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Optimal bounds for the Dunkl kernel in the dihedral case 二面情况下邓克尔核的最优边界
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-07 DOI: 10.1016/j.jfa.2024.110743
Jean-Philippe Anker , Bartosz Trojan
We establish sharp upper and lower estimates of the Dunkl kernel in the case of dihedral groups.
在二面群的情况下,我们建立了邓克尔核的尖锐上下估计值。
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引用次数: 0
Scalar curvature rigidity and the higher mapping degree 标量曲率刚度和高映射度
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-07 DOI: 10.1016/j.jfa.2024.110744
Thomas Tony
A closed connected oriented Riemannian manifold N with non-vanishing Euler characteristic, non-negative curvature operator and 0<2RicN<scalN is area-rigid in the sense that any area non-increasing spin map f:MN with non-vanishing Aˆ-degree and scalMscalNf is a Riemannian submersion with scalM=scalNf. This is due to Goette and Semmelmann and generalizes a result by Llarull. In this article, we show area-rigidity for not necessarily orientable manifolds with respect to a larger class of maps f:MN by replacing the topological condition on the Aˆ-degree by a less restrictive condition involving the so-called higher mapping degree. This includes fiber bundles over even dimensional spheres with enlargeable fibers, e.g. pr1:S2n×TkS2n. We develop a technique to extract from a non-vanishing higher index a geometrically useful family of almost
-harmonic sections. This also leads to a new proof of the fact that any closed connected spin manifold with non-negative scalar curvature and non-trivial Rosenberg index is Ricci flat.
一个封闭连通的定向黎曼流形 N,其欧拉特征非递减,曲率算子非负,且 0<2RicN<scalN 是面积刚性的,即任何面积非递增的自旋映射 f:M→N 的 Aˆ度非递减且 scalM≥scalN∘f 是一个黎曼潜影,scalM=scalN∘f。这归功于 Goette 和 Semmelmann,并推广了 Llarull 的一个结果。在这篇文章中,我们用一个涉及所谓高映射度的限制性较小的条件取代了关于 Aˆ度的拓扑条件,从而证明了不一定是可定向流形的面积刚度,即关于更大一类映射 f:M→N 的面积刚度。这包括偶数维球面上具有可放大纤维的纤维束,例如 pr1:S2n×Tk→S2n。我们开发了一种技术,可以从非矢量高指数中提取几何上有用的近谐波截面族。这也引出了一个新的证明,即任何具有非负标量曲率和非三重罗森伯格指数的封闭连通自旋流形都是利玛窦平坦的。
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引用次数: 0
C⁎-algebras associated to directed graphs of groups, and models of Kirchberg algebras 与群的有向图相关联的 C⁎ 算法,以及基希贝格算法模型
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110740
Victor Wu
We introduce C-algebras associated to directed graphs of groups. In particular, we associate a combinatorial C-algebra to each row-finite directed graph of groups with no sources, and show that this C-algebra is Morita equivalent to the crossed product coming from the corresponding group action on the boundary of a directed tree. Finally, we show that these C-algebras (and their Morita equivalent crossed products) contain the class of stable UCT Kirchberg algebras.
我们介绍与有向群图相关联的 C⁎-代数。特别是,我们将一个组合 C⁎-代数与每个无源群的行无限有向图关联起来,并证明这个 C⁎-代数等价于有向树边界上相应群作用的交叉积。最后,我们证明这些 C⁎-代数(及其莫里塔等价交叉积)包含稳定的 UCT 基希贝格代数类。
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引用次数: 0
Pure ⁎-homomorphisms 纯⁎同构
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110739
Joan Bosa , Eduard Vilalta
We introduce and study the notion of pureness for *-homomorphisms and, more generally, for cpc order-zero maps. After providing various important examples of pureness, we show our main result: Any composition of two pure maps factors through a pure object up to Cuntz equivalence. This is used to obtain several factorization results at the level of C-algebras.
