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On the topology of manifolds with positive intermediate curvature 正中间曲率流形的拓扑结构
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-11 DOI: 10.1016/j.aim.2025.110731
Liam Mazurowski , Tongrui Wang , Xuan Yao
We formulate a conjecture relating the topology of a manifold's universal cover with the existence of metrics with positive m-intermediate curvature. We prove the result for manifolds of dimension n{3,4,5} and for most choices of m when n=6. As a corollary, we show that a closed, aspherical 6-manifold cannot admit a metric with positive 4-intermediate curvature.
给出了流形泛盖拓扑与正m-中间曲率度量的存在性之间的一个猜想。我们证明了维数n∈{3,4,5}的流形和当n=6时m的大多数选择的结果。作为一个推论,我们证明了一个封闭的非球面6流形不允许有正4中间曲率的度规。
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引用次数: 0
The tt*-Toda equations of An type An型的tt*-Toda方程
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-10 DOI: 10.1016/j.aim.2025.110730
Martin A. Guest , Alexander R. Its , Chang-Shou Lin
The purpose of this article is to answer comprehensively, with self-contained proofs, a longstanding question posed by the physicists Cecotti and Vafa in the 1990's concerning solutions of the topological-antitopological fusion equations of Toda type, the An tt*-Toda equations. These equations are also of interest in differential geometry and the theory of integrable systems as a certain real form of the radial Toda equations. We describe the complete set of solutions explicitly in terms of their asymptotics, and in terms of their Stokes data. In view of the wide-ranging nature of our methods, we also provide explanatory remarks intended to make the article accessible to researchers in different areas.
本文的目的是用完备的证据全面地回答物理学家Cecotti和Vafa在20世纪90年代提出的一个长期存在的问题,该问题涉及Toda型拓扑-反拓扑融合方程的解,即An tt*-Toda方程。这些方程在微分几何和可积系统理论中也很有意义,它们是径向Toda方程的某种实形式。我们根据解的渐近性和Stokes数据明确地描述了解的完备集。鉴于我们方法的广泛性,我们还提供了解释性注释,旨在使不同领域的研究人员可以访问本文。
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引用次数: 0
Nearby cycles commute with proper direct image on stacks of shtukas 附近的自行车通勤时,在一堆木卡上有适当的直接图像
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-10 DOI: 10.1016/j.aim.2025.110729
Arnaud Eteve, Cong Xue
Let G be a generically reductive group over a smooth projective curve X over a finite field. For any finite set I, we show that nearby cycles commute with proper direct image from stacks of shtukas to XI. This generalizes some results of Salmon and the authors.
设G是有限域上光滑投影曲线X上的一般约化群。对于任意有限集I,我们证明了邻近环可以用适当的直接像从shtukas堆交换到XI。这概括了萨尔蒙和作者的一些结果。
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引用次数: 0
Towards 2-derivators for formal ∞-category theory 关于形式∞范畴论的2导函数
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-10 DOI: 10.1016/j.aim.2025.110726
Nicola Di Vittorio
Derivators, introduced independently by Grothendieck and Heller in the 1980s, provide a categorical framework for studying homotopy theory. They are based on the idea that, while the homotopy 1-category of a single model category or (,1)-category retains only limited information, the structured collection of homotopy 1-categories of diagram categories often suffices for many homotopical purposes. In this paper, we introduce a set of axioms for a 2-dimensional analog of derivators: a refinement of the homotopy 2-category of an enriched model category or (,2)-category into a coherent system of homotopy 2-categories of higher categories of diagrams. We show that these axioms are satisfied in a variety of models, including standard ones related to (,1)-category theory. Moreover, we prove that the axioms are preserved under a certain shift operation.
