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Generalized orthogonal measures on the space of unital completely positive maps 单位完全正映射空间上的广义正交测量
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0330
Angshuman Bhattacharya, Chaitanya J. Kulkarni
A classical result by Effros connects the barycentric decomposition of a state on a C*-algebra to the disintegration theory of the GNS representation of the state with respect to an orthogonal measure on the state space of the C*-algebra. In this note, we take this approach to the space of unital completely positive maps on a C*-algebra with values in B ( H ) {B(H)} , connecting the barycentric decomposition of the unital completely positive map and the disintegration theory of the minimal Stinespring dilation of the same. This generalizes Effros’ work in the non-commutative setting. We do this by introducing a special class of barycentric measures which we call generalized orthogonal measures. We end this note by mentioning some examples of generalized orthogonal measures.
埃夫罗斯(Effros)的一个经典结果将 C* 代数上的状态的重心分解与状态的 GNS 表示的解体理论联系起来,而 GNS 表示是关于 C* 代数的状态空间上的正交度量的。在本注释中,我们将这一方法应用于 C* 代数上在 B ( H ) {B(H)}中取值的单元全正映射空间,将单元全正映射的重心分解与同一映射的最小施蒂尼斯普林扩张的解体理论联系起来。这概括了埃弗罗斯在非交换背景下的工作。为此,我们引入了一类特殊的重心度量,我们称之为广义正交度量。最后,我们举几个广义正交度量的例子来结束本说明。
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引用次数: 0
Octonionic monogenic and slice monogenic Hardy and Bergman spaces 八元单源和切片单源哈代和伯格曼空间
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0039
Fabrizio Colombo, Rolf Sören Kraußhar, Irene Sabadini
In this paper we discuss some basic properties of octonionic Bergman and Hardy spaces. In the first part we review some fundamental concepts of the general theory of octonionic Hardy and Bergman spaces together with related reproducing kernel functions in the monogenic setting. We explain how some of the fundamental problems in well-defining a reproducing kernel can be overcome in the non-associative setting by looking at the real part of an appropriately defined para-linear octonion-valued inner product. The presence of a weight factor of norm 1 in the definition of the inner product is an intrinsic new ingredient in the octonionic setting. Then we look at the slice monogenic octonionic setting using the classical complex book structure. We present explicit formulas for the slice monogenic reproducing kernels for the unit ball, the right octonionic half-space and strip domains bounded in the real direction. In the setting of the unit ball we present an explicit sequential characterization which can be obtained by applying the special Taylor series representation of the slice monogenic setting together with particular octonionic calculation rules that reflect the property of octonionic para-linearity.
在本文中,我们将讨论八离子伯格曼和哈代空间的一些基本性质。在第一部分中,我们回顾了八离子哈代和伯格曼空间一般理论的一些基本概念,以及单元环境中的相关重现核函数。我们解释了如何通过研究适当定义的准线性八离子值内积的实部,来克服在非联立环境中妥善定义重现核的一些基本问题。内积定义中存在规范为 1 的权重因子是八离子环境中一个固有的新要素。然后,我们使用经典的复书结构来研究切片单原八离子环境。我们给出了单位球、右八离子半空间和实方向有界条域的切片单原重现核的明确公式。在单位球设置中,我们提出了一个明确的序列特征,通过应用切片单原设置的特殊泰勒级数表示,以及反映八离子副线性性质的特殊八离子计算规则,可以获得该特征。
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引用次数: 0
The quotient set of the quadratic distance set over finite fields 有限域上二次距离集的商集
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0313
Alex Iosevich, Doowon Koh, Firdavs Rakhmonov
