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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。
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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
A Weyl law for the p-Laplacian p 拉普拉斯的韦尔定律
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-06 DOI: 10.1016/j.jfa.2024.110734
Liam Mazurowski
We show that a Weyl law holds for the variational spectrum of the p-Laplacian. More precisely, let (λi)i=1 be the variational spectrum of Δp on a closed Riemannian manifold (X,g) and let N(λ)=#{i:λi<λ} be the associated counting function. Then we have a Weyl lawN(λ)cvol(X)λn/p. This confirms a conjecture of Friedlander. The proof is based on ideas of Gromov [5] and Liokumovich, Marques, Neves [7].
我们证明,p-拉普拉斯的变谱存在韦尔定律。更确切地说,设 (λi)i=1∞ 为封闭黎曼流形 (X,g) 上 Δp 的变分谱,设 N(λ)=#{i:λi<λ} 为相关的计数函数。那么我们就有一个韦尔定律N(λ)∼cvol(X)λn/p。这证实了弗里德兰德的猜想。证明基于 Gromov [5] 和 Liokumovich, Marques, Neves [7] 的观点。
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引用次数: 0
Lipschitz truncation method for parabolic double-phase systems and applications 抛物线双相系统的 Lipschitz 截断法及其应用
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-05 DOI: 10.1016/j.jfa.2024.110738
Wontae Kim, Juha Kinnunen, Lauri Särkiö
We discuss a Lipschitz truncation technique for parabolic double-phase problems of p-Laplace type in order to prove energy estimates and uniqueness results for the Dirichlet problem. Moreover, we show existence for a non-homogeneous double-phase problem. The Lipschitz truncation method is based on a Whitney-type covering result and a related partition of unity in the intrinsic geometry for the double-phase problem.
我们讨论了 p-Laplace 型抛物线双相问题的 Lipschitz 截断技术,以证明 Dirichlet 问题的能量估计和唯一性结果。此外,我们还证明了非均质双相问题的存在性。Lipschitz截断方法基于惠特尼型覆盖结果和双相问题内在几何中的相关统一分割。
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引用次数: 0
Simplicity of crossed products of the actions of totally disconnected locally compact groups on their boundaries 完全互不相连的局部紧凑群在其边界上的作用的交叉积的简单性
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-11-05 DOI: 10.1016/j.jfa.2024.110732
Ryoya Arimoto
We prove that if a totally disconnected locally compact group admits a topologically free boundary, then the reduced crossed product of continuous functions on its Furstenberg boundary by the group is simple. We also prove a partial converse of this result.
我们证明,如果一个完全断开的局部紧凑群具有拓扑自由边界,那么该群在其弗斯滕伯格边界上的连续函数的还原交叉积是简单的。我们还证明了这一结果的部分反证。
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引用次数: 0
Corrigendum to “Mourre theory for analytically fibered operators” [J. Funct. Anal. 152 (1) (1998) 202–219] 对 "分析纤维化算子的穆尔勒理论 "的更正 [J. Funct. Anal. 152 (1) (1998) 202-219]
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-10-30 DOI: 10.1016/j.jfa.2024.110697
F. Nier , C. Gérard
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引用次数: 0
On the Hankel transform of Bessel functions on complex numbers and explicit spectral formulae over the Gaussian field 关于复数上贝塞尔函数的汉克尔变换和高斯域上的明确谱公式
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-10-28 DOI: 10.1016/j.jfa.2024.110723
Zhi Qi
In this paper, on the complex field C, we prove two integral formulae for the Hankel–Mellin transform and the double Fourier–Mellin transform of Bessel functions, both resulting the hypergeometric function. As two applications, we use the former integral formula to make explicit the spectral formula of Bruggeman and Motohashi for the fourth moment of Dedekind zeta function over the Gaussian number field Q(i) and to establish a spectral formula for the Hecke-eigenvalue twisted second moment of central L-values for the Picard group PGL2(Z[i]). Moreover, we develop the theory of distributional Hankel transform on C{0}.
