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The Hodge conjecture for Weil fourfolds with discriminant 1 via singular OG6-varieties 具有判别1的Weil四重函数的奇异og6变异的Hodge猜想
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-06-01 Epub Date: 2026-02-06 DOI: 10.1016/j.matpur.2026.103876
Salvatore Floccari , Lie Fu
We give a new proof of the Hodge conjecture for abelian fourfolds of Weil type with discriminant 1 and all of their powers. The Hodge conjecture for these abelian fourfolds was proven by Markman using hyperholomorphic sheaves on hyper-Kähler varieties of generalized Kummer type, and by constructing semiregular sheaves on abelian varieties. Our proof instead relies on a direct geometric relation between abelian fourfolds of Weil type with discriminant 1 and the six-dimensional hyper-Kähler varieties K˜ of O'Grady type arising as crepant resolutions K˜K of a locally trivial deformation of a singular moduli space of sheaves on an abelian surface. As applications, we establish the Hodge conjecture and the Tate conjecture for any variety K˜ of OG6-type as above, and all of its powers.
给出了判别为1的Weil型阿贝尔四重矩阵及其所有幂的Hodge猜想的一个新的证明。Markman利用广义Kummer型的hyper-Kähler变种上的超全纯束,以及在阿贝尔变种上构造半正则束,证明了这些阿贝尔四重的Hodge猜想。相反,我们的证明依赖于具有判别式1的Weil型阿贝尔四重与O'Grady型的六维hyper-Kähler变体K ~之间的直接几何关系,这些变体K ~→K是由阿贝尔曲面上束的奇异模空间的局部平凡变形的蠕变分辨率K ~→K引起的。作为应用,我们建立了上述og6型任意K ~的Hodge猜想和Tate猜想,以及它的所有幂。
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引用次数: 0
Monotonicity for solutions to semilinear problems in epigraphs 题词中半线性问题解的单调性
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-06-01 Epub Date: 2026-02-06 DOI: 10.1016/j.matpur.2026.103868
Nicolas Beuvin , Alberto Farina , Berardino Sciunzi
We consider positive solutions, possibly unbounded, to the semilinear equation Δu=f(u) on continuous epigraphs bounded from below. Under the homogeneous Dirichlet boundary condition, we prove new monotonicity results for u, when f is a (locally or globally) Lipschitz-continuous function satisfying f(0)0. As an application of our new monotonicity theorems, we prove some classification and/or non-existence results. To prove our results, we first establish some new comparison principles for semilinear problems on general unbounded open sets of RN, and then we use them to start and to complete a modified version of the moving plane method adapted to the geometry of the epigraph Ω. As a by-product of our analysis, we also prove some new results of uniqueness and symmetry for solutions (possibly unbounded and sign-changing) to the homogeneous Dirichlet BVP for the semilinear Poisson equation in fairly general unbounded domains.
我们考虑半线性方程- Δu=f(u)在有界连续柱石上的正解,可能是无界的。在齐次Dirichlet边界条件下,证明了当f是满足f(0)≥0的(局部或全局)lipschitz -连续函数时u的新的单调性结果。作为我们的新单调性定理的一个应用,我们证明了一些分类和/或不存在的结果。为了证明我们的结果,我们首先建立了一些新的关于一般无界RN开集上的半线性问题的比较原理,然后我们用它们开始并完成了一个适合于墓石Ω几何形状的改进版的移动平面方法。在相当一般的无界域上,证明了半线性泊松方程齐次Dirichlet BVP解(可能是无界的和变号的)的唯一性和对称性的一些新结果。
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引用次数: 0
Compressible fluids excited by space-dependent transport noise 受空间相关输运噪声激励的可压缩流体
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-06-01 Epub Date: 2026-02-06 DOI: 10.1016/j.matpur.2026.103875
Dominic Breit , Eduard Feireisl , Martina Hofmanová , Piotr B. Mucha
We study the compressible Navier–Stokes system driven by physically relevant transport noise, where the noise influences both the continuity and momentum equations. Our approach is based on transforming the system into a partial differential equation with random, time- and space-dependent coefficients. A key challenge arises from the fact that these coefficients are non-differentiable in time, rendering standard compactness arguments for the identification of the pressure inapplicable. To overcome this difficulty, we develop a novel multi-layer approximation scheme and introduce a precise localization strategy with respect to both the sample space and time variable. The limit pressure is then identified via the corresponding effective viscous flux identity. By means of stochastic compactness methods, particularly Skorokhod's representation theorem and its generalization by Jakubowski, we ensure the progressive measurability required to return to the original system. Our results broaden the applicability of transport noise models in fluid dynamics and offer new insights into the interaction between stochastic effects and compressibility.