Let <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msubsup> <m:mi>𝔽</m:mi> <m:mi>q</m:mi> <m:mi>d</m:mi> </m:msubsup> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0296.png" /> <jats:tex-math>{mathbb{F}_{q}^{d}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> be the <jats:italic>d</jats:italic>-dimensional vector space over the finite field <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mi>𝔽</m:mi> <m:mi>q</m:mi> </m:msub> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0298.png" /> <jats:tex-math>{mathbb{F}_{q}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> with <jats:italic>q</jats:italic> elements. For each non-zero <jats:italic>r</jats:italic> in <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:msub> <m:mi>𝔽</m:mi> <m:mi>q</m:mi> </m:msub> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0298.png" /> <jats:tex-math>{mathbb{F}_{q}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> and <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mi>E</m:mi> <m:mo>⊂</m:mo> <m:msubsup> <m:mi>𝔽</m:mi> <m:mi>q</m:mi> <m:mi>d</m:mi> </m:msubsup> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0186.png" /> <jats:tex-math>{Esubsetmathbb{F}_{q}^{d}}</jats:tex-math> </jats:alternatives> </jats:inline-formula>, we define <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mi>W</m:mi> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>r</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0235.png" /> <jats:tex-math>{W(r)}</jats:tex-math> </jats:alternatives> </jats:inline-formula> as the number of quadruples <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>x</m:mi> <m:mo>,</m:mo> <m:mi>y</m:mi> <m:mo>,</m:mo> <m:mi>z</m:mi> <m:mo>,</m:mo> <m:mi>w</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> <m:mo>∈</m:mo> <m:msup> <m:mi>E</m:mi> <m:mn>4</m:mn> </m:msup> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0313_eq_0153.png" /> <jats:tex-math>{(x,y,z,w)in E^{4}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> such that <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mfrac> <m:mrow> <m:mi>Q</m:mi> <m:mo>⁢</m:mo> <m:
设 𝔽 q d {mathbb{F}_{q}^{d}} 是有限域 𝔽 q {mathbb{F}_{q}} 上有 q 个元素的 d 维向量空间。对于𝔽 q {mathbb{F}_{q}} 中的每一个非零 r 和 E ⊂ 𝔽 q d {Esubsetmathbb{F}_{q}^{d}} ,我们定义 W ( r ) {mathbb{F}_{q}^{d} 为有限域上、有 q 个元素的 d 维向量空间。 我们定义 W ( r ) {W(r)} 为∈ E 4 {(x,y,z,w)in E^{4}} 中 Q ( x - y ) Q ( z - w ) = r {frac{Q(x-y)}{Q(z-w)}=r} 的四元数 ( x , y , z , w ) ,其中 Q 是 𝔽 q {mathbb{F}_{q}} 上 d 个变量的非退化二次型。 .当 Q ( α ) = ∑ i = 1 d α i 2 {Q(alpha)=sum_{i=1}^{d}alpha_{i}^{2}} 时,α = ( α 1 , ... , α d ) ∈ α 。, α d ) ∈ 𝔽 q d {alpha=(alpha_{1},ldots,alpha_{d})inmathbb{F}_{q}^{d}} Pham (2022) 最近使用群作用机制证明,如果 E ⊂ 𝔽 q 2 {Esubsetmathbb{F}_{q}^{2}} with q ≡ 3 ( mod 4 ) {qequiv 3~{}(operatorname{mod},4)} and | E |≥ C q {|E|geq Cq} ,那么有 W ( r ) 。 对于任意非零平方数 r∈ 𝔽 q {rinmathbb{F}_{q}} ,其中 C 是一个足够大的平方数。 其中 C 是一个足够大的常数,c 是介于 0 和 1 之间的某个数,而 | E | {|E|} 表示集合 E 的万有引力。在本文中,我们将 Pham 在二维中的结果改进并扩展到具有一般非退化二次距离的任意维度。作为我们结果的一个推论,我们还概括了前两位作者和 Parshall (2019) 关于距离集的商集的 Falconer 型问题的尖锐结果。此外,我们还提供了基础集合大小条件的改进常数。新的关键要素是将 W ( r ) {W(r)} 的估计值与 2 d {2d} 维向量空间中的二次同素异形体联系起来。这种方法富有成果,因为它允许我们利用高斯和,而高斯和比标准距离类型问题中出现的克洛斯特曼和更容易处理。
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引用次数: 0
A fixed point theorem for isometries on a metric space 度量空间上等距物的定点定理
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0193
Andrzej Wiśnicki
We show that if <jats:italic>X</jats:italic> is a complete metric space with uniform relative normal structure and <jats:italic>G</jats:italic> is a subgroup of the isometry group of <jats:italic>X</jats:italic> with bounded orbits, then there is a point in <jats:italic>X</jats:italic> fixed by every isometry in <jats:italic>G</jats:italic>. As a corollary, we obtain a theorem of U. Lang (2013) concerning injective metric spaces. A few applications of this theorem are given to the problems of inner derivations. In particular, we show that if <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:msub> <m:mi>L</m:mi> <m:mn>1</m:mn> </m:msub> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>μ</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0193_eq_0087.png" /> <jats:tex-math>{L_{1}(mu)}</jats:tex-math> </jats:alternatives> </jats:inline-formula> is an essential Banach <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:msub> <m:mi>L</m:mi> <m:mn>1</m:mn> </m:msub> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>G</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0193_eq_0086.png" /> <jats:tex-math>{L_{1}(G)}</jats:tex-math> </jats:alternatives> </jats:inline-formula>-bimodule, then any continuous derivation <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mi>δ</m:mi> <m:mo>:</m:mo> <m:mrow> <m:mrow> <m:msub> <m:mi>L</m:mi> <m:mn>1</m:mn> </m:msub> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>G</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> <m:mo>→</m:mo> <m:mrow> <m:msub> <m:mi>L</m:mi> <m:mi mathvariant="normal">∞</m:mi> </m:msub> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>μ</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0193_eq_0136.png" /> <jats:tex-math>{delta:L_{1}(G)rightarrow L_{infty}(mu)}</jats:tex-math> </jats:alternatives> </jats:inline-formula> is inner. This extends a theorem of B. E. Johnson (1991) asserting that the convolution algebra <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:msub> <m:mi>L</m:mi> <m:mn>1</m:mn> </m:msub> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>G</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0193_eq_0086.png" /> <jats:tex-math>{L_{1}(G)}</jats:tex-math> </jats:alternatives> </jats:inline-formula> is weakly am
我们证明,如果 X 是具有均匀相对法向结构的完全度量空间,而 G 是 X 的有界轨道等值群的一个子群,那么 X 中存在一个被 G 中的每个等值固定的点。这个定理在内层衍生问题上有一些应用。特别是,我们证明了如果 L 1 ( μ ) {L_{1}(mu)} 是一个本质的巴纳赫 L 1 ( G ) {L_{1}(G)} - 二模子,那么任何连续求导 δ : L 1 ( G ) → L ∞ ( μ ) {delta:L_{1}(G)rightarrow L_{infty}(mu)} 都是内求导。这扩展了 B. E. Johnson (1991) 的一个定理,即如果 G 是局部紧凑群,卷积代数 L 1 ( G ) {L_{1}(G)} 是弱可变的。
{"title":"A fixed point theorem for isometries on a metric space","authors":"Andrzej Wiśnicki","doi":"10.1515/forum-2023-0193","DOIUrl":"https://doi.org/10.1515/forum-2023-0193","url":null,"abstract":"We show that if &lt;jats:italic&gt;X&lt;/jats:italic&gt; is a complete metric space with uniform relative normal structure and &lt;jats:italic&gt;G&lt;/jats:italic&gt; is a subgroup of the isometry group of &lt;jats:italic&gt;X&lt;/jats:italic&gt; with bounded orbits, then there is a point in &lt;jats:italic&gt;X&lt;/jats:italic&gt; fixed by every isometry in &lt;jats:italic&gt;G&lt;/jats:italic&gt;. As a corollary, we obtain a theorem of U. Lang (2013) concerning injective metric spaces. A few applications of this theorem are given to the problems of inner derivations. In particular, we show that if &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mi&gt;L&lt;/m:mi&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:msub&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;μ&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0193_eq_0087.png\" /&gt; &lt;jats:tex-math&gt;{L_{1}(mu)}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; is an essential Banach &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mi&gt;L&lt;/m:mi&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:msub&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;G&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0193_eq_0086.png\" /&gt; &lt;jats:tex-math&gt;{L_{1}(G)}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;-bimodule, then any continuous derivation &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:mi&gt;δ&lt;/m:mi&gt; &lt;m:mo&gt;:&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mi&gt;L&lt;/m:mi&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:msub&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;G&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;m:mo&gt;→&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mi&gt;L&lt;/m:mi&gt; &lt;m:mi mathvariant=\"normal\"&gt;∞&lt;/m:mi&gt; &lt;/m:msub&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;μ&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0193_eq_0136.png\" /&gt; &lt;jats:tex-math&gt;{delta:L_{1}(G)rightarrow L_{infty}(mu)}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; is inner. This extends a theorem of B. E. Johnson (1991) asserting that the convolution algebra &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:msub&gt; &lt;m:mi&gt;L&lt;/m:mi&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:msub&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;G&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0193_eq_0086.png\" /&gt; &lt;jats:tex-math&gt;{L_{1}(G)}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; is weakly am","PeriodicalId":12433,"journal":{"name":"Forum Mathematicum","volume":"8 1","pages":""},"PeriodicalIF":0.8,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139078683","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Finite rigid sets of the non-separating curve complex 非分离曲线复合体的有限刚性集
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0024
Rodrigo De Pool
We prove that the non-separating curve complex of every surface of finite type and genus at least three admits an exhaustion by finite rigid sets.
我们证明,每一个有限类型、至少三属的曲面的非分离曲线复曲面都可以通过有限刚集穷尽。
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引用次数: 0
One-sided Gorenstein rings 单面戈伦斯坦环
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0303
Lars Winther Christensen, Sergio Estrada, Li Liang, Peder Thompson, Junpeng Wang
Distinctive characteristics of Iwanaga–Gorenstein rings are typically understood through their intrinsic symmetry. We show that several of those that pertain to the Gorenstein global dimensions carry over to the one-sided situation, even without the noetherian hypothesis. Our results yield new relations among homological invariants related to the Gorenstein property, not only Gorenstein global dimensions but also the suprema of projective/injective dimensions of injective/projective modules and finitistic dimensions.
岩永-戈伦斯坦环的显著特征通常通过其内在对称性来理解。我们的研究表明,其中一些与戈伦斯坦全维相关的特征可以延续到单侧情况,即使没有诺特假说也是如此。我们的结果产生了与戈伦斯坦性质相关的同调不变式之间的新关系,不仅包括戈伦斯坦全维,还包括注入/射出模块的射出/注入维的上界和有限维。
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引用次数: 0
Archimedean toroidal maps and their edge covers 阿基米德环状映射及其边盖
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2024-01-01 DOI: 10.1515/forum-2023-0168
Arnab Kundu, Dipendu Maity
The automorphism group of a map on a surface acts naturally on its flags (triples of incident vertices, edges, and faces). We will study the action of the automorphism group of a map on its edges. A map is semi-equivelar if all of its vertices have the same type of face-cycles. A semi-equivelar toroidal map refers to a semi-equivelar map embedded on a torus. If a map has k edge orbits under its automorphism group, it is referred to as a k-edge orbital or k-orbital. Specifically, it is referred to as an edge-transitive map if k = 1 {k=1} . If any two edges have the same edge-symbol, a map is said to be edge-homogeneous. Every edge-homogeneous toroidal map has an edge-transitive cover, as proved in [A. Orbanić, D. Pellicer, T. Pisanski and T. W. Tucker, Edge-transitive maps of low genus, Ars Math. Contemp. 4 2011, 2, 385–402]. In this article, we show the existence and give a classification of k-edge covers of semi-equivelar toroidal maps.
