVSs) carrying fractional angular momentum in a defocusing cubic nonlinear medium modulated by the cylindrical Bessel optical lattice. Linear stability analysis and direct simulations show that PVSs remain stable when the propagation constant exceeds a critical value but revert to a ring vortex soliton at a second threshold. Fundamental fractional vortex soliton possesses an opening gap in the intensity ring, and its power and angular momentum per photon vary continuously with the propagating constant. Higher-order PVS exhibits an odd number of petals, which results from a complex phase distribution containing an equal number of phase dislocations. Specifically, the stability domain of the soliton shrinks as the number of petals increases.
我们预测了由圆柱贝塞尔光学晶格调制的离焦立方非线性介质中携带分数角动量的花瓣状涡旋孤子(ppvss)的存在。线性稳定性分析和直接模拟表明,当传播常数超过一个临界值时,pds保持稳定,但在第二个阈值时恢复为环形涡孤子。基本分数涡旋孤子在强度环上具有开口隙,其功率和每光子角动量随传播常数连续变化。高阶pv呈现奇数花瓣,这是由包含相等数量相位错的复杂相分布造成的。具体来说,随着花瓣数量的增加,孤子的稳定域会缩小。
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引用次数: 0
Nonlinear chaotic dynamics of functionally graded graphene composite curved plates for the wings of low-altitude aircrafts 低空飞机机翼功能梯度石墨烯复合材料弯曲板的非线性混沌动力学
IF 5.6 1区 数学 Q1 MATHEMATICS, INTERDISCIPLINARY APPLICATIONS Pub Date : 2026-01-14 DOI: 10.1016/j.chaos.2026.117877
Yifeng Zhang , Wei Zhang , Yufei Zhang
Low-altitude aircrafts are subject to complex aerodynamic and environmental disturbances, which place stringent demands on lightweight structures with reliable dynamic stability. Functionally graded graphene-reinforced composites (FG-GRCs), owing to their high specific strength and tunable properties, are promising candidates for load-bearing and vibration-sensitive components in such vehicles. This study investigates the complex nonlinear dynamics, particularly multi-pulse chaotic vibrations, of cantilever laminated curved plate subjected simultaneous transverse and in-plane parametric excitations. A nonlinear dynamic model incorporating geometric curvature and material gradation effects is established and validated by finite element analysis, revealing a critical 1:1 internal resonance between specific modes under particular geometric configurations. The extended Melnikov method is applied to theoretically predict the Shilnikov-type multi-pulse chaotic motions. Bi-parameter threshold surfaces derived from the Melnikov function are proposed and quantitatively validated against two-dimensional maximum Lyapunov exponent (MLE) diagrams, exhibiting good agreement in identifying chaotic regions. Extensive numerical simulations, including bifurcation diagrams, phase portraits, Poincaré maps, and time histories, confirm the presence of complex dynamics such as periodic motions, chaotic vibrations, and their transitions. The results provide crucial insights into the parameter domains that may trigger hazardous chaotic responses in FG-GRC curved plates, supporting the safe and reliable design of next-generation low-altitude aircraft structures such as wings, rotor arms, and fuselage skins.
低空飞行器受到复杂的空气动力学和环境干扰,这对具有可靠动力稳定性的轻型结构提出了苛刻的要求。功能梯度石墨烯增强复合材料(FG-GRCs)由于其高比强度和可调性能,是此类车辆中承载和振动敏感部件的有希望的候选者。本文研究了悬臂层合弯曲板在同时受到横向和平面参数激励下的复杂非线性动力学,特别是多脉冲混沌振动。建立了考虑几何曲率和材料梯度效应的非线性动力学模型,并通过有限元分析验证了该模型的有效性,揭示了特定几何构型下特定模态之间存在1:1的临界内共振。应用扩展梅尔尼科夫方法对希利尼科夫型多脉冲混沌运动进行了理论预测。提出了由Melnikov函数导出的双参数阈值曲面,并对二维最大李雅普诺夫指数(MLE)图进行了定量验证,在识别混沌区域方面表现出良好的一致性。广泛的数值模拟,包括分岔图、相肖像、庞加莱图和时间历史,证实了复杂动力学的存在,如周期运动、混沌振动及其转换。该结果为FG-GRC弯曲板中可能引发危险混沌响应的参数域提供了重要见解,为下一代低空飞机结构(如机翼、旋翼臂和机身蒙皮)的安全可靠设计提供了支持。
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引用次数: 0
Local Hölder regularity for quasilinear elliptic equations with mixed local-nonlocal operators, variable exponents, and weights 具有混合局部-非局部算子,可变指数和权重的拟线性椭圆方程的局部Hölder正则性
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2026-01-14 DOI: 10.1016/j.jmaa.2026.130417
Juan Pablo Alcon Apaza