衍生子是Grothendieck和Heller在20世纪80年代独立提出的,它为研究同伦理论提供了一个范畴框架。它们基于这样的思想:当单个模型范畴的同伦1-范畴或(∞,1)-范畴只保留有限的信息时,图范畴的同伦1-范畴的结构化集合通常足以满足许多同伦目的。本文引入了一类二维类似导数的公理:将富模型范畴的同伦2-范畴或(∞,2)-范畴细化为图的高范畴的同伦2-范畴的相干系统。我们证明了这些公理在各种模型中都是满足的,包括与(∞,1)-范畴论相关的标准模型。此外,我们还证明了这些公理在一定的移位操作下是保持的。
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引用次数: 0
Locality in sumsets 日落的局部性
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-09 DOI: 10.1016/j.aim.2025.110727
Peter van Hintum , Peter Keevash
<div><div>Motivated by the Polynomial Freiman-Ruzsa (PFR) Conjecture, we develop a theory of locality in sumsets, with several applications to John-type approximation and stability of sets with small doubling. One highlight shows that if <span><math><mi>A</mi><mo>⊂</mo><mi>Z</mi></math></span> with <span><math><mo>|</mo><mi>A</mi><mo>+</mo><mi>A</mi><mo>|</mo><mo>≤</mo><mo>(</mo><mn>1</mn><mo>−</mo><mi>ϵ</mi><mo>)</mo><msup><mrow><mn>2</mn></mrow><mrow><mi>d</mi></mrow></msup><mo>|</mo><mi>A</mi><mo>|</mo></math></span> is non-degenerate then <em>A</em> is covered by <span><math><mi>O</mi><mo>(</mo><msup><mrow><mn>2</mn></mrow><mrow><mi>d</mi></mrow></msup><mo>)</mo></math></span> translates of a <em>d</em>-dimensional generalised arithmetic progression (<em>d</em>-GAP) <em>P</em> with <span><math><mo>|</mo><mi>P</mi><mo>|</mo><mo>≤</mo><msub><mrow><mi>O</mi></mrow><mrow><mi>d</mi><mo>,</mo><mi>ϵ</mi></mrow></msub><mo>(</mo><mo>|</mo><mi>A</mi><mo>|</mo><mo>)</mo></math></span>; thus we obtain one of the polynomial bounds required by PFR, under the non-degeneracy assumption that <em>A</em> is not efficiently covered by <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>d</mi><mo>,</mo><mi>ϵ</mi></mrow></msub><mo>(</mo><mn>1</mn><mo>)</mo></math></span> translates of a <span><math><mo>(</mo><mi>d</mi><mo>−</mo><mn>1</mn><mo>)</mo></math></span>-GAP.</div><div>We also prove a stability result showing for any <span><math><mi>ϵ</mi><mo>,</mo><mi>α</mi><mo>></mo><mn>0</mn></math></span> that if <span><math><mi>A</mi><mo>⊆</mo><mi>Z</mi></math></span> with <span><math><mo>|</mo><mi>A</mi><mo>+</mo><mi>A</mi><mo>|</mo><mo>≤</mo><mo>(</mo><mn>2</mn><mo>−</mo><mi>ϵ</mi><mo>)</mo><msup><mrow><mn>2</mn></mrow><mrow><mi>d</mi></mrow></msup><mo>|</mo><mi>A</mi><mo>|</mo></math></span> is non-degenerate then some <span><math><msup><mrow><mi>A</mi></mrow><mrow><mo>′</mo></mrow></msup><mo>⊂</mo><mi>A</mi></math></span> with <span><math><mo>|</mo><msup><mrow><mi>A</mi></mrow><mrow><mo>′</mo></mrow></msup><mo>|</mo><mo>></mo><mo>(</mo><mn>1</mn><mo>−</mo><mi>α</mi><mo>)</mo><mo>|</mo><mi>A</mi><mo>|</mo></math></span> is efficiently covered by either a <span><math><mo>(</mo><mi>d</mi><mo>+</mo><mn>1</mn><mo>)</mo></math></span>-GAP or <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>α</mi></mrow></msub><mo>(</mo><mn>1</mn><mo>)</mo></math></span> translates of a <em>d</em>-GAP. This ‘dimension-free’ bound for approximate covering makes for a surprising contrast with exact covering, where the required number of translates not only grows with <em>d</em>, but does so exponentially. Another highlight shows that if <span><math><mi>A</mi><mo>⊂</mo><mi>Z</mi></math></span> is non-degenerate with <span><math><mo>|</mo><mi>A</mi><mo>+</mo><mi>A</mi><mo>|</mo><mo>≤</mo><mo>(</mo><msup><mrow><mn>2</mn></mrow><mrow><mi>d</mi></mrow></msup><mo>+</mo><mi>ℓ</mi><mo>)</mo><mo>|</mo><mi>A</mi><mo>|</mo></math></span> and <span><math><mi>ℓ</mi><mo>≤</mo><mn>0.1</mn><mo>⋅</m
