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Boundary current fluctuations for the half-space ASEP and six-vertex model 半空间 ASEP 和六顶点模型的边界电流波动
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-02-18 DOI: 10.1112/plms.12585
Jimmy He
We study fluctuations of the current at the boundary for the half-space asymmetric simple exclusion process (ASEP) and the height function of the half-space six-vertex model at the boundary at large times. We establish a phase transition depending on the effective density of particles at the boundary, with Gaussian symplectic ensemble (GSE) and Gaussian orthogonal ensemble (GOE) limits as well as the Baik–Rains crossover distribution near the critical point. This was previously known for half-space last-passage percolation, and recently established for the half-space log-gamma polymer and Kardar–Parisi–Zhang equation in the groundbreaking work of Imamura, Mucciconi, and Sasamoto. The proof uses the underlying algebraic structure of these models in a crucial way to obtain exact formulas. In particular, we show a relationship between the half-space six-vertex model and a half-space Hall–Littlewood measure with two boundary parameters, which is then matched to a free boundary Schur process via a new identity of symmetric functions. Fredholm Pfaffian formulas are established for the half-space ASEP and six-vertex model, indicating a hidden free fermionic structure.
我们研究了半空间非对称简单排斥过程(ASEP)的边界电流波动和大时间边界半空间六顶点模型的高度函数。我们在临界点附近建立了一个取决于边界粒子有效密度的相变,具有高斯折射集合(GSE)和高斯正交集合(GOE)极限以及拜克-莱恩斯交叉分布。这在半空间最后通道渗流中是已知的,最近在 Imamura、Mucciconi 和 Sasamoto 的开创性工作中为半空间 log-gamma 聚合物和 Kardar-Parisi-Zhang 方程建立了这一证明。证明中使用了这些模型的基本代数结构,从而获得了精确公式。特别是,我们展示了半空间六顶点模型与具有两个边界参数的半空间霍尔-利特尔伍德量度之间的关系,然后通过对称函数的新特性将其与自由边界舒尔过程相匹配。为半空间 ASEP 和六顶点模型建立了弗雷德霍姆-普法因子公式,表明了一种隐藏的自由费米子结构。
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引用次数: 0
Simple spines of homotopy 2-spheres are unique 同构 2 球体的简单棘刺是唯一的
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-02-14 DOI: 10.1112/plms.12583
Patrick Orson, Mark Powell
A locally flatly embedded 2-sphere in a compact 4-manifold <mjx-container aria-label="upper X" ctxtmenu_counter="0" ctxtmenu_oldtabindex="1" jax="CHTML" role="application" sre-explorer- style="font-size: 103%; position: relative;" tabindex="0"><mjx-math aria-hidden="true"><mjx-semantics><mjx-mi data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic- data-semantic-role="latinletter" data-semantic-speech="upper X" data-semantic-type="identifier"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml aria-hidden="true" display="inline" unselectable="on"><math altimg="/cms/asset/0849428e-8bdc-41aa-8881-92e8cadc8a45/plms12583-math-0001.png" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mi data-semantic-="" data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic-role="latinletter" data-semantic-speech="upper X" data-semantic-type="identifier">X</mi>$X$</annotation></semantics></math></mjx-assistive-mml></mjx-container> is called a spine if the inclusion map is a homotopy equivalence. A spine is called simple if the complement of the 2-sphere has abelian fundamental group. We prove that if two simple spines represent the same generator of <mjx-container aria-label="upper H 2 left parenthesis upper X right parenthesis" ctxtmenu_counter="1" ctxtmenu_oldtabindex="1" jax="CHTML" role="application" sre-explorer- style="font-size: 103%; position: relative;" tabindex="0"><mjx-math aria-hidden="true"><mjx-semantics><mjx-mrow data-semantic-annotation="clearspeak:simple" data-semantic-children="2,6" data-semantic-content="7,0" data-semantic- data-semantic-role="simple function" data-semantic-speech="upper H 2 left parenthesis upper X right