我们介绍并研究了*同态的纯粹性概念,更广义地说,介绍并研究了cpc零阶映射的纯粹性概念。在提供了纯合性的各种重要例子之后,我们展示了我们的主要结果:两个纯映射的任何组合都会通过一个纯对象进行因式分解,直到昆兹等价。利用这一结果,我们可以在 C⁎-gebras 层面上得到几个因式分解结果。
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引用次数: 0
Multi-window STFT phase retrieval: Lattice uniqueness 多窗口 STFT 相位检索:晶格唯一性
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110733
Philipp Grohs , Lukas Liehr , Martin Rathmair
<div><div>Short-time Fourier transform (STFT) phase retrieval refers to the reconstruction of a function <em>f</em> from its spectrogram, i.e., the magnitudes of its short-time Fourier transform <span><math><msub><mrow><mi>V</mi></mrow><mrow><mi>g</mi></mrow></msub><mi>f</mi></math></span> with window function <em>g</em>. While it is known that for appropriate windows, any function <span><math><mi>f</mi><mo>∈</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo></math></span> can be reconstructed from the full spectrogram <span><math><mo>|</mo><msub><mrow><mi>V</mi></mrow><mrow><mi>g</mi></mrow></msub><mi>f</mi><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo><mo>|</mo></math></span>, in practical scenarios, the reconstruction must be achieved from discrete samples, typically taken on a lattice. It turns out that the sampled problem becomes much more subtle: recent results have demonstrated that uniqueness via lattice-sampling is unachievable, irrespective of the choice of the window function or the lattice density. In the present paper, we initiate the study of multi-window STFT phase retrieval as a way to effectively bypass the discretization barriers encountered in the single-window case. By establishing a link between multi-window Gabor systems, sampling in Fock space, and phase retrieval for finite frames, we derive conditions under which square-integrable functions can be uniquely recovered from spectrogram samples on a lattice. Specifically, we provide conditions on window functions <span><math><msub><mrow><mi>g</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><mo>…</mo><mo>,</mo><msub><mrow><mi>g</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>∈</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo></math></span>, such that every <span><math><mi>f</mi><mo>∈</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo></math></span> is determined up to a global phase from<span><span><span><math><mrow><mo>(</mo><mo>|</mo><msub><mrow><mi>V</mi></mrow><mrow><msub><mrow><mi>g</mi></mrow><mrow><mn>1</mn></mrow></msub></mrow></msub><mi>f</mi><mo>(</mo><mi>A</mi><msup><mrow><mi>Z</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo><mo>|</mo><mo>,</mo><mspace></mspace><mo>…</mo><mo>,</mo><mspace></mspace><mo>|</mo><msub><mrow><mi>V</mi></mrow><mrow><msub><mrow><mi>g</mi></mrow><mrow><mn>4</mn></mrow></msub></mrow></msub><mi>f</mi><mo>(</mo><mi>A</mi><msup><mrow><mi>Z</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo><mo>|</mo><mo>)</mo></mrow></math></span></span></span> whenever <span><math><mi>A</mi><mo>∈</mo><msub><mrow><mi>GL</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>R</mi><mo>)</mo></math></span> satisfies the density condition <span><math><mo>|</mo><mi>det</mi><mo>⁡</mo><mi>A</mi><msup><mrow><mo>|</mo></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mo>≥</mo><mn>4</mn></math></span>. For real
短时傅里叶变换(STFT)相位检索是指从函数 f 的频谱图(即其短时傅里叶变换 Vgf 与窗口函数 g 的大小)中重建函数 f。众所周知,对于适当的窗口,任何函数 f∈L2(R) 都可以从完整的频谱图 |Vgf(R2)| 中重建,但在实际应用中,重建必须从离散采样(通常在晶格上采样)中实现。事实证明,采样问题变得更加微妙:最近的研究结果表明,无论窗口函数或网格密度如何选择,通过网格采样都无法实现唯一性。在本文中,我们开始研究多窗口 STFT 相位检索,以此有效绕过单窗口情况下遇到的离散化障碍。通过在多窗口 Gabor 系统、Fock 空间采样和有限帧相位检索之间建立联系,我们推导出了从网格上的频谱图样本中唯一恢复方积分函数的条件。具体来说,我们提供了窗口函数 g1、......、g4∈L2(R) 的条件,只要 A∈GL2(R) 满足密度条件 |detA|-1≥4,则每个 f∈L2(R) 的全局相位都是由(|Vg1f(AZ2)|,......,|Vg4f(AZ2)|)确定的。对于实值函数,|detA|-1≥2 的密度就足够了。同时还显示了不规则采样的相应结果。
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While it is known that for appropriate windows, any function &lt;span&gt;&lt;math&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&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; can be reconstructed from the full spectrogram &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;f&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;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, in practical scenarios, the reconstruction must be achieved from discrete samples, typically taken on a lattice. It turns out that the sampled problem becomes much more subtle: recent results have demonstrated that uniqueness via lattice-sampling is unachievable, irrespective of the choice of the window function or the lattice density. In the present paper, we initiate the study of multi-window STFT phase retrieval as a way to effectively bypass the discretization barriers encountered in the single-window case. By establishing a link between multi-window Gabor systems, sampling in Fock space, and phase retrieval for finite frames, we derive conditions under which square-integrable functions can be uniquely recovered from spectrogram samples on a lattice. Specifically, we provide conditions on window