在多项式Freiman-Ruzsa (PFR)猜想的启发下,我们建立了sumset的局域性理论,并将其应用于小倍集的john型逼近和稳定性。一个重点表明,如果A∧Z与|A+A|≤(1−λ)2d|A|是非简并的,则A被一个d维广义等差数列(d-GAP) P的O(2d)平移覆盖,其中|P|≤Od, λ (|A|);因此,我们得到了PFR所需的多项式界之一,在非简并假设A没有被Od有效覆盖的情况下,A (d−1)-GAP的λ(1)平移。我们还证明了一个稳定性结果,表明对于任意一个λ,α>0,如果a≤| a + a≤(2−λ)2d| a≤| a≤|是不简并的,则某些a′∧a≤| a′∧|>;(1−α)| a≤|被a (d+1)-GAP或d-GAP的Oα(1)平移覆盖。近似覆盖的“无维”边界与精确覆盖形成了惊人的对比,在精确覆盖中,所需的转换次数不仅随d增长,而且呈指数增长。另一个亮点是,如果A∧Z是非简并的,且|A+A|≤(2d+ r)|A|,且r≤0.1⋅2d,则A被一个d-GAP P的r +1平移所覆盖,且|P|≤Od(|A|);这是紧密的,因为不能用更小的数来代替。上述结果也适用于A∧Rd,用gap和凸体的一个合适的共同推广来代替gap,我们称之为广义凸级数。在这种情况下,非简并性条件自动成立,因此我们得到了本质上最优的界,在A上没有附加的假设。这里我们证明,如果A´Rk满足|A+A2|≤(1+δ)|A|,且δ∈(0,1),则∃A´∧A与|A′|≥(1−δ)|A|,使得|co(A′)|≤Ok,1−δ(|A|)。这是相等集的Brunn-Minkowski不等式的一个维度无关的锐稳定性结果,它暗示了pracemoppa - leindler不等式可能的类似物。这些结果都是从一个统一理论中推导出来的,在这个统一理论中,我们引入了一个新的任何集合的内在结构近似,我们称之为“加性壳”,并通过对弗里曼定理的改进来发展它的理论,并具有额外的分离特性。另一个将单独发表的应用是Ruzsa离散布伦-闵可夫斯基猜想的证明。
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One highlight shows that if &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&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;mi&gt;ϵ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is non-degenerate then &lt;em&gt;A&lt;/em&gt; is covered by &lt;span&gt;&lt;math&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; translates of a &lt;em&gt;d&lt;/em&gt;-dimensional generalised arithmetic progression (&lt;em&gt;d&lt;/em&gt;-GAP) &lt;em&gt;P&lt;/em&gt; with &lt;span&gt;&lt;math&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;ϵ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;; thus we obtain one of the polynomial bounds required by PFR, under the non-degeneracy assumption that &lt;em&gt;A&lt;/em&gt; is not efficiently covered by &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;ϵ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&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; translates of a &lt;span&gt;&lt;math&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&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;-GAP.&lt;/div&gt;&lt;div&gt;We also prove a stability result showing for any &lt;span&gt;&lt;math&gt;&lt;mi&gt;ϵ&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; that if &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;⊆&lt;/mo&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;ϵ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is non-degenerate then some &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;A&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;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;A&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;&gt;&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is efficiently covered by either a &lt;span&gt;&lt;math&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&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;-GAP or &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&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; translates of a &lt;em&gt;d&lt;/em&gt;-GAP. This ‘dimension-free’ bound for approximate covering makes for a surprising contrast with exact covering, where the required number of translates not only grows with &lt;em&gt;d&lt;/em&gt;, but does so exponentially. Another highlight shows that if &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is non-degenerate with &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;0.1&lt;/mn&gt;&lt;mo&gt;⋅&lt;/m","PeriodicalId":50860,"journal":{"name":"Advances in Mathematics","volume":"485 ","pages":"Article 110727"},"PeriodicalIF":1.5,"publicationDate":"2025-12-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145749187","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
Rigidity of saddle loops 鞍形环刚度
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-08 DOI: 10.1016/j.aim.2025.110712
Daniel Panazzolo , Maja Resman , Loïc Teyssier
A saddle loop is a germ of a holomorphic foliation near a homoclinic saddle connection. We prove that they are classified by their Poincaré first-return map. We also prove that they are formally rigid when the Poincaré map is multivalued. Finally, we provide a list of all analytic classes of Liouville-integrable saddle loops.