<div><div>We establish local boundedness and local Hölder continuity of weak solutions to the following prototype problem:<span><span><span><math><mo>−</mo><mi>div</mi><mspace></mspace><mrow><mo>(</mo><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mo>−</mo><mn>2</mn><mi>β</mi></mrow></msup><mo>|</mo><mi>∇</mi><mi>u</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>q</mi><mo>−</mo><mn>2</mn></mrow></msup><mi>∇</mi><mi>u</mi><mo>)</mo></mrow><mo>+</mo><msubsup><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow><mrow><mi>Ω</mi><mo>,</mo><mi>p</mi><mo>(</mo><mo>⋅</mo><mo>,</mo><mo>⋅</mo><mo>)</mo><mo>,</mo><mi>β</mi></mrow><mrow><mi>s</mi><mo>(</mo><mo>⋅</mo><mo>,</mo><mo>⋅</mo><mo>)</mo></mrow></msubsup><mi>u</mi><mo>=</mo><mn>0</mn><mspace></mspace><mtext> in </mtext><mspace></mspace><mi>Ω</mi><mo>,</mo></math></span></span></span> where <span><math><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup></math></span>, <span><math><mi>n</mi><mo>≥</mo><mn>2</mn></math></span>, is a bounded domain. The nonlocal operator is defined by<span><span><span><math><msubsup><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow><mrow><mi>Ω</mi><mo>,</mo><mi>p</mi><mo>(</mo><mo>⋅</mo><mo>,</mo><mo>⋅</mo><mo>)</mo><mo>,</mo><mi>β</mi></mrow><mrow><mi>s</mi><mo>(</mo><mo>⋅</mo><mo>,</mo><mo>⋅</mo><mo>)</mo></mrow></msubsup><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>:</mo><mo>=</mo><mrow><mi>P</mi><mo>.</mo><mi>V</mi><mi>.</mi></mrow><mspace></mspace><munder><mo>∫</mo><mrow><mi>Ω</mi></mrow></munder><mfrac><mrow><mo>|</mo><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mi>u</mi><mo>(</mo><mi>y</mi><mo>)</mo><msup><mrow><mo>|</mo></mrow><mrow><mi>p</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>y</mi><mo>)</mo><mo>−</mo><mn>2</mn></mrow></msup><mo>(</mo><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mi>u</mi><mo>(</mo><mi>y</mi><mo>)</mo><mo>)</mo></mrow><mrow><mo>|</mo><mi>x</mi><mo>−</mo><mi>y</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>n</mi><mo>+</mo><mi>s</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>y</mi><mo>)</mo><mi>p</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>y</mi><mo>)</mo></mrow></msup></mrow></mfrac><mo>⋅</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>β</mi></mrow></msup><mo>|</mo><mi>y</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>β</mi></mrow></msup></mrow></mfrac><mspace></mspace><mi>d</mi><mi>y</mi><mo>.</mo></math></span></span></span> Here, <span><math><mi>p</mi><mo>:</mo><mi>Ω</mi><mo>×</mo><mi>Ω</mi><mo>→</mo><mo>(</mo><mn>1</mn><mo>,</mo><mo>∞</mo><mo>)</mo></math></span> and <span><math><mi>s</mi><mo>:</mo><mi>Ω</mi><mo>×</mo><mi>Ω</mi><mo>→</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo></math></span> are measurable functions, <span><math><mi>q</mi><mo>:</mo><mo>=</mo><mi>ess</mi><mspace></mspace><msub><mrow><mi>sup</mi></mrow><mrow><mi>Ω</mi><mo>×</mo><mi>Ω</mi></mrow></msub><mo>⁡</mo><mspace></mspace><mi>p</mi></math></span>, and <span><math><mn>0</mn><mo>≤</mo><mn>2</mn>
我们建立了以下原型问题弱解的局部有界性和局部Hölder连续性:−div(|x|−2β|∇u|q−2∇u)+(−Δ)Ω,p(⋅,⋅),βs(⋅,⋅)u=0在Ω中,其中Ω∧Rn, n≥2是一个有界域。外地操作符被定义为(−Δ)Ω,p(⋅⋅),β年代(⋅⋅)u (x): = pv∫Ω| u (x)−u (y) | p (x, y)−2 (u (x)−u (y)) x−y | | n + s (x, y) p (x, y)⋅1 | x |βy | |βdy。在这里,p:Ω×Ω→(∞)和年代:Ω×Ω→(0,1)是可测函数,问:= esssupΩ×Ω⁡p,和0≤2β& lt; n。我们的方法是解析的,依赖于De Giorgi-Nash-Moser理论对具有可变指数和权重的混合局部-非局部框架的适应。
{"title":"Local Hölder regularity for quasilinear elliptic equations with mixed local-nonlocal operators, variable exponents, and weights","authors":"Juan Pablo Alcon Apaza","doi":"10.1016/j.jmaa.2026.130417","DOIUrl":"10.1016/j.jmaa.2026.130417","url":null,"abstract":"&lt;div&gt;&lt;div&gt;We establish local boundedness and local Hölder continuity of weak solutions to the following prototype problem:&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;div&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt; in &lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; where &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;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, is a bounded domain. The nonlocal operator is defined by&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mo&gt;⋅&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&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;mo&gt;=&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;mi&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;munder&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;/munder&gt;&lt;mfrac&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;mo&gt;−&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;p&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&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;u&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;/mrow&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;y&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;s&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;mi&gt;p&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;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&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;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mspace&gt;&lt;/mspace&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;p&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mi&gt;Ω&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;mo&gt;∞&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;→&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&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; are measurable functions, &lt;span&gt;&lt;math&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;ess&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;sup&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;","PeriodicalId":50147,"journal":{"name":"Journal of Mathematical Analysis and Applications","volume":"558 2","pages":"Article 130417"},"PeriodicalIF":1.2,"publicationDate":"2026-01-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145978789","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
Lp–Lq existence for the open compressible MHD system 开放可压缩MHD系统的Lp-Lq存在性
IF 1.3 2区 数学 Q1 MATHEMATICS Pub Date : 2026-01-14 DOI: 10.1016/j.na.2026.114057
Mostafa Meliani
We study the local existence of solutions to the Navier–Stokes–Fourier-magnetohydrodynamics (NSF-MHD) system describing the motion of a compressible, viscous, electrically and heat conducting fluid in the LpLq class with inhomogeneous boundary conditions. The open system is allowed to receive incoming matter from the outside through (part of) the boundary which we refer to as an inflow boundary. This setup brings about a difficulty in estimating the regularity of the density ϱ which we remedy by assuming appropriate hypotheses on the velocity field, domain boundary and on the boundary and initial data of ϱ. The main result ensures the local well-posedness of the full NSF-MHD system which is shown through a linearization combined with a Banach fixed-point theorem.
研究了具有非均匀边界条件的可压缩、粘性、导电和导热流体的navier - stokes - fourier -磁流体动力学(NSF-MHD)系统解的局部存在性。开放系统允许从外部通过(部分)边界接收进入的物质,我们称之为流入边界。这种设置给估计密度的规律性带来了困难,我们通过对速度场、域边界以及ϱ的边界和初始数据进行适当的假设来弥补这一困难。主要结果保证了全NSF-MHD系统的局部适定性,并通过结合Banach不动点定理的线性化来证明。
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引用次数: 0
On the well-posedness of the unsteady velocity-vorticity-helicity formulation of the Navier–Stokes equations Navier-Stokes方程非定常速度-涡度-螺旋形式的适定性
IF 1.2 3区 数学 Q1 MATHEMATICS Pub Date : 2026-01-14 DOI: 10.1016/j.jmaa.2026.130421
K. Benmoussa , J. Deteix , D. Yakoubi
In this paper, we study the three-dimensional velocity–vorticity–helicity (VVH) formulation modeling the flow of incompressible Newtonian fluids. We present an analysis of the formulation that encompasses the existence and regularity of solutions, providing a rigorous functional framework in which the VVH formulation is shown to be equivalent to the more traditional velocity–pressure formulation.