parenthesis" data-semantic-type="appl"><mjx-msub data-semantic-children="0,1" data-semantic- data-semantic-parent="8" data-semantic-role="simple function" data-semantic-type="subscript"><mjx-mi data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic- data-semantic-operator="appl" data-semantic-parent="2" data-semantic-role="simple function" data-semantic-type="identifier"><mjx-c></mjx-c></mjx-mi><mjx-script style="vertical-align: -0.15em; margin-left: -0.057em;"><mjx-mn data-semantic-annotation="clearspeak:simple" data-semantic-font="normal" data-semantic- data-semantic-parent="2" data-semantic-role="integer" data-semantic-type="number" size="s"><mjx-c></mjx-c></mjx-mn></mjx-script></mjx-msub><mjx-mo data-semantic-added="true" data-semantic- data-semantic-operator="appl" data-semantic-parent="8" data-semantic-role="application" data-semantic-type="punctuation" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo><mjx-mrow data-semantic-children="4" data-semantic-content="3,5" data-semantic- data-semantic-parent="8" data-semantic-role="leftright" data-semantic-type="fenced"><mjx-mo data-semantic- data-semantic-operator="fenced" data-semantic-parent="6" data-semantic-role="open" data-semant
如果包含映射是同调等价的,那么紧凑四芒星 X$X$ 中局部平嵌的 2 球称为脊。如果 2 球的补集具有非良性基群,则称为简单脊。我们证明,如果两个简单脊柱代表 H2(X)$H_2(X)$ 的同一个生成器,那么它们就是同构的。特别是,该定理适用于结迹中的简单摇动切片 2 球。
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引用次数: 0
On the number of high-dimensional partitions 关于高维分区的数量
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-02-14 DOI: 10.1112/plms.12586
Cosmin Pohoata, Dmitrii Zakharov
Let <mjx-container aria-label="upper P Subscript d Baseline left parenthesis n right parenthesis" ctxtmenu_counter="0" ctxtmenu_oldtabindex="1" jax="CHTML" role="application" sre-explorer- style="font-size: 103%; position: relative;" tabindex="0"><mjx-math aria-hidden="true"><mjx-semantics><mjx-mrow data-semantic-annotation="clearspeak:simple" data-semantic-children="2,6" data-semantic-content="7,0" data-semantic- data-semantic-role="simple function" data-semantic-speech="upper P Subscript d Baseline left parenthesis n right parenthesis" data-semantic-type="appl"><mjx-msub data-semantic-children="0,1" data-semantic- data-semantic-parent="8" data-semantic-role="simple function" data-semantic-type="subscript"><mjx-mi data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic- data-semantic-operator="appl" data-semantic-parent="2" data-semantic-role="simple function" data-semantic-type="identifier"><mjx-c></mjx-c></mjx-mi><mjx-script style="vertical-align: -0.15em; margin-left: -0.109em;"><mjx-mi data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic- data-semantic-parent="2" data-semantic-role="latinletter" data-semantic-type="identifier" size="s"><mjx-c></mjx-c></mjx-mi></mjx-script></mjx-msub><mjx-mo data-semantic-added="true" data-semantic- data-semantic-operator="appl" data-semantic-parent="8" data-semantic-role="application" data-semantic-type="punctuation" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo><mjx-mrow data-semantic-children="4" data-semantic-content="3,5" data-semantic- data-semantic-parent="8" data-semantic-role="leftright" data-semantic-type="fenced"><mjx-mo data-semantic- data-semantic-operator="fenced" data-semantic-parent="6" data-semantic-role="open" data-semantic-type="fence" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo><mjx-mi data-semantic-annotation="clearspeak:simple" data-semantic-font="italic" data-semantic- data-semantic-parent="6" data-semantic-role="latinletter" data-semantic-type="identifier"><mjx-c></mjx-c></mjx-mi><mjx-mo