本文在复数场 C 上证明了贝塞尔函数的汉克尔-梅林变换和双傅里叶-梅林变换的两个积分公式,这两个积分公式都产生了超几何函数。作为两个应用,我们利用前一个积分公式明确了布鲁格曼和本桥对高斯数域 Q(i) 的 Dedekind zeta 函数第四矩的谱公式,并建立了皮卡组 PGL2(Z[i]) 的赫克特征值扭转中心 L 值第二矩的谱公式。此外,我们还发展了 C∖{0} 上的分布汉克尔变换理论。
{"title":"On the Hankel transform of Bessel functions on complex numbers and explicit spectral formulae over the Gaussian field","authors":"Zhi Qi","doi":"10.1016/j.jfa.2024.110723","DOIUrl":"10.1016/j.jfa.2024.110723","url":null,"abstract":"<div><div>In this paper, on the complex field <span><math><mi>C</mi></math></span>, we prove two integral formulae for the Hankel–Mellin transform and the double Fourier–Mellin transform of Bessel functions, both resulting the hypergeometric function. As two applications, we use the former integral formula to make explicit the spectral formula of Bruggeman and Motohashi for the fourth moment of Dedekind zeta function over the Gaussian number field <span><math><mi>Q</mi><mo>(</mo><mi>i</mi><mo>)</mo></math></span> and to establish a spectral formula for the Hecke-eigenvalue twisted second moment of central <em>L</em>-values for the Picard group <span><math><msub><mrow><mi>PGL</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>Z</mi><mo>[</mo><mi>i</mi><mo>]</mo><mo>)</mo></math></span>. Moreover, we develop the theory of distributional Hankel transform on <span><math><mi>C</mi><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo></math></span>.</div></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110723"},"PeriodicalIF":1.7,"publicationDate":"2024-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142578184","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
Weighted Dirichlet spaces that are de Branges-Rovnyak spaces with equivalent norms 具有等效规范的 de Branges-Rovnyak 空间的加权 Dirichlet 空间
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-10-24 DOI: 10.1016/j.jfa.2024.110717
Stamatis Pouliasis
For a positive Borel measure μ in the unit disc, we examine which weighted Dirichlet spaces Dμ can be identified with de Branges-Rovnyak spaces Hb, with equivalent norms. We prove a necessary condition for the equality Dμ=Hb and we explore its consequences. For Carleson measures μ, we give a necessary and sufficient condition for the equality Dμ=Hbμ, for a certain outer function bμ related with the balayage of μ on the unit circle, and we provide examples of those spaces.
对于单位圆盘中的正伯勒量μ,我们研究了哪些加权德里赫特空间 Dμ 可以与具有等效规范的 de Branges-Rovnyak 空间 Hb 标识。我们证明了 Dμ=Hb 相等的必要条件,并探讨了其后果。对于卡莱森量μ,我们给出了Dμ=Hbμ相等的必要条件和充分条件,条件是与单位圆上μ的巴拉维相关的某个外函数bμ,我们还提供了这些空间的例子。
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引用次数: 0
On boundedness of isomerization paths for non- and semirelativistic molecules 论非相对论分子和半相对论分子异构化路径的有界性
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-10-24 DOI: 10.1016/j.jfa.2024.110713
Ioannis Anapolitanos , Marco Olivieri , Sylvain Zalczer
This article focuses on isomerizations of molecules, i.e. chemical reactions during which a molecule is transformed into another one with atoms in a different spatial configuration. We consider the special case in which the system breaks into two submolecules whose internal geometry is solid during the whole procedure. We prove, under some conditions, that the distance between the two submolecules stays bounded during the reaction. This paper extends [Anapolitanos-Lewin, 2020] in two directions. The first one is that we relax assumptions that the ground state eigenspaces of the submolecules have to fulfill. The second one is that we allow semirelativistic kinetic energy as well. We provide an asymptotic expansion of the interaction energy between two molecules, including multipolar interactions and the van der Waals attraction. In addition to this static result, we proceed to a quasistatic analysis to investigate the variation of the energy when the nuclei move.