鞍环是在同斜鞍连接附近的全纯叶的胚芽。我们证明了它们是由它们的poincar首回图来分类的。我们还证明了当庞卡罗映射是多值映射时它们是形式刚性的。最后,我们给出了所有liouville可积鞍环的解析类的列表。
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引用次数: 0
The modified Camassa-Holm equation with nonzero background: Soliton resolution conjecture and asymptotic stability of N-soliton solutions 具有非零背景的修正Camassa-Holm方程:n -孤子解的孤子分辨猜想和渐近稳定性
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-03 DOI: 10.1016/j.aim.2025.110552
Jin-Jie Yang, Shou-Fu Tian , Zhi-Qiang Li
<div><div>We consider the long-time asymptotic behavior of the modified Camassa-Holm (mCH) equation with finite density initial data<span><span><span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>+</mo><msub><mrow><mo>(</mo><mo>(</mo><msup><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><msubsup><mrow><mi>u</mi></mrow><mrow><mi>x</mi></mrow><mrow><mn>2</mn></mrow></msubsup><mo>)</mo><mi>m</mi><mo>)</mo></mrow><mrow><mi>x</mi></mrow></msub><mo>=</mo><mn>0</mn><mo>,</mo><mspace></mspace><mi>m</mi><mo>=</mo><mi>u</mi><mo>−</mo><msub><mrow><mi>u</mi></mrow><mrow><mi>x</mi><mi>x</mi></mrow></msub><mo>,</mo><mspace></mspace><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>∈</mo><mi>R</mi><mo>×</mo><msup><mrow><mi>R</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>,</mo><mi>u</mi><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo><mo>=</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>,</mo><mspace></mspace><mspace></mspace><munder><mi>lim</mi><mrow><mi>x</mi><mo>→</mo><mo>±</mo><mo>∞</mo></mrow></munder><mo>⁡</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>=</mo><mn>1</mn><mo>,</mo><mspace></mspace><mspace></mspace><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mn>1</mn><mo>∈</mo><msup><mrow><mi>H</mi></mrow><mrow><mn>4</mn><mo>,</mo><mn>1</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo><mo>,</mo></math></span></span></span> where <span><math><msub><mrow><mi>m</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>:</mo><mo>=</mo><mi>m</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>=</mo><mn>0</mn><mo>)</mo></math></span> and <span><math><msub><mrow><mi>m</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mn>1</mn><mo>∈</mo><msup><mrow><mi>H</mi></mrow><mrow><mn>2</mn><mo>,</mo><mn>1</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo></math></span>. By deforming the Lax pair of the mCH equation, we successfully establish a well-defined mapping from initial values to reflection coefficients. Then by developing the <span><math><mover><mrow><mo>∂</mo></mrow><mo>‾</mo></mover></math></span>-nonlinear steepest descent method, we reveal that the mCH equation has four different asymptotic regions depending on <span><math><mi>τ</mi><mo>:</mo><mo>=</mo><mi>x</mi><mo>/</mo><mi>t</mi></math></span>. For the region <span><math><mi>τ</mi><mo>∈</mo><mo>(</mo><mo>−</mo><mo>∞</mo><mo>,</mo><mn>3</mn><mo>/</mo><mn>4</mn><mo>)</mo><mo>∪</mo><mo>(</mo><mn>3</mn><mo>,</mo><mo>∞</mo><mo>)</mo></math></span> without steady-state phase points, we strictly prove that the solution of the mCH equation can be characterized by the soliton solution and an error term, and further prove the asymptotic stability of the <em>N</em>-soliton solution. In the regions <span><math><mi>τ</mi><mo>∈</mo><mo>(</mo><mn>3</mn><mo>/</mo><mn>4</mn><mo>,</mo><mn>1</mn
考虑有限密度初始数据t+((u2 - ux2)m)x=0,m=u - uxx,(x,t)∈R×R+,u(x,0)=u0(x),limx→±∞∑u0(x)=1,u0(x)−1∈h4,1 (R),其中m0(x):=m(x,t=0)和m0(x)−1∈H2,1(R)的修正Camassa-Holm (mCH)方程的长时间渐近性质。通过对mCH方程的Lax对的变形,我们成功地建立了从初值到反射系数的良好定义映射。然后,通过开发∂不要紧非线性最陡下降法,我们揭示了mCH方程有四个不同的渐近区域,这取决于τ:=x/t。对于无稳态相点的区域τ∈(−∞,3/4)∪(3,∞),我们严格证明了mCH方程的解可以用孤子解和误差项来表征,并进一步证明了n -孤子解的渐近稳定性。在τ∈(3/4,1)和τ∈(1,3)区域中,相函数θ(z)分别有8个和4个稳态相点。我们的研究结果严格分析了具有有限密度初值的mCH方程解在四个不同区域的长时间渐近行为,不仅证明了孤子分辨猜想,而且证明了n -孤子解的渐近稳定性。