曲面上的映射的自形群自然地作用于它的旗(入射顶点、边和面的三元组)。我们将研究映射的自形群对其边的作用。如果一个映射的所有顶点都有相同类型的面循环,那么这个映射就是半等式映射。半等边环面映射指的是嵌入在环面上的半等边映射。如果一个映射在其自动形群下有 k 个边轨道,则称为 k 边轨道或 k 轨道。具体来说,如果 k = 1 {k=1} ,则称为边跨映射。如果任意两条边的边符号相同,则称为边同构映射。Orbanić, D. Pellicer, T. Pisanski and T. W. Tucker, Edge-transitive maps of low genus, Ars Math.Contemp.4 2011, 2, 385-402].在本文中,我们证明了半等价环面映射的 k 边盖的存在并给出了其分类。
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引用次数: 0
Improved spectral cluster bounds for orthonormal systems 正交系统的改进谱群边界
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2023-12-14 DOI: 10.1515/forum-2023-0254
Tianyi Ren, An Zhang
We improve the work [R. L. Frank and J. Sabin, Spectral cluster bounds for orthonormal systems and oscillatory integral operators in Schatten spaces, Adv. Math. 317 2017, 157–192] concerning the spectral cluster bounds for orthonormal systems at <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mi>p</m:mi> <m:mo>=</m:mo> <m:mi mathvariant="normal">∞</m:mi> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0254_eq_0261.png" /> <jats:tex-math>{p=infty}</jats:tex-math> </jats:alternatives> </jats:inline-formula>, on the flat torus and spaces of nonpositive sectional curvature, by shrinking the spectral band from <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mo stretchy="false">[</m:mo> <m:msup> <m:mi>λ</m:mi> <m:mn>2</m:mn> </m:msup> <m:mo>,</m:mo> <m:msup> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mrow> <m:mi>λ</m:mi> <m:mo>+</m:mo> <m:mn>1</m:mn> </m:mrow> <m:mo stretchy="false">)</m:mo> </m:mrow> <m:mn>2</m:mn> </m:msup> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0254_eq_0140.png" /> <jats:tex-math>{[lambda^{2},(lambda+1)^{2})}</jats:tex-math> </jats:alternatives> </jats:inline-formula> to <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mo stretchy="false">[</m:mo> <m:msup> <m:mi>λ</m:mi> <m:mn>2</m:mn> </m:msup> <m:mo>,</m:mo> <m:msup> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mrow> <m:mi>λ</m:mi> <m:mo>+</m:mo> <m:mrow> <m:mi>ϵ</m:mi> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>λ</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:mrow> <m:mo stretchy="false">)</m:mo> </m:mrow> <m:mn>2</m:mn> </m:msup> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0254_eq_0142.png" /> <jats:tex-math>{[lambda^{2},(lambda+epsilon(lambda))^{2})}</jats:tex-math> </jats:alternatives> </jats:inline-formula>, where <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mi>ϵ</m:mi> <m:mo>⁢</m:mo> <m:mrow> <m:mo stretchy="false">(</m:mo> <m:mi>λ</m:mi> <m:mo stretchy="false">)</m:mo> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0254_eq_0166.png" /> <jats:tex-math>{epsilon(lambda)}</jats:tex-math> </jats:alternatives> </jats:inline-formula> is a function of λ that goes to 0 as λ goes to <jats:inline-formula> <jats:alternatives> <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mi mathvariant="normal">∞</m:mi> </m:math> <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_forum-2023-0254_eq_0184.png" /> <jats:tex-math>{i
我们改进了 [R. L. Frank 和 J. Sabin, Schatten 空间中正态系统和振荡积分算子的谱群边界, Adv.L. Frank and J. Sabin, Spectral cluster bounds for orthonormal systems and oscillatory integral operators in Schatten spaces, Adv. Math.317 2017, 157-192] concerning the spectral cluster bounds for orthonormal systems at p = ∞ {p=infty} , on the flat torus and spaces of non-finfty}. 通过将谱带从[ λ 2 , ( λ + 1 ) 2 ) 缩小,在平环面和非正断面曲率空间上,正交系统的谱簇边界 {[lambda^{2},(lambda+1)^{2})}缩小到[λ 2 , ( λ + ϵ ( λ ) 2 ) {[lambda^{2},(lambda+epsilon(lambda))^{2})} 其中 ϵ ( λ ) {epsilon(lambda)} 是 λ 的函数,当 λ 变为 ∞ {infty} 时,该函数变为 0。为了实现这一目标,我们引用了 [J. Bourgain, P. Shao] 中开发的方法。Bourgain, P. Shao, C. D. Sogge and X. Yao, On L p L^{p} -resolvent estimates and the density density} 中开发的方法。 -紧凑黎曼流形的残余估计和特征值密度,Comm.Math.333 2015, 3, 1483-1527].