本文的重点是分子的异构化,即在化学反应过程中,一个分子转变为另一个具有不同空间构型原子的分子。我们考虑了一种特殊情况,即在整个反应过程中,体系分裂成两个内部几何形状为固态的子分子。我们证明,在某些条件下,两个子分子之间的距离在反应过程中保持有界。本文在两个方向上扩展了[Anapolitanos-Lewin, 2020]。首先,我们放宽了亚分子基态特征空间必须满足的假设条件。第二,我们也允许半惯性动能。我们提供了两个分子之间相互作用能量的渐近展开,包括多极相互作用和范德华吸引力。除了这一静态结果,我们还进行了准静态分析,以研究原子核移动时的能量变化。
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引用次数: 0
Operator ℓp → ℓq norms of random matrices with iid entries 具有 iid 条目的随机矩阵的运算符 ℓp → ℓq 准则
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-10-24 DOI: 10.1016/j.jfa.2024.110720
Rafał Latała, Marta Strzelecka
<div><div>We prove that for every <span><math><mi>p</mi><mo>,</mo><mi>q</mi><mo>∈</mo><mo>[</mo><mn>1</mn><mo>,</mo><mo>∞</mo><mo>]</mo></math></span> and every random matrix <span><math><mi>X</mi><mo>=</mo><msub><mrow><mo>(</mo><msub><mrow><mi>X</mi></mrow><mrow><mi>i</mi><mo>,</mo><mi>j</mi></mrow></msub><mo>)</mo></mrow><mrow><mi>i</mi><mo>≤</mo><mi>m</mi><mo>,</mo><mi>j</mi><mo>≤</mo><mi>n</mi></mrow></msub></math></span> with iid centered entries satisfying the <em>α</em>-regularity assumption <span><math><msub><mrow><mo>‖</mo><msub><mrow><mi>X</mi></mrow><mrow><mi>i</mi><mo>,</mo><mi>j</mi></mrow></msub><mo>‖</mo></mrow><mrow><mn>2</mn><mi>ρ</mi></mrow></msub><mo>≤</mo><mi>α</mi><msub><mrow><mo>‖</mo><msub><mrow><mi>X</mi></mrow><mrow><mi>i</mi><mo>,</mo><mi>j</mi></mrow></msub><mo>‖</mo></mrow><mrow><mi>ρ</mi></mrow></msub></math></span> for every <span><math><mi>ρ</mi><mo>≥</mo><mn>1</mn></math></span>, the expectation of the operator norm of <em>X</em> from <span><math><msubsup><mrow><mi>ℓ</mi></mrow><mrow><mi>p</mi></mrow><mrow><mi>n</mi></mrow></msubsup></math></span> to <span><math><msubsup><mrow><mi>ℓ</mi></mrow><mrow><mi>q</mi></mrow><mrow><mi>m</mi></mrow></msubsup></math></span> is comparable, up to a constant depending only on <em>α</em>, to<span><span><span><math><msup><mrow><mi>m</mi></mrow><mrow><mn>1</mn><mo>/</mo><mi>q</mi></mrow></msup><munder><mi>sup</mi><mrow><mi>t</mi><mo>∈</mo><msubsup><mrow><mi>B</mi></mrow><mrow><mi>p</mi></mrow><mrow><mi>n</mi></mrow></msubsup></mrow></munder><mo>⁡</mo><msub><mrow><mo>‖</mo><munderover><mo>∑</mo><mrow><mi>j</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>n</mi></mrow></munderover><msub><mrow><mi>t</mi></mrow><mrow><mi>j</mi></mrow></msub><msub><mrow><mi>X</mi></mrow><mrow><mn>1</mn><mo>,</mo><mi>j</mi></mrow></msub><mo>‖</mo></mrow><mrow><mi>q</mi><mo>∧</mo><mi>Log</mi><mspace></mspace><mi>m</mi></mrow></msub><mo>+</mo><msup><mrow><mi>n</mi></mrow><mrow><mn>1</mn><mo>/</mo><msup><mrow><mi>p</mi></mrow><mrow><mo>⁎</mo></mrow></msup></mrow></msup><munder><mi>sup</mi><mrow><mi>s</mi><mo>∈</mo><msubsup><mrow><mi>B</mi></mrow><mrow><msup><mrow><mi>q</mi></mrow><mrow><mo>⁎</mo></mrow></msup></mrow><mrow><mi>m</mi></mrow></msubsup></mrow></munder><mo>⁡</mo><msub><mrow><mo>‖</mo><munderover><mo>∑</mo><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>m</mi></mrow></munderover><msub><mrow><mi>s</mi></mrow><mrow><mi>i</mi></mrow></msub><msub><mrow><mi>X</mi></mrow><mrow><mi>i</mi><mo>,</mo><mn>1</mn></mrow></msub><mo>‖</mo></mrow><mrow><msup><mrow><mi>p</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>∧</mo><mi>Log</mi><mspace></mspace><mi>n</mi></mrow></msub><mo>.</mo></math></span></span></span> We give more explicit formulas, expressed as exact functions of <em>p</em>, <em>q</em>, <em>m</em>, and <em>n</em>, for the two-sided bounds of the operator norms in the case when the entries <span><math><msub><mrow><mi>X</mi></mrow><mrow><mi>i</mi><mo>,</mo><mi>j</mi></mrow></msub></math></span> are: Gaussia