data-semantic- data-semantic-operator="fenced" data-semantic-parent="6" data-semantic-role="close" data-semantic-type="fence" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo></mjx-mrow></mjx-mrow></mjx-semantics></mjx-math><mjx-assistive-mml aria-hidden="true" display="inline" unselectable="on"><math altimg="/cms/asset/127a3c0f-7553-4810-ba2f-0ecc75bac01f/plms12586-math-0001.png" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow data-semantic-="" data-semantic-annotation="clearspeak:simple" data-semantic-children="2,6" data-semantic-content="7,0" data-semantic-role="simple function" data-semantic-speech="upper P Subscript d Baseline left parenthesis n right parenthesis" data-semantic-type="appl"><msub data-semantic-="" data-semantic-children="0,1" data-semantic-parent="8" data-semantic-role="simple function" data-semantic-type="subscript
让 Pd(n)$P_{d}(n)$ 表示条目来自 {0,1,...n}$lbrace 0,1,ldots,nrbrace$ 的 n×...×nd$n times ldots times n d$ 维分区的个数。在 Balogh-Treglown-Wagner 和 Noel-Scott-Sudakov 的研究基础上,我们证明了当 d→∞$d rightarrow infty$ 时、
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引用次数: 0
The Loewner–Kufarev energy and foliations by Weil–Petersson quasicircles 卢瓦纳-库法里夫能量和魏尔-彼得森准圆的叶状结构
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-02-13 DOI: 10.1112/plms.12582
Fredrik Viklund, Yilin Wang
We study foliations by chord–arc Jordan curves of the twice punctured Riemann sphere <mjx-container aria-label="double struck upper C minus StartSet 0 EndSet" ctxtmenu_counter="0" ctxtmenu_oldtabindex="1" jax="CHTML" role="application" sre-explorer- style="font-size: 103%; position: relative;" tabindex="0"><mjx-math aria-hidden="true"><mjx-semantics><mjx-mrow data-semantic-children="0,5" data-semantic-content="1" data-semantic- data-semantic-role="subtraction" data-semantic-speech="double struck upper C minus StartSet 0 EndSet" data-semantic-type="infixop"><mjx-mi data-semantic-font="double-struck" data-semantic- data-semantic-parent="6" data-semantic-role="numbersetletter" data-semantic-type="identifier"><mjx-c></mjx-c></mjx-mi><mjx-mo data-semantic- data-semantic-operator="infixop,∖" data-semantic-parent="6" data-semantic-role="subtraction" data-semantic-type="operator" rspace="4" space="4"><mjx-c></mjx-c></mjx-mo><mjx-mrow data-semantic-children="3" data-semantic-content="2,4" data-semantic- data-semantic-parent="6" data-semantic-role="set singleton" data-semantic-type="fenced"><mjx-mo data-semantic- data-semantic-operator="fenced" data-semantic-parent="5" data-semantic-role="open" data-semantic-type="fence" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo><mjx-mn data-semantic-annotation="clearspeak:simple" data-semantic-font="normal" data-semantic- data-semantic-parent="5" data-semantic-role="integer" data-semantic-type="number"><mjx-c></mjx-c></mjx-mn><mjx-mo data-semantic- data-semantic-operator="fenced" data-semantic-parent="5" data-semantic-role="close" data-semantic-type="fence" style="margin-left: 0.056em; margin-right: 0.056em;"><mjx-c></mjx-c></mjx-mo></mjx-mrow></mjx-mrow></mjx-semantics></mjx-math><mjx-assistive-mml aria-hidden="true" display="inline" unselectable="on"><math altimg="/cms/asset/18b294c8-16a0-4c92-85bd-1f96c88b00a8/plms12582-math-0001.png" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow data-semantic-="" data-semantic-children="0,5" data-semantic-content="1" data-semantic-role="subtraction" data-semantic-speech="double struck upper C minus StartSet 0 EndSet" data-semantic-type="infixop"><mi data-semantic-="" data-semantic-font="double-struck" data-semantic-parent="6" data-semantic-role="numbersetletter" data-semantic-type="identifier" mathvariant="double-struck">C</mi><mo data-semantic-="" data-semantic-operator="infixop,∖" data-semantic-parent="6" data-semantic-role="subtraction" data-semantic-type="operator">∖</mo><mrow data-semantic-="" data-semantic-children="3" data-semantic-content="2,4" data-semantic-parent="6" data-semantic-role="set singleton" data-semantic-type="fenced"><mo data-semantic-="" data-semantic-operator="fenced" data-semantic-parent="5" data-semantic-role="open" data-semantic-type="fence" stretchy="false">{</mo><mn data-semantic-="" data-semantic-annotation="clearspeak:simple" data-semantic-font="normal" data-semantic-parent="5" data-semantic-role="integer"