functions &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;g&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;mo&gt;…&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;g&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;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&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;mi&gt;R&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, such that every &lt;span&gt;&lt;math&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&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; is determined up to a global phase from&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Z&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;mo&gt;|&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mo&gt;…&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;Z&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;mo&gt;|&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; whenever &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;GL&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;R&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; satisfies the density condition &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;det&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mi&gt;A&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;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;. For real","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110733"},"PeriodicalIF":1.7,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142659892","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
Corrigendum to “Classifying decomposition and wavelet coorbit spaces using coarse geometry” [J. Funct. Anal. 283(9) (2022) 109637] 利用粗几何学对分解和小波同位空间进行分类》[《函数分析杂志》283(9) (2022) 109637]勘误表
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110714
Hartmut Führ , René Koch
{"title":"Corrigendum to “Classifying decomposition and wavelet coorbit spaces using coarse geometry” [J. Funct. Anal. 283(9) (2022) 109637]","authors":"Hartmut Führ ,&nbsp;René Koch","doi":"10.1016/j.jfa.2024.110714","DOIUrl":"10.1016/j.jfa.2024.110714","url":null,"abstract":"","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110714"},"PeriodicalIF":1.7,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142593732","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Constructing non-AMNM weighted convolution algebras for every semilattice of infinite breadth 为每个无限广度半网格构建非AMNM加权卷积代数
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110735
Yemon Choi , Mahya Ghandehari , Hung Le Pham
The AMNM property for commutative Banach algebras is a form of Ulam stability for multiplicative linear functionals. We show that on any semilattice of infinite breadth, one may construct a weight for which the resulting weighted convolution algebra fails to have the AMNM property. Our work is the culmination of a trilogy started in [4] and continued in [5]. In particular, we obtain a refinement of the main result of [5], by establishing a dichotomy for union-closed set systems that has a Ramsey-theoretic flavour.
巴拿赫交换代数的 AMNM 特性是乘法线性函数的乌兰稳定性的一种形式。我们的研究表明,在任何无限宽的半网格上,我们都可以构造一个权值,由此得到的加权卷积代数不具有 AMNM 性质。我们的研究是始于 [4] 并延续于 [5] 的三部曲的顶点。特别是,我们通过建立具有拉姆齐理论色彩的联合封闭集系统二分法,得到了 [5] 主要结果的完善。
{"title":"Constructing non-AMNM weighted convolution algebras for every semilattice of infinite breadth","authors":"Yemon Choi ,&nbsp;Mahya Ghandehari ,&nbsp;Hung Le Pham","doi":"10.1016/j.jfa.2024.110735","DOIUrl":"10.1016/j.jfa.2024.110735","url":null,"abstract":"<div><div>The AMNM property for commutative Banach algebras is a form of Ulam stability for multiplicative linear functionals. We show that on any semilattice of infinite breadth, one may construct a weight for which the resulting weighted convolution algebra fails to have the AMNM property. Our work is the culmination of a trilogy started in <span><span>[4]</span></span> and continued in <span><span>[5]</span></span>. In particular, we obtain a refinement of the main result of <span><span>[5]</span></span>, by establishing a dichotomy for union-closed set systems that has a Ramsey-theoretic flavour.</div></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110735"},"PeriodicalIF":1.7,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142659807","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Approximated harmonic maps with tension fields in Zygmund class 具有齐格蒙类张力场的近似谐波映射
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110736
Jiayu Li , Xiangrong Zhu
Suppose that u is a map from D8 to a compact smooth Riemannian manifold N with bounded energy. We show that there exists a constant λ>0 which depends only on N and E(u,D8) such that if the tension field τ belongs to Zygmund class LlnλL(D8), then the Hopf differential of u belongs to the Zygmund class Lln3L(D1) and the norm hLln3L(D1) depends only on N,E(u,D8) and τLlnλL(D8). As a direct corollary, we obtain the energy identity and necklessness of a blow-up sequence un with bounded energy E(un) and bounded τ(un) in LlnλL(D8).