{"title":"The modified Camassa-Holm equation with nonzero background: Soliton resolution conjecture and asymptotic stability of N-soliton solutions","authors":"Jin-Jie Yang,&nbsp;Shou-Fu Tian ,&nbsp;Zhi-Qiang Li","doi":"10.1016/j.aim.2025.110552","DOIUrl":"10.1016/j.aim.2025.110552","url":null,"abstract":"&lt;div&gt;&lt;div&gt;We consider the long-time asymptotic behavior of the modified Camassa-Holm (mCH) equation with finite density initial data&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&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;/msup&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;x&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;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;u&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;mi&gt;x&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;R&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;/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;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&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;0&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;mspace&gt;&lt;/mspace&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;munder&gt;&lt;mi&gt;lim&lt;/mi&gt;&lt;mrow&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;/munder&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;0&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;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&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;H&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&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;mi&gt;R&lt;/mi&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; where &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&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;H&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&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;mi&gt;R&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. By deforming the Lax pair of the mCH equation, we successfully establish a well-defined mapping from initial values to reflection coefficients. Then by developing the &lt;span&gt;&lt;math&gt;&lt;mover&gt;&lt;mrow&gt;&lt;mo&gt;∂&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;‾&lt;/mo&gt;&lt;/mover&gt;&lt;/math&gt;&lt;/span&gt;-nonlinear steepest descent method, we reveal that the mCH equation has four different asymptotic regions depending on &lt;span&gt;&lt;math&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;. For the region &lt;span&gt;&lt;math&gt;&lt;mi&gt;τ&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;mn&gt;3&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∪&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;3&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; without steady-state phase points, we strictly prove that the solution of the mCH equation can be characterized by the soliton solution and an error term, and further prove the asymptotic stability of the &lt;em&gt;N&lt;/em&gt;-soliton solution. In the regions &lt;span&gt;&lt;math&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;1&lt;/mn","PeriodicalId":50860,"journal":{"name":"Advances in Mathematics","volume":"484 ","pages":"Article 110552"},"PeriodicalIF":1.5,"publicationDate":"2025-12-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145693585","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
Pluriclosed flow and the Hull-Strominger system 多闭流和赫尔-施特罗明格系统
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-01 DOI: 10.1016/j.aim.2025.110699
Mario Garcia-Fernandez , Raul Gonzalez Molina , Jeffrey Streets
We define a natural extension of pluriclosed flow aiming at constructing solutions of the Hull-Strominger system. We give several geometric formulations of this flow, which yield a series of a priori estimates for the flow and also for the Hull-Strominger system. The evolution equations are derived using the theory of string algebroids, a class of Courant algebroids which occur naturally in higher gauge theory. Using this, we interpret the flow as generalized Ricci flow and also as a higher/coupled version of Hermitian-Yang-Mills flow, proving furthermore that it is compatible with symmetry reduction. Regarding analytical results, we prove a priori C estimates for uniformly parabolic solutions. This in particular settles the question of smooth regularity of uniformly elliptic solutions of the Hull-Strominger system, generalizing Yau's C3 estimate for the complex Monge-Ampère equation. We prove global existence and convergence results for the flow on special backgrounds, and discuss a conjectural relationship of the flow to the geometrization of Reid's fantasy.