研究了由物理相关输运噪声驱动的可压缩Navier-Stokes系统,其中噪声对连续性方程和动量方程都有影响。我们的方法是基于将系统转换成具有随机、时间和空间相关系数的偏微分方程。一个关键的挑战来自于这些系数在时间上是不可微的,这使得用于识别压力的标准紧致性参数不适用。为了克服这一困难,我们开发了一种新的多层近似方案,并引入了一种关于样本空间和时间变量的精确定位策略。然后通过相应的有效粘性通量同一性来确定极限压力。利用随机紧性方法,特别是Skorokhod的表示定理及其Jakubowski的推广,我们保证了回归到原始系统所需的渐进可测性。我们的研究结果扩大了输运噪声模型在流体动力学中的适用性,并为随机效应与可压缩性之间的相互作用提供了新的见解。
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引用次数: 0
Suppression of blow-up for the 3D Patlak-Keller-Segel-Navier-Stokes system via the Couette flow 通过Couette气流抑制3D patak - keller - segel - navier - stokes系统的爆炸
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-06-01 Epub Date: 2026-02-09 DOI: 10.1016/j.matpur.2026.103874
Shikun Cui, Lili Wang, Wendong Wang
As is well known, for the 3D Patlak-Keller-Segel system, regardless of whether they are parabolic-elliptic or parabolic-parabolic forms, finite-time blow-up may occur for arbitrarily small values of the initial mass. In this paper, it is proved for the first time that one can prevent the finite-time blow-up when the initial mass is less than a certain critical threshold via the stabilizing effect of the moving Navier-Stokes flows. In details, we investigate the nonlinear stability of the Couette flow (Ay,0,0) in the Patlak-Keller-Segel-Navier-Stokes system and show that if the Couette flow is sufficiently strong (A is large enough), then the solutions for Patlak-Keller-Segel-Navier-Stokes system are global in time provided that the initial velocity is sufficiently small and the initial cell mass is less than 245π2.
众所周知,对于三维patak - keller - segel系统,无论是抛物线-椭圆型还是抛物线-抛物线型,初始质量的任意小值都可能发生有限时间爆炸。本文首次证明了利用运动Navier-Stokes流的稳定作用,可以防止初始质量小于某一临界阈值时的有限时间爆破。详细地研究了patak - keller - segel - navier - stokes系统中Couette流(Ay,0,0)的非线性稳定性,并证明了当Couette流足够强(A足够大)时,在初始速度足够小且细胞质量小于245π2的条件下,patak - keller - segel - navier - stokes系统的解在时间上是全局的。
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引用次数: 0
Supersonic reacting jet flows from two-dimensional divergent nozzles 二维发散喷嘴的超音速反应射流
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-06-01 Epub Date: 2026-02-09 DOI: 10.1016/j.matpur.2026.103878
Geng Lai , Wancheng Sheng
This paper investigates a supersonic reacting jet issuing from a two-dimensional, finite-length divergent nozzle. To model the jet, a free boundary value problem for the steady two-dimensional Zeldovdovich-von Neumann-Döring (ZND) combustion equations is formulated. The flow is assumed to satisfy a slip condition along the nozzle walls, with its state prescribed at the nozzle inlet. Two external conditions are examined. First, when the nozzle exhausts into a vacuum, the global existence of a supersonic reacting jet is established using the method of characteristics. Furthermore, a sufficient condition on the nozzle wall geometry is provided that leads to the formation of a vacuum region inside the nozzle; it is shown that any such vacuum region must be adjacent to one wall. Second, when the nozzle is surrounded by a static atmosphere whose pressure is lower than the jet pressure at the exit, the analysis demonstrates the formation of singularities (i.e., shock waves) in the jet. This result provides a rigorous mathematical confirmation of the physical phenomenon described in Sec. 148 of the classical text Supersonic Flow and Shock Waves.