假设 u 是一个从 D8 到紧凑光滑黎曼流形 N 的有界能的映射。我们将证明存在一个常数 λ>;0,使得如果张力场τ属于齐格蒙类 LlnλL(D8),那么u 的霍普夫微分属于齐格蒙类 Lln3L(D1),且规范‖h‖Lln3L(D1)只取决于 N、E(u,D8) 和‖τ‖LlnλL(D8)。作为直接推论,我们得到了在 LlnλL(D8) 中具有有界能量 E(un) 和有界 τ(un) 的炸裂序列 un 的能量同一性和无颈性。
{"title":"Approximated harmonic maps with tension fields in Zygmund class","authors":"Jiayu Li ,&nbsp;Xiangrong Zhu","doi":"10.1016/j.jfa.2024.110736","DOIUrl":"10.1016/j.jfa.2024.110736","url":null,"abstract":"<div><div>Suppose that <em>u</em> is a map from <span><math><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub></math></span> to a compact smooth Riemannian manifold <em>N</em> with bounded energy. We show that there exists a constant <span><math><mi>λ</mi><mo>&gt;</mo><mn>0</mn></math></span> which depends only on <em>N</em> and <span><math><mi>E</mi><mo>(</mo><mi>u</mi><mo>,</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub><mo>)</mo></math></span> such that if the tension field <em>τ</em> belongs to Zygmund class <span><math><mi>L</mi><msup><mrow><mi>ln</mi></mrow><mrow><mi>λ</mi></mrow></msup><mo>⁡</mo><mi>L</mi><mo>(</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub><mo>)</mo></math></span>, then the Hopf differential of <em>u</em> belongs to the Zygmund class <span><math><mi>L</mi><msup><mrow><mi>ln</mi></mrow><mrow><mn>3</mn></mrow></msup><mo>⁡</mo><mi>L</mi><mo>(</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></math></span> and the norm <span><math><msub><mrow><mo>‖</mo><mi>h</mi><mo>‖</mo></mrow><mrow><mi>L</mi><msup><mrow><mi>ln</mi></mrow><mrow><mn>3</mn></mrow></msup><mo>⁡</mo><mi>L</mi><mo>(</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow></msub></math></span> depends only on <span><math><mi>N</mi><mo>,</mo><mi>E</mi><mo>(</mo><mi>u</mi><mo>,</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub><mo>)</mo></math></span> and <span><math><msub><mrow><mo>‖</mo><mi>τ</mi><mo>‖</mo></mrow><mrow><mi>L</mi><msup><mrow><mi>ln</mi></mrow><mrow><mi>λ</mi></mrow></msup><mo>⁡</mo><mi>L</mi><mo>(</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub><mo>)</mo></mrow></msub></math></span>. As a direct corollary, we obtain the energy identity and necklessness of a blow-up sequence <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>n</mi></mrow></msub></math></span> with bounded energy <span><math><mi>E</mi><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mi>n</mi></mrow></msub><mo>)</mo></math></span> and bounded <span><math><mi>τ</mi><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mi>n</mi></mrow></msub><mo>)</mo></math></span> in <span><math><mi>L</mi><msup><mrow><mi>ln</mi></mrow><mrow><mi>λ</mi></mrow></msup><mo>⁡</mo><mi>L</mi><mo>(</mo><msub><mrow><mi>D</mi></mrow><mrow><mn>8</mn></mrow></msub><mo>)</mo></math></span>.</div></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110736"},"PeriodicalIF":1.7,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142659887","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
Poisson transform and unipotent complex geometry 泊松变换和单能复几何
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110742
Heiko Gimperlein , Bernhard Krötz , Luz Roncal , Sundaram Thangavelu