为了构造Hull-Strominger系统的解,我们定义了多闭流的一个自然扩展。我们给出了这种流动的几个几何公式,这些公式产生了一系列的流动和赫尔-施特罗明格系统的先验估计。利用高规范理论中自然存在的一类Courant代数群——弦代数群理论,推导了演化方程。利用这一点,我们将流解释为广义Ricci流,也解释为Hermitian-Yang-Mills流的更高/耦合版本,进一步证明了它与对称约简相容。关于解析结果,我们证明了一致抛物型解的先验C∞估计。这特别地解决了Hull-Strominger系统一致椭圆解的光滑正则性问题,推广了Yau对复monge - amp方程的C3估计。我们证明了流在特殊背景下的整体存在性和收敛性结果,并讨论了流与里德幻想几何化的推测关系。
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引用次数: 0
Essential graded algebra over polynomial rings with real exponents 实指数多项式环上的基本渐变代数
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-01 DOI: 10.1016/j.aim.2025.110682
Ezra Miller
The geometric and algebraic theory of monomial ideals and multigraded modules is initiated over real-exponent polynomial rings and, more generally, monoid algebras for real polyhedral cones. The main results include the generalization of Nakayama's lemma; complete theories of minimal and dense primary, secondary, and irreducible decomposition, including associated and attached faces; socles and tops; minimality and density for downset hulls, upset covers, and fringe presentations; Matlis duality; and geometric analysis of staircases. Modules that are semialgebraic or piecewise-linear (PL) have the relevant property preserved by functorial constructions as well as by minimal primary and secondary decompositions. And when the modules in question are subquotients of the group itself, such as monomial ideals and quotients modulo them, minimal primary and secondary decompositions are canonical, as are irreducible decompositions up to the new real-exponent notion of density.
在实指数多项式环和更一般的实多面体锥的一元代数上,开始了单项式理想和多阶模的几何和代数理论。主要成果包括:中山引理的推广;完整的最小和密集的原生、次生和不可约分解理论,包括相关面和附着面;鞋跟和鞋帮;最小和密度的下置船体,翻转盖,和边缘展示;Matlis二元性;以及楼梯的几何分析。半代数或分段线性(PL)的模块具有功能结构以及最小初等分解和次要分解所保留的相关性质。当所讨论的模是群本身的子商时,比如单项式理想和对它们模的商,最小初等分解和次分解是正则的,就像不可约分解直到新的实指数密度概念一样。
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引用次数: 0
Exponential mixing of all orders and CLT for automorphisms of compact Kähler manifolds 紧态Kähler流形自同构的全阶指数混合及CLT
IF 1.5 1区 数学 Q1 MATHEMATICS Pub Date : 2025-12-01 DOI: 10.1016/j.aim.2025.110689
Fabrizio Bianchi , Tien-Cuong Dinh
We consider the unique measure of maximal entropy of an automorphism of a compact Kähler manifold with simple action on cohomology. We show that it is exponentially mixing of all orders with respect to Hölder observables. It follows that the Central Limit Theorem (CLT) holds for these observables. In particular, our result applies to all automorphisms of compact Kähler surfaces with positive entropy.
考虑上同调上作用简单的紧Kähler流形的自同构最大熵的唯一测度。我们证明了它是关于Hölder可观测值的所有阶的指数混合。由此可见,中心极限定理(CLT)对这些可观测值成立。特别地,我们的结果适用于所有具有正熵的紧致Kähler曲面的自同构。
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引用次数: 0
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