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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
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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