本文研究了二维有限长发散喷管发出的超声速反应射流。为了模拟射流,建立了稳态二维zeldovovich -von Neumann-Döring (ZND)燃烧方程的自由边值问题。假定沿喷嘴壁面流动满足滑移条件,其状态在喷嘴入口处规定。考察了两个外部条件。首先,利用特征值法建立了超音速反应射流在真空状态下的整体存在性。此外,提供喷嘴壁面几何形状的充分条件,导致在喷嘴内形成真空区域;结果表明,任何这样的真空区域都必须与一个壁相邻。其次,当喷嘴被静态大气包围时,其压力低于出口处的射流压力,分析表明射流中形成了奇点(即激波)。这一结果为经典文本超音速流动和激波第148节中描述的物理现象提供了严格的数学证实。
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引用次数: 0
Uniqueness theorems for solutions of mixed order elliptic system with general nonlinearity on R4 R4上具有一般非线性的混合阶椭圆系统解的唯一性定理
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-05-01 Epub Date: 2026-02-06 DOI: 10.1016/j.matpur.2026.103879
Daomin Cao , Yuxia Guo , Shaolong Peng
<div><div>The objective of this paper is to investigate the uniqueness theorems for solutions of the following mixed-order semi-linear elliptic system in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mn>4</mn></mrow></msup></math></span>:<span><span><span>(0.1)</span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><msup><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>=</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>)</mo><mo>,</mo></mtd></mtr><mtr><mtd><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>=</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>)</mo><mo>,</mo></mtd></mtr><mtr><mtd><msup><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow><mrow><mfrac><mrow><mn>3</mn></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>=</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>)</mo><mo>,</mo></mtd></mtr><mtr><mtd><msup><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow><mrow><mn>2</mn></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>=</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>,</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>)</mo><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> where <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>j</mi></mrow></msub><mo>≥</mo><mn>0</mn><mo>(</mo><mi>j</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>,</mo><mn>3</mn><mo>)</mo></math></span>, <span><math><msub><mrow><mi>u</mi></mrow><mrow><mn>4</mn></mrow></msub></math></span> may change signs, <span><math><msub><mrow><mi>f
本文的目的是研究R4中以下混合阶半线性椭圆系统解的惟一性定理:(0.1){(−Δ)12u1(x)=f1(u1,u2,u3,u4),(−Δ)u2(x)=f2(u1,u2,u3,u4),(−Δ)32u3(x)=f3(u1,u2,u3,u4),(−Δ)2u4(x)=f4(u1,u2,u3,u4),其中uj≥0(j=1,2,3), u4可以变号,fi(u1,u2,u3,u4)(i=1,2,3,4)是单调连续函数(可增可减),f4满足有限总曲率条件,即:∫R4f4 (u1, u2, u3, u4) (x) dx< +∞。首先,我们建立了一个等价于(0.1)的积分表示公式,并在特定的假设下证明了关于u4的一个重要的渐近性质。最后,在一定的假设条件下,利用移动法结合积分不等式证明了上述方程在两种不同条件下经典解的唯一性定理。我们的工作建立了半线性椭圆系统的唯一性结果,而不假设非线性是一个非递减函数(只假设非线性是单调函数)。我们还将R4中具有一般非线性项的混合阶椭圆方程推广到Rn的高维情况。
{"title":"Uniqueness theorems for solutions of mixed order elliptic system with general nonlinearity on R4","authors":"Daomin Cao ,&nbsp;Yuxia Guo ,&nbsp;Shaolong Peng","doi":"10.1016/j.matpur.2026.103879","DOIUrl":"10.1016/j.matpur.2026.103879","url":null,"abstract":"&lt;div&gt;&lt;div&gt;The objective of this paper is to investigate the uniqueness theorems for solutions of the following mixed-order semi-linear elliptic system 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;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;:&lt;span&gt;&lt;span&gt;&lt;span&gt;(0.1)&lt;/span&gt;&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msup&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;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&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;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msup&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;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msup&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&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;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; where &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&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;mn&gt;3&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;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; may change signs, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;f","PeriodicalId":51071,"journal":{"name":"Journal de Mathematiques Pures et Appliquees","volume":"209 ","pages":"Article 103879"},"PeriodicalIF":2.3,"publicationDate":"2026-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146175326","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"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
Weak KAM theory for infinite co-dimensional Hamiltonian systems 无限协维哈密顿系统的弱KAM理论
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-05-01 Epub Date: 2026-02-05 DOI: 10.1016/j.matpur.2026.103871
Xun Niu , Kaizhi Wang , Yong Li
This paper establishes several weak KAM type results for Hamiltonian systems with infinite dimensional normal directions, which we call infinite co-dimensional Hamiltonian systems. We first study the Mather's minimization problem for a class of infinite co-dimensional Hamiltonians. Then we prove the existence of weak solutions of the corresponding Hamilton-Jacobi equation which satisfy the equation σ-almost everywhere, where σ is a projected minimal measure satisfying a divergence equation. The abovementioned weak solution transforms the infinite co-dimensional Hamiltonian system into a system with an integrable structure in the weak sense. Finally, we apply our results to a class of one-dimensional nonlinear Schrödinger equations.