我们通过两次穿刺黎曼球 C∖{0}$mathbb{C}的弦弧乔丹曲线来研究叶形。setminus lbrace 0rbrace$ 使用卢瓦纳-库法列夫方程。我们将平面上的一个函数与这样的叶片关联起来,这个函数描述了沿每个叶片的 "局部卷绕"。我们的主要定理是,当且仅当洛厄纳驱动度量 ρ$rho$ 具有有限的洛厄纳-库法列弗能量时,这个函数才具有有限的迪里夏特能量,其定义为
{"title":"The Loewner–Kufarev energy and foliations by Weil–Petersson quasicircles","authors":"Fredrik Viklund, Yilin Wang","doi":"10.1112/plms.12582","DOIUrl":"https://doi.org/10.1112/plms.12582","url":null,"abstract":"We study foliations by chord–arc Jordan curves of the twice punctured Riemann sphere &lt;mjx-container aria-label=\"double struck upper C minus StartSet 0 EndSet\" ctxtmenu_counter=\"0\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"&gt;&lt;mjx-math aria-hidden=\"true\"&gt;&lt;mjx-semantics&gt;&lt;mjx-mrow data-semantic-children=\"0,5\" data-semantic-content=\"1\" data-semantic- data-semantic-role=\"subtraction\" data-semantic-speech=\"double struck upper C minus StartSet 0 EndSet\" data-semantic-type=\"infixop\"&gt;&lt;mjx-mi data-semantic-font=\"double-struck\" data-semantic- data-semantic-parent=\"6\" data-semantic-role=\"numbersetletter\" data-semantic-type=\"identifier\"&gt;&lt;mjx-c&gt;&lt;/mjx-c&gt;&lt;/mjx-mi&gt;&lt;mjx-mo data-semantic- data-semantic-operator=\"infixop,∖\" data-semantic-parent=\"6\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" rspace=\"4\" space=\"4\"&gt;&lt;mjx-c&gt;&lt;/mjx-c&gt;&lt;/mjx-mo&gt;&lt;mjx-mrow data-semantic-children=\"3\" data-semantic-content=\"2,4\" data-semantic- data-semantic-parent=\"6\" data-semantic-role=\"set singleton\" data-semantic-type=\"fenced\"&gt;&lt;mjx-mo data-semantic- data-semantic-operator=\"fenced\" data-semantic-parent=\"5\" data-semantic-role=\"open\" data-semantic-type=\"fence\" style=\"margin-left: 0.056em; margin-right: 0.056em;\"&gt;&lt;mjx-c&gt;&lt;/mjx-c&gt;&lt;/mjx-mo&gt;&lt;mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"integer\" data-semantic-type=\"number\"&gt;&lt;mjx-c&gt;&lt;/mjx-c&gt;&lt;/mjx-mn&gt;&lt;mjx-mo data-semantic- data-semantic-operator=\"fenced\" data-semantic-parent=\"5\" data-semantic-role=\"close\" data-semantic-type=\"fence\" style=\"margin-left: 0.056em; margin-right: 0.056em;\"&gt;&lt;mjx-c&gt;&lt;/mjx-c&gt;&lt;/mjx-mo&gt;&lt;/mjx-mrow&gt;&lt;/mjx-mrow&gt;&lt;/mjx-semantics&gt;&lt;/mjx-math&gt;&lt;mjx-assistive-mml aria-hidden=\"true\" display=\"inline\" unselectable=\"on\"&gt;&lt;math altimg=\"/cms/asset/18b294c8-16a0-4c92-85bd-1f96c88b00a8/plms12582-math-0001.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;semantics&gt;&lt;mrow data-semantic-=\"\" data-semantic-children=\"0,5\" data-semantic-content=\"1\" data-semantic-role=\"subtraction\" data-semantic-speech=\"double struck upper C minus StartSet 0 EndSet\" data-semantic-type=\"infixop\"&gt;&lt;mi data-semantic-=\"\" data-semantic-font=\"double-struck\" data-semantic-parent=\"6\" data-semantic-role=\"numbersetletter\" data-semantic-type=\"identifier\" mathvariant=\"double-struck\"&gt;C&lt;/mi&gt;&lt;mo data-semantic-=\"\" data-semantic-operator=\"infixop,∖\" data-semantic-parent=\"6\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\"&gt;∖&lt;/mo&gt;&lt;mrow data-semantic-=\"\" data-semantic-children=\"3\" data-semantic-content=\"2,4\" data-semantic-parent=\"6\" data-semantic-role=\"set