{"title":"Improved spectral cluster bounds for orthonormal systems","authors":"Tianyi Ren, An Zhang","doi":"10.1515/forum-2023-0254","DOIUrl":"https://doi.org/10.1515/forum-2023-0254","url":null,"abstract":"We improve the work [R. L. Frank and J. Sabin, Spectral cluster bounds for orthonormal systems and oscillatory integral operators in Schatten spaces, Adv. Math. 317 2017, 157–192] concerning the spectral cluster bounds for orthonormal systems at &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:mi&gt;p&lt;/m:mi&gt; &lt;m:mo&gt;=&lt;/m:mo&gt; &lt;m:mi mathvariant=\"normal\"&gt;∞&lt;/m:mi&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0254_eq_0261.png\" /&gt; &lt;jats:tex-math&gt;{p=infty}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;, on the flat torus and spaces of nonpositive sectional curvature, by shrinking the spectral band from &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;[&lt;/m:mo&gt; &lt;m:msup&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mn&gt;2&lt;/m:mn&gt; &lt;/m:msup&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:msup&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mo&gt;+&lt;/m:mo&gt; &lt;m:mn&gt;1&lt;/m:mn&gt; &lt;/m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mn&gt;2&lt;/m:mn&gt; &lt;/m:msup&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0254_eq_0140.png\" /&gt; &lt;jats:tex-math&gt;{[lambda^{2},(lambda+1)^{2})}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; to &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;[&lt;/m:mo&gt; &lt;m:msup&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mn&gt;2&lt;/m:mn&gt; &lt;/m:msup&gt; &lt;m:mo&gt;,&lt;/m:mo&gt; &lt;m:msup&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mo&gt;+&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mi&gt;ϵ&lt;/m:mi&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;m:mn&gt;2&lt;/m:mn&gt; &lt;/m:msup&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0254_eq_0142.png\" /&gt; &lt;jats:tex-math&gt;{[lambda^{2},(lambda+epsilon(lambda))^{2})}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt;, where &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mrow&gt; &lt;m:mi&gt;ϵ&lt;/m:mi&gt; &lt;m:mo&gt;⁢&lt;/m:mo&gt; &lt;m:mrow&gt; &lt;m:mo stretchy=\"false\"&gt;(&lt;/m:mo&gt; &lt;m:mi&gt;λ&lt;/m:mi&gt; &lt;m:mo stretchy=\"false\"&gt;)&lt;/m:mo&gt; &lt;/m:mrow&gt; &lt;/m:mrow&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0254_eq_0166.png\" /&gt; &lt;jats:tex-math&gt;{epsilon(lambda)}&lt;/jats:tex-math&gt; &lt;/jats:alternatives&gt; &lt;/jats:inline-formula&gt; is a function of λ that goes to 0 as λ goes to &lt;jats:inline-formula&gt; &lt;jats:alternatives&gt; &lt;m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"&gt; &lt;m:mi mathvariant=\"normal\"&gt;∞&lt;/m:mi&gt; &lt;/m:math&gt; &lt;jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_forum-2023-0254_eq_0184.png\" /&gt; &lt;jats:tex-math&gt;{i","PeriodicalId":12433,"journal":{"name":"Forum Mathematicum","volume":"258 1","pages":""},"PeriodicalIF":0.8,"publicationDate":"2023-12-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138692558","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Some Betti numbers of the moduli of 1-dimensional sheaves on ℙ2 讨论了一维轴在a2上模的若干Betti数