<div><div>Our concern is with Riemannian symmetric spaces <span><math><mi>Z</mi><mo>=</mo><mi>G</mi><mo>/</mo><mi>K</mi></math></span> of the non-compact type and more precisely with the Poisson transform <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>λ</mi></mrow></msub></math></span> which maps generalized functions on the boundary ∂<em>Z</em> to <em>λ</em>-eigenfunctions on <em>Z</em>. Special emphasis is given to a maximal unipotent group <span><math><mi>N</mi><mo><</mo><mi>G</mi></math></span> which naturally acts on both <em>Z</em> and ∂<em>Z</em>. The <em>N</em>-orbits on <em>Z</em> are parametrized by a torus <span><math><mi>A</mi><mo>=</mo><msup><mrow><mo>(</mo><msub><mrow><mi>R</mi></mrow><mrow><mo>></mo><mn>0</mn></mrow></msub><mo>)</mo></mrow><mrow><mi>r</mi></mrow></msup><mo><</mo><mi>G</mi></math></span> (Iwasawa) and letting the level <span><math><mi>a</mi><mo>∈</mo><mi>A</mi></math></span> tend to 0 on a ray we retrieve <em>N</em> via <span><math><msub><mrow><mi>lim</mi></mrow><mrow><mi>a</mi><mo>→</mo><mn>0</mn></mrow></msub><mo>⁡</mo><mi>N</mi><mi>a</mi></math></span> as an open dense orbit in ∂<em>Z</em> (Bruhat). For positive parameters <em>λ</em> the Poisson transform <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>λ</mi></mrow></msub></math></span> is defined and injective for functions <span><math><mi>f</mi><mo>∈</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>N</mi><mo>)</mo></math></span> and we give a novel characterization of <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>λ</mi></mrow></msub><mo>(</mo><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>N</mi><mo>)</mo><mo>)</mo></math></span> in terms of complex analysis. For that we view eigenfunctions <span><math><mi>ϕ</mi><mo>=</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>λ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span> as families <span><math><msub><mrow><mo>(</mo><msub><mrow><mi>ϕ</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>)</mo></mrow><mrow><mi>a</mi><mo>∈</mo><mi>A</mi></mrow></msub></math></span> of functions on the <em>N</em>-orbits, i.e. <span><math><msub><mrow><mi>ϕ</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>(</mo><mi>n</mi><mo>)</mo><mo>=</mo><mi>ϕ</mi><mo>(</mo><mi>n</mi><mi>a</mi><mo>)</mo></math></span> for <span><math><mi>n</mi><mo>∈</mo><mi>N</mi></math></span>. The general theory then tells us that there is a tube domain <span><math><mi>T</mi><mo>=</mo><mi>N</mi><mi>exp</mi><mo>⁡</mo><mo>(</mo><mi>i</mi><mi>Λ</mi><mo>)</mo><mo>⊂</mo><msub><mrow><mi>N</mi></mrow><mrow><mi>C</mi></mrow></msub></math></span> such that each <span><math><msub><mrow><mi>ϕ</mi></mrow><mrow><mi>a</mi></mrow></msub></math></span> extends to a holomorphic function on the scaled tube <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>=</mo><mi>N</mi><mi>exp</mi><mo>⁡</mo><mo>(</mo><mi>i</mi><mi>Ad</mi><mo>(</mo><mi>a</mi><mo>)</mo><mi>Λ</mi><mo>)</mo></math></span>. We
我们关注的是非紧凑类型的黎曼对称空间 Z=G/K,更确切地说,是将∂Z 边界上的广义函数映射为 Z 上的λ特征函数的泊松变换 Pλ。我们特别强调了自然作用于 Z 和∂Z 的最大单能群 N<G。Z 上的 N 轨道由一个环 A=(R>0)r<G(岩泽)参数化,让水平 a∈A 在射线上趋向于 0,我们就可以通过 lima→0Na 在 ∂Z 中检索到作为开放密集轨道的 N(布鲁哈特)。对于正参数 λ,函数 f∈L2(N) 的泊松变换 Pλ 是定义的和注入的,我们从复分析的角度给出了 Pλ(L2(N))的新特征。为此,我们将特征函数 ϕ=Pλ(f) 视为 N 轨道上的函数族 (ja)a∈A,即 n∈N 时 ϕa(n)=j(na)。一般理论告诉我们,存在一个管域 T=Nexp(iΛ)⊂NC,使得每个 ϕa 在缩放管 Ta=Nexp(iAd(a)Λ) 上扩展为一个全形函数。我们定义了管子 T 上的一类 N 不变权函数 wλ,对每一个 a∈A 将它们重标度为 Ta 上的权 wλ,a,并证明每个 ja 位于 L2 加权伯格曼空间 B(Ta,wλ,a):=O(Ta)∩L2(Ta,wλ,a)。文章的主要结果将 Pλ(L2(N))描述为ϕa∈B(Ta,wλ,a)和‖ϕ‖:=supa∈AaReλ-2ρ‖ϕa‖Ba,λ<∞成立的特征函数。