本文研究了不可压缩牛顿流体流动的三维速度-涡度-螺旋度(VVH)公式。我们对包含解的存在性和规律性的公式进行了分析,提供了一个严格的功能框架,其中VVH公式被证明与更传统的速度-压力公式等效。
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引用次数: 0
Wavelength Selection for Periodic Travelling Waves: An Unsolved Problem. 周期行波的波长选择:一个尚未解决的问题。
IF 2.2 4区 数学 Q2 BIOLOGY Pub Date : 2026-01-14 DOI: 10.1007/s11538-025-01576-1
Lukas Eigentler, Mattia Sensi

Periodic travelling waves (PTWs) are a common solution type of models describing spatio-temporal patterns in biology and ecology. Particularly in ecology, pattern formation is regarded as a resilience mechanism and an ecosystem's ability to change its pattern wavelength is seen as a tool to adapt to environmental change. PTW solutions of corresponding mathematical models also possess this ability and typically undergo a cascade of wavelength changes in response to a gradual change in a bifurcation parameter. Extensive analysis has been conducted to develop a predictive understanding of parameter thresholds leading to wavelength changes. By contrast, theory on what determines PTW wavelength selection during a wavelength change is currently lacking and most conjectures stem from limited observations of specific simulations, or apply to special cases only. In this unsolved problems article, we first provide a review of how linear stability analysis and Busse balloon theory are used to predict parameter values at which PTW wavelength changes occur. On the topic of wavelength selection, we review the special case of PTWs in λ - ω systems, often used to predict wavelengths of predator-prey dynamics in the wake of an invasion front. For more general systems, we highlight that the Busse balloon theory that is so successful in determining parameter values of wavelength changes is unlikely able to provide information on PTW wavelength selection. Finally, we present new numerical trends of PTW wavelength selection during PTW-to-PTW transitions that highlight that some stable wavelengths are more frequently selected than others, and that cascades of wavelength changes can also result in extinction events despite bistability of the extinction state with PTWs. We conclude with a tentative list of potential approaches to unravel a deeper understanding of this topic. Combined, we aim to stimulate new approaches to gain more insights into the unsolved problem of PTW wavelength selection during PTW-to-PTW transitions.

周期行波(PTWs)是生物学和生态学中描述时空格局的一种常见解型模型。特别是在生态学中,模式形成被视为一种弹性机制,生态系统改变其模式波长的能力被视为适应环境变化的工具。相应数学模型的PTW解也具有这种能力,并且通常随着分岔参数的逐渐变化而发生一连串的波长变化。已经进行了广泛的分析,以开发导致波长变化的参数阈值的预测性理解。相比之下,关于在波长变化过程中是什么决定了PTW波长选择的理论目前还很缺乏,大多数猜测都是基于对特定模拟的有限观察,或者只适用于特殊情况。在这篇尚未解决的问题文章中,我们首先回顾了如何使用线性稳定性分析和Busse气球理论来预测PTW波长发生变化的参数值。在波长选择方面,我们回顾了λ - ω系统中PTWs的特殊情况,通常用于预测入侵前沿后捕食者-猎物动态的波长。对于更一般的系统,我们强调在确定波长变化参数值方面如此成功的Busse气球理论不太可能提供关于PTW波长选择的信息。最后,我们提出了在PTW到PTW转换过程中PTW波长选择的新数值趋势,强调了一些稳定波长比其他波长更频繁地被选择,并且尽管PTW的消光状态具有双稳定性,但波长变化的级联也可能导致消光事件。最后,我们暂时列出了一些潜在的方法,以加深对这一主题的理解。总之,我们的目标是激发新的方法,以获得更多关于PTW到PTW转换过程中PTW波长选择的未解决问题的见解。
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引用次数: 0
Almost surely exponential stability of nonlinear stochastic systems with random impulses and its application in chaos synchronization 具有随机脉冲的非线性随机系统的指数稳定性及其在混沌同步中的应用
IF 3.8 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-01-14 DOI: 10.1016/j.cnsns.2026.109664
Zenghui Hu , Jiamin Liu , Yiming Wang , Lijie You
The almost surely exponential stability (ES a.s.) is investigated for nonlinear systems subject to the effects of stochastic noises and random impulses. The randomness of impulsive effects is considered in two aspects: impulsive intensity and density. In detail, the impulsive instants and jumps are respectively impelled by a renewal process and a Markov chain. By analyzing the coupling effect among stochastic noise, randomly impulsive intensity and density, novel criteria of ES a.s. are obtained by employing Lyapunov-based approach. The proposed results not only capture the positive effect of stochastic noise, but also remove the non-zero property of solution required in existing works. As an application, the synchronization problem of master-slave stochastic chaotic systems is solved by applying the randomly impulsive control method. Two examples are provided to illustrate the effectiveness and application of the proposed results.