singleton\" data-semantic-type=\"fenced\"&gt;&lt;mo data-semantic-=\"\" data-semantic-operator=\"fenced\" data-semantic-parent=\"5\" data-semantic-role=\"open\" data-semantic-type=\"fence\" stretchy=\"false\"&gt;{&lt;/mo&gt;&lt;mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"5\" data-semantic-role=\"integer\"","PeriodicalId":49667,"journal":{"name":"Proceedings of the London Mathematical Society","volume":"55 1","pages":""},"PeriodicalIF":1.8,"publicationDate":"2024-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139759322","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
Diophantine approximation, large intersections and geodesics in negative curvature 负曲率中的 Diophantine 近似、大交点和测地线
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-02-10 DOI: 10.1112/plms.12581
Anish Ghosh, Debanjan Nandi
In this paper, we prove quantitative results about geodesic approximations to submanifolds in negatively curved spaces. Among the main tools is a new and general Jarník–Besicovitch type theorem in Diophantine approximation. Our framework allows manifolds of variable negative curvature, a variety of geometric targets, and logarithm laws as well as spiraling phenomena in both measure and dimension aspect. Several of the results are new also for manifolds of constant negative sectional curvature. We further establish a large intersection property of Falconer in this context.
在本文中,我们证明了关于负弯曲空间中子线面的大地近似的定量结果。其中的主要工具是 Diophantine approximation 中新的通用 Jarník-Besicovitch 型定理。我们的框架允许可变负曲率流形、各种几何目标、对数法则以及度量和维度方面的螺旋现象。其中一些结果也是针对恒定负截面曲率流形的新结果。在此背景下,我们进一步建立了 Falconer 的大交点性质。
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引用次数: 0
Geometry of canonical genus 4 curves 典型属 4 曲线几何学
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2024-01-15 DOI: 10.1112/plms.12577
Fatemeh Rezaee
We apply the machinery of Bridgeland stability conditions on derived categories of coherent sheaves to describe the geometry of classical moduli spaces associated with canonical genus 4 space curves via an effective control over its wall-crossing. This article provides the first description of a moduli space of Pandharipande–Thomas stable pairs that is used as an intermediate step toward the description of the associated Hilbert scheme, which in turn is the first example where the components of a classical moduli space were completely determined via wall-crossing. We give a full list of irreducible components of the space of stable pairs, along with a birational description of each component, and a partial list for the Hilbert scheme. There are several long standing open problems regarding classical sheaf theoretic moduli spaces, and the present work will shed light on further studies of such moduli spaces such as Hilbert schemes of curves and moduli of stable pairs that are very hard to tackle without the wall-crossing techniques.
我们将布里奇兰稳定性条件的机制应用于相干剪切的派生范畴,通过对其壁交的有效控制来描述与典型属4空间曲线相关的经典模空间的几何。本文首次描述了潘达里潘德-托马斯稳定对的模空间,并将其作为描述相关希尔伯特方案的中间步骤。我们给出了稳定对空间不可还原成分的完整列表,以及每个成分的双向描述和希尔伯特方案的部分列表。关于经典剪子理论模空间有几个长期未决的问题,本研究将为进一步研究此类模空间(如曲线的希尔伯特方案和稳定对的模空间)提供启发,而不使用壁交技术是很难解决这些问题的。
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引用次数: 0
On the existence of harmonic metrics on non-Hermitian Yang–Mills bundles 论非ermitian Yang-Mills 束上谐波度量的存在性
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2023-12-25 DOI: 10.1112/plms.12580
Changpeng Pan, Zhenghan Shen, Xi Zhang
In this paper, we study the non-Hermitian Yang–Mills (NHYM) bundles over compact Kähler manifolds. We show that the existence of harmonic metrics is equivalent to the semisimplicity of NHYM bundles, which confirms the Conjecture 8.7 in Kaledin and Verbitsky (Selecta Math. (N.S.) 4 (1998) 279–320).