{"title":"Poisson transform and unipotent complex geometry","authors":"Heiko Gimperlein ,&nbsp;Bernhard Krötz ,&nbsp;Luz Roncal ,&nbsp;Sundaram Thangavelu","doi":"10.1016/j.jfa.2024.110742","DOIUrl":"10.1016/j.jfa.2024.110742","url":null,"abstract":"&lt;div&gt;&lt;div&gt;Our concern is with Riemannian symmetric spaces &lt;span&gt;&lt;math&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mi&gt;K&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; of the non-compact type and more precisely with the Poisson transform &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; which maps generalized functions on the boundary ∂&lt;em&gt;Z&lt;/em&gt; to &lt;em&gt;λ&lt;/em&gt;-eigenfunctions on &lt;em&gt;Z&lt;/em&gt;. Special emphasis is given to a maximal unipotent group &lt;span&gt;&lt;math&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; which naturally acts on both &lt;em&gt;Z&lt;/em&gt; and ∂&lt;em&gt;Z&lt;/em&gt;. The &lt;em&gt;N&lt;/em&gt;-orbits on &lt;em&gt;Z&lt;/em&gt; are parametrized by a torus &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; (Iwasawa) and letting the level &lt;span&gt;&lt;math&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; tend to 0 on a ray we retrieve &lt;em&gt;N&lt;/em&gt; via &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;lim&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;→&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; as an open dense orbit in ∂&lt;em&gt;Z&lt;/em&gt; (Bruhat). For positive parameters &lt;em&gt;λ&lt;/em&gt; the Poisson transform &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; is defined and injective for functions &lt;span&gt;&lt;math&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; and we give a novel characterization of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; in terms of complex analysis. For that we view eigenfunctions &lt;span&gt;&lt;math&gt;&lt;mi&gt;ϕ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;λ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; as families &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ϕ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; of functions on the &lt;em&gt;N&lt;/em&gt;-orbits, i.e. &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ϕ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;ϕ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; for &lt;span&gt;&lt;math&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;. The general theory then tells us that there is a tube domain &lt;span&gt;&lt;math&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mi&gt;exp&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mi&gt;Λ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; such that each &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ϕ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; extends to a holomorphic function on the scaled tube &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mi&gt;exp&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mi&gt;Ad&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mi&gt;Λ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. We ","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110742"},"PeriodicalIF":1.7,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142659696","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Lp estimates of the maximal Schrödinger operator in Rn Rn 中最大薛定谔算子的 Lp 估计值
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110737
Xiumin Du, Jianhui Li
We obtain Lp estimates of the maximal Schrödinger operator in Rn using polynomial partitioning, bilinear refined Strichartz estimates, and weighted restriction estimates.
我们利用多项式分割、双线性精炼斯特里查兹估计和加权限制估计,得到了 Rn 中最大薛定谔算子的 Lp 估计值。
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引用次数: 0
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Journal of Functional Analysis
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