我们证明,对于每个 p,q∈[1,∞]和每个随机矩阵 X=(Xi,j)i≤m,j≤n,其 iid 居中条目满足α正则假设‖Xi,j‖2ρ≤α‖Xi,j‖ρ,对于每个 ρ≥1、从 ℓpn 到 ℓqm 的 X 的算子规范的期望是可比的,直到一个只取决于 α 的常数,tom1/qsupt∈Bpn‖∑j=1ntjX1,j‖q∧Logm+n1/p⁎sups∈Bq⁎m‖∑i=1msiXi,1‖p⁎∧Logn。我们给出了更明确的公式,用 p、q、m 和 n 的精确函数表示了当条目 Xi,j 为以下情况时算子规范的双侧边界:高斯、魏布里安、对数凹尾和对数凸尾。在 1≤q≤2≤p 的范围内,我们提供了较弱正则假设 (EX1,14)1/4≤α(EX1,12)1/2 下的双侧边界。
{"title":"Operator ℓp → ℓq norms of random matrices with iid entries","authors":"Rafał Latała,&nbsp;Marta Strzelecka","doi":"10.1016/j.jfa.2024.110720","DOIUrl":"10.1016/j.jfa.2024.110720","url":null,"abstract":"&lt;div&gt;&lt;div&gt;We prove that for every &lt;span&gt;&lt;math&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;q&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 every random matrix &lt;span&gt;&lt;math&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; with iid centered entries satisfying the &lt;em&gt;α&lt;/em&gt;-regularity assumption &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;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; for every &lt;span&gt;&lt;math&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, the expectation of the operator norm of &lt;em&gt;X&lt;/em&gt; from &lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt; to &lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt; is comparable, up to a constant depending only on &lt;em&gt;α&lt;/em&gt;, to&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;munder&gt;&lt;mi&gt;sup&lt;/mi&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/mrow&gt;&lt;/munder&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;munderover&gt;&lt;mo&gt;∑&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/munderover&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&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;mi&gt;Log&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;munder&gt;&lt;mi&gt;sup&lt;/mi&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;q&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/mrow&gt;&lt;/munder&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;munderover&gt;&lt;mo&gt;∑&lt;/mo&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/munderover&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;‖&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;p&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;Log&lt;/mi&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; We give more explicit formulas, expressed as exact functions of &lt;em&gt;p&lt;/em&gt;, &lt;em&gt;q&lt;/em&gt;, &lt;em&gt;m&lt;/em&gt;, and &lt;em&gt;n&lt;/em&gt;, for the two-sided bounds of the operator norms in the case when the entries &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;X&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;j&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; are: Gaussia","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"288 3","pages":"Article 110720"},"PeriodicalIF":1.7,"publicationDate":"2024-10-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142578185","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}
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Journal of Functional Analysis
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