在本文中,我们研究了紧凑凯勒流形上的非全息杨-米尔斯(NHYM)束。我们证明了调和度量的存在等同于 NHYM 束的半简单性,这证实了 Kaledin 和 Verbitsky (Selecta Math. (N.S.) 4 (1998) 279-320) 中的猜想 8.7。
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引用次数: 0
The spectrum of a twisted commutative algebra 扭曲交换代数的谱
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2023-12-22 DOI: 10.1112/plms.12576
Andrew Snowden
A twisted commutative algebra is (for us) a commutative Q�$mathbf {Q}$�-algebra equipped with an action of the infinite general linear group. In such algebras, the “GL�$mathbf {GL}$�-prime” ideals assume the duties fulfilled by prime ideals in ordinary commutative algebra, and so it is crucial to understand them. Unfortunately, distinct GL�$mathbf {GL}$�-primes can have the same radical, which obstructs one from studying them geometrically. We show that this problem can be eliminated by working with super vector spaces: doing so provides enough geometry to distinguish GL�$mathbf {GL}$�-primes. This yields an effective method for analyzing GL�$mathbf {GL}$�-primes.
扭曲交换代数(对我们来说)是一个交换 Q$mathbf {Q}$-代数,带有无限一般线性群的作用。在这样的代数中,"GL$mathbf {GL$}-prime" 理想承担着普通交换代数中素数理想的职责,因此理解它们至关重要。遗憾的是,不同的 GL$mathbf {GL}$-prime 可以具有相同的根,这阻碍了我们从几何学角度对它们进行研究。我们的研究表明,这个问题可以通过超向量空间来解决:超向量空间提供了足够的几何图形来区分 GL$mathbf {GL}$-primes 。这就产生了分析 GL$mathbf {GL}$-primes 的有效方法。
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引用次数: 0
Rates of mixing for the measure of maximal entropy of dispersing billiard maps 分散台球图最大熵量的混合率
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2023-12-20 DOI: 10.1112/plms.12578
Mark F. Demers, Alexey Korepanov
In a recent work, Baladi and Demers constructed a measure of maximal entropy for finite horizon dispersing billiard maps and proved that it is unique, mixing and moreover Bernoulli. We show that this measure enjoys natural probabilistic properties for Hölder continuous observables, such as at least polynomial decay of correlations and the Central Limit Theorem. The results of Baladi and Demers are subject to a condition of sparse recurrence to singularities. We use a similar and slightly stronger condition, and it has a direct effect on our rate of decay of correlations. For billiard tables with bounded complexity (a property conjectured to be generic), we show that the sparse recurrence condition is always satisfied and the correlations decay at a super-polynomial rate.
在最近的一项研究中,Baladi 和 Demers 构建了有限视界分散台球映射的最大熵量,并证明了它的唯一性、混合性和伯努利性。我们证明,对于赫尔德连续观测变量,这一量度具有天然的概率特性,如相关性的至少多项式衰减和中心极限定理。Baladi 和 Demers 的结果受制于奇点稀疏递归条件。我们使用了一个类似但稍强的条件,它对我们的相关性衰减率有直接影响。对于复杂度有界的台球桌(这一性质被猜测为通用性质),我们证明稀疏递归条件总是满足的,相关性以超多项式速率衰减。
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引用次数: 0
Slowly recurrent Collet–Eckmann maps with non-empty Fatou set 具有非空 Fatou 集的缓慢递归 Collet-Eckmann 地图
IF 1.8 1区 数学 Q1 MATHEMATICS Pub Date : 2023-12-19 DOI: 10.1112/plms.12574
Magnus Aspenberg, Mats Bylund, Weiwei Cui
In this paper, we study rational Collet–Eckmann maps for which the Julia set is not the whole sphere and for which the critical points are recurrent at a slow rate. In families where the orders of the critical points are fixed, we prove that such maps are Lebesgue density points of hyperbolic maps. In particular, if all critical points are simple, these maps are Lebesgue density points of hyperbolic maps in the full space of rational maps of any degree d2�$d geqslant 2$�.
在本文中,我们研究了有理 Collet-Eckmann 映射,对于这些映射,Julia 集不是整个球面,而且临界点以缓慢的速度反复出现。在临界点阶数固定的族中,我们证明了这类映射是双曲映射的勒贝格密度点。特别是,如果所有临界点都是简单的,这些映射就是任意度 d⩾2$d geqslant 2$ 的有理映射全空间中双曲映射的 Lebesgue 密度点。
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Proceedings of the London Mathematical Society
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