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2023-11-29 DOI: 10.1515/forum-2023-0111
Yao Yuan
Abstract Let M ⁢ ( d , χ ) {M(d,chi)} , with ( d , χ ) = 1 {(d,chi)=1} , be the moduli space of semistable sheaves on ℙ 2 {mathbb{P}^{2}} supported on curves of degree d and with Euler characteristic χ. The cohomology ring H * ⁢ ( M ⁢ ( d , χ ) , ℤ ) {H^{*}(M(d,chi),mathbb{Z})} of M ⁢ ( d , χ ) {M(d,chi)} is isomorphic to its Chow ring A * ⁢ ( M ⁢ ( d , χ ) ) {A^{*}(M(d,chi))} by Markman’s result. Pi and Shen have described a minimal generating set of A * ⁢ ( M ⁢ ( d , χ ) ) {A^{*}(M(d,chi))} consisting of 3 ⁢ d - 7 {3d-7} generators, which they also showed to have no relation in A ≤ d - 2 ⁢ ( M ⁢ ( d , χ ) ) {A^{leq d-2}(M(d,chi))} . We compute the two Betti numbers b 2 ⁢ ( d - 1 ) {b_{2(d-1)}} and b 2 ⁢ d {b_{2d}} of M ⁢ ( d , χ ) {M(d,chi)} , and as a corollary we show that the generators given by Pi and Shen have no relations in A ≤ d - 1 ⁢ ( M ⁢ ( d , χ ) ) {A^{leq d-1}(M(d,chi))} , but do have three linearly independent relations in A d ⁢ ( M ⁢ ( d , χ ) ) {A^{d}(M(d,chi))} .
设M ^ (d, χ) {M(d);chi)} , (d, χ) = 1 {(d);chi)=1} ,为a2上半稳定滑轮的模空间 {mathbb{P}^{2}} 支持d次曲线,并具有欧拉特征χ。上同调环H * (M¹(d, χ), M) {h ^{*}(M(d);chi),mathbb{Z})} (M) (d, χ) {M(d);chi)} 同构于它的周环A * (M) (d, χ)) {a ^{*}(M(d);chi))} 马克曼的结果。Pi和Shen描述了a * (M) (d, χ))的最小生成集 {a ^{*}(M(d);chi))} 由3∑d - 7组成 {3d-7} 在A≤d - 2减去(M减去(d, χ)) {a ^{leq d-2}(M(d);chi))} . 我们计算两个贝蒂数b2减去(d - 1) {b……{2(d-1)}} b2减去d {b……{2d}} (M) (d, χ) {M(d);chi)} 作为推论,我们证明了由Pi和Shen给出的发生器在a≤d - 1 (M) (d, χ))中没有关系。 {a ^{leq d-1}(M(d);chi))} ,但在A d¹(M¹(d, χ))中确实有三个线性无关的关系 {a ^{d}(M(d);chi))} .
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引用次数: 0
Positive rigs 积极的钻井平台
IF 0.8 3区 数学 Q1 MATHEMATICS Pub Date : 2023-11-29 DOI: 10.1515/forum-2022-0271
Matías Menni
A positive rig is a commutative and unitary semi-ring A such that 1 + x {1+x} is invertible for every x A {xin A} . We show that the category of positive rigs shares many properties with that of K-algebras for a (non-algebraically closed) field K. In particular, it is coextensive and, although we do not have an analogue of Hilbert’s basis theorem for positive rigs, we show that every finitely presentable positive rig is a finite direct product of directly indecomposable ones. We also describe free positive rigs as rigs of rational functions with non-negative rational coefficients, and we give a characterization of the positive rigs with a unique maximal ideal.
正对是一个交换酉半环A,使得1+x {1+x}对A中的每一个x∈A {xin A}可逆。我们证明了正钻机的范畴与k -代数的范畴在(非代数闭)域k上具有许多相同的性质,特别是,它是共扩展的,尽管我们没有关于正钻机的希尔伯特基定理的类似物,但我们证明了每一个有限可呈现的正钻机都是直接不可分解的有限直接积。我们还将自由正钻机描述为具有非负有理系数的有理函数钻机,并给出了具有唯一极大理想的正钻机的表征。
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引用次数: 0
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