研究了受随机噪声和随机脉冲影响的非线性系统的指数稳定性。从脉冲强度和脉冲密度两个方面考虑脉冲效应的随机性。脉冲瞬间和跳跃分别由更新过程和马尔可夫链驱动。通过分析随机噪声、随机脉冲强度和密度之间的耦合效应,采用基于李雅普诺夫的方法得到了新的ES as准则。所提出的结果不仅捕获了随机噪声的积极影响,而且消除了现有工作中要求的解的非零性质。作为应用,采用随机脉冲控制方法解决主从随机混沌系统的同步问题。给出了两个实例来说明所提结果的有效性和应用。
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引用次数: 0
Unconditionally energy-stable and accurate schemes based on hyperbolic tangent scalar auxiliary variable approach for gradient flows 基于双曲正切标量辅助变量方法的梯度流无条件能量稳定精确格式
IF 2.5 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-01-14 DOI: 10.1016/j.camwa.2025.12.031
Haihong Zhou , Huan Zhang , Xiaomin Pan
In this paper, we extend the selection of auxiliary variables by proposing a hyperbolic tangent scalar auxiliary variable (tanh-SAV) approach for solving gradient flows. The proposed tanh-SAV schemes introduce an auxiliary variable based on the hyperbolic tangent function, providing a well-defined formulation that enables the construction of decoupled, linear, and efficient numerical schemes. We demonstrate the construction of first-order, second-order, and higher-order unconditionally energy-stable schemes, utilizing either the Crank–Nicolson method or a k-step backward differentiation formula for time discretization. Only one constant-coefficient equation needs to be solved per time step, and we prove that all resulting tanh-SAV schemes are uniquely solvable at each time level. Furthermore, the theoretical analysis demonstrates the discrete energy stability of the proposed numerical schemes and proves the positivity property of the auxiliary variable. For the tanh-SAV/BDFk schemes (k=2,3,4) combined with a Fourier pseudo-spectral spatial discretization, we further establish fully discrete optimal-order error estimates. In addition, we provide numerical simulations of one- and two-dimensional Cahn–Hilliard, Allen–Cahn, and phase-field crystal models. The results demonstrate that, consistent with the theoretical analysis, the proposed schemes preserve the positivity of the auxiliary variable, maintain excellent stability, and achieve the desired temporal accuracy.
本文通过提出求解梯度流的双曲正切标量辅助变量法(tanh-SAV),扩展了辅助变量的选择。提出的tanh-SAV方案引入了一个基于双曲正切函数的辅助变量,提供了一个定义良好的公式,可以构建解耦、线性和高效的数值方案。我们利用Crank-Nicolson方法或k步后向微分公式进行时间离散,证明了一阶、二阶和高阶无条件能量稳定格式的构造。每个时间步只需要求解一个常系数方程,并证明了所有的tanh-SAV格式在每个时间水平上都是唯一可解的。理论分析进一步证明了所提数值格式的离散能量稳定性,并证明了辅助变量的正性。对于tanh-SAV/BDFk格式(k=2,3,4),结合傅里叶伪谱空间离散,我们进一步建立了完全离散的最优阶误差估计。此外,我们还提供了一维和二维Cahn-Hilliard, Allen-Cahn和相场晶体模型的数值模拟。结果表明,与理论分析一致,所提出的方案保留了辅助变量的正性,保持了良好的稳定性,并达到了期望的时间精度。
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引用次数: 0
A simplified discontinuous reproducing kernel method for impulsive differential equations 脉冲微分方程的简化不连续再现核方法
IF 3.4 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-01-14 DOI: 10.1016/j.amc.2026.129950
Liangcai Mei , Yingchao Zhang , Boying Wu , Yingzhen Lin
In this article, a spatial concept of direct sum space based on the discontinuous reproducing kernel method (RKM for short) is proposed for impulsive differential equations, and a reproducing kernel numerical solution method is constructed. Based on the piecewise smoothness of the solution, a discontinuous reproducing kernel is constructed, and a direct sum space is constructed in vector form to represent the structure of the equation system. Furthermore, the simplified RKM is used to solve the operator equation, and an approximate solution in series form is obtained. Finally, the regularity analysis and uniform convergence analysis are carried out, and numerical experiments verify the second-order convergence and stability of the algorithm.
针对脉冲微分方程,提出了基于不连续再现核法(简称RKM)的直接和空间概念,并构造了再现核数值求解方法。基于解的分段平滑性,构造了一个不连续的再现核,并以向量形式构造了一个直接和空间来表示方程组的结构。在此基础上,利用简化的RKM对算子方程进行求解,得到了近似的级数解。最后进行了正则性分析和一致收敛性分析,并通过数值实验验证了算法的二阶收敛性和稳定性。
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引用次数: 0
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