本文建立了具有无限维法向的哈密顿系统的几个弱KAM型结果,我们称之为无限协维哈密顿系统。我们首先研究了一类无穷余维哈密顿量的马瑟极小化问题。然后证明了相应的Hamilton-Jacobi方程几乎处处满足σ-的弱解的存在性,其中σ是满足散度方程的投影极小测度。上述弱解将无限协维哈密顿系统转化为弱意义上具有可积结构的系统。最后,我们将我们的结果应用于一类一维非线性Schrödinger方程。
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引用次数: 0
Existence and non-existence for weighted fourth order elliptic problems in exterior domains 加权四阶椭圆型外域问题的存在性与不存在性
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-05-01 Epub Date: 2026-02-05 DOI: 10.1016/j.matpur.2026.103870
Zongming Guo , Jiayu Li , Fangshu Wan
Existence and non-existence for weighted fourth order elliptic problems in exterior domains are studied. The Liouville type results are obtained for the subcritical case and a unique nontrivial nonnegative radial fast-decay solution is obtained for the supercritical case. It is also seen that the nontrivial nonnegative radial solution does not exist for the critical case.
研究了加权四阶椭圆型外域问题的存在性和不存在性。在亚临界情况下得到了Liouville型结果,在超临界情况下得到了唯一的非平凡非负径向快衰解。在临界情况下,非平凡非负径向解不存在。
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引用次数: 0
Regularity theory of a gradient degenerate Neumann problem 梯度退化Neumann问题的正则性理论
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-05-01 Epub Date: 2026-02-05 DOI: 10.1016/j.matpur.2026.103863
William M. Feldman, Zhonggan Huang
We study the regularity and comparison principle for a gradient degenerate Neumann problem. The problem is a generalization of the Signorini or thin obstacle problem which appears in the study of certain singular anisotropic free boundary problems arising from homogenization. In scaling terms, the problem is critical since the gradient degeneracy and the Neumann PDE operator are of the same order. We show the (optimal) C1,12 regularity in dimension d=2 and we show the same regularity result in d3 conditional on the assumption that the degenerate values of the solution do not accumulate. We also prove a comparison principle characterizing minimal supersolutions, which we believe will have applications to homogenization and other related scaling limits.
研究了一类梯度退化Neumann问题的正则性和比较原理。该问题是在研究由均匀化引起的某些奇异各向异性自由边界问题时出现的sigorini问题或薄障碍问题的推广。在尺度方面,这个问题是关键的,因为梯度退化和诺伊曼PDE算子是同一阶的。我们在d=2的维度上展示了(最优)C1,12的规律性,并在假设解的退化值不累积的条件下,在d≥3的维度上展示了相同的规律性结果。我们还证明了表征最小超解的比较原理,我们相信它将应用于均质化和其他相关的缩放极限。
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引用次数: 0
Derivation of Kirchhoff-type plate theories for elastic materials with voids 含孔洞弹性材料的kirchhoff型板理论的推导
IF 2.3 1区 数学 Q1 MATHEMATICS Pub Date : 2026-05-01 Epub Date: 2026-02-06 DOI: 10.1016/j.matpur.2026.103865
Manuel Friedrich , Leonard Kreutz , Konstantinos Zemas
We rigorously derive a Blake-Zisserman-Kirchhoff theory for thin plates with material voids, starting from a three-dimensional model with elastic bulk and interfacial energy featuring a Willmore-type curvature penalization. The effective two-dimensional model comprises a classical elastic bending energy and surface terms which reflect the possibility that voids can persist in the limit, that the limiting plate can be broken apart into several pieces, or that the plate can be folded. Building upon and extending the techniques used in the authors' recent work [34] on the derivation of one-dimensional theories for thin brittle rods with voids, the present contribution generalizes the results of [60], by considering general geometries on the admissible set of voids and constructing recovery sequences for all admissible limiting configurations.
我们从具有弹性体积和具有willmore型曲率惩罚的界面能的三维模型出发,严格推导了具有材料空洞的薄板的Blake-Zisserman-Kirchhoff理论。有效的二维模型包括经典弹性弯曲能和表面项,这些表面项反映了空洞在极限下持续存在的可能性,极限板可以分裂成几块的可能性,或者板可以折叠的可能性。在作者最近关于带孔洞的薄脆棒一维理论推导的工作[34]的基础上,本文通过考虑孔洞集上的一般几何形状和构造所有允许极限构型的恢复序列,推广了[60]的结果。
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引用次数: 0
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Journal de Mathematiques Pures et Appliquees
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