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Iterated random walks in random scenery (PAPAPA) 随机场景中的迭代随机漫步(PAPAPA)
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-03-01 Epub Date: 2025-12-10 DOI: 10.1016/j.spa.2025.104843
Nadine Guillotin-Plantard , Françoise Pène , Frédérique Watbled
We establish a limit theorem for a new model of 3-dimensional random walk in an inhomogeneous lattice with random orientations. This model can be seen as a 3-dimensional version of the Matheron and de Marsily model [1]. This new model leads us naturally to the study of iterated random walk in random scenery, which is a new process that can be described as a random walk in random scenery evolving in a second random scenery. We use the french acronym PAPAPA for this process unprecedented in literature, and answer a question about its stochastic behaviour asked about twenty years ago by Stéphane Le Borgne.
建立了具有随机方向的非齐次格上三维随机行走新模型的极限定理。这个模型可以看作是Matheron和de marsiy模型[1]的三维版本。这个新模型自然引导我们研究随机场景中的迭代随机行走,这是一个新的过程,可以描述为随机场景中的随机行走在第二个随机场景中的进化。我们使用法语首字母缩略词PAPAPA来描述这一史无前例的过程,并回答了大约20年前st法内·勒·博涅提出的关于其随机行为的问题。
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引用次数: 0
Convergence rate for the coupon collector’s problem with Stein’s method 用Stein方法求解优惠券收集器问题的收敛速度
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-03-01 Epub Date: 2025-11-29 DOI: 10.1016/j.spa.2025.104835
Bruno Costacèque, Laurent Decreusefond
The functional characterization of a measure, an essential but delicate aspect of Stein’s method, is shown to be accessible for stable probability distributions on convex cones. This notion encompasses the usual stable distributions e.g. Gaussian, Pareto, etc. but also the max-stable distributions: Weibull, Gumbel and Fréchet. We use the definition of max-stability to define a Markov process whose invariant measure is the stable measure of interest. In this paper, we focus on the Gumbel distribution and show how this construction can be applied to estimate the rate of convergence in the classical coupon collector’s problem.
测度的泛函特征,是斯坦因方法的一个重要而微妙的方面,被证明可用于凸锥上的稳定概率分布。这个概念包含了常见的稳定分布,如高斯分布、帕累托分布等,但也包括了极大稳定分布:威布尔分布、甘贝尔分布和弗雷姆切特分布。我们用极大稳定性的定义来定义一个马尔可夫过程,它的不变测度是我们感兴趣的稳定测度。在本文中,我们关注Gumbel分布,并展示了如何将这种结构应用于估计经典券集问题的收敛速度。
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引用次数: 0
Quasi-stationarity of the Dyson Brownian motion with collisions 带碰撞的戴森-布朗运动的准平稳性
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-03-01 Epub Date: 2025-12-15 DOI: 10.1016/j.spa.2025.104851
Arnaud Guillin , Boris Nectoux , Liming Wu
In this work, we investigate the ergodic behavior of a system of particules, subject to collisions, before it exits a fixed subdomain of its state space. This system is composed of several one-dimensional ordered Brownian particules in interaction with electrostatic repulsions, which is usually referred as the (generalized) Dyson Brownian motion. The starting points of our analysis are the work [E. Cépa and D. Lépingle, 1997 Probab. Theory Relat. Fields] which provides existence and uniqueness of such a system subject to collisions via the theory of multivalued SDEs and a Krein-Rutman type theorem derived in [A. Guillin, B. Nectoux, L. Wu, 2020 J. Eur. Math. Soc.].
在这项工作中,我们研究了一个粒子系统,受到碰撞,在它退出其状态空间的固定子域之前的遍历行为。该系统由若干一维有序布朗粒子与静电斥力相互作用组成,通常称为(广义)戴森布朗运动。我们分析的起点是工作[E]。c.c.a和d.l acimingle, 1997。代数理论。域],通过多值sde理论和[a]中导出的Krein-Rutman型定理提供了这种受碰撞影响的系统的存在唯一性。吴丽娟,吴丽娟,吴丽娟,2020 。欧元。数学。Soc。]。
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引用次数: 0
Creation of chaos for interacting Brownian particles 相互作用的布朗粒子产生混沌
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-03-01 Epub Date: 2025-12-11 DOI: 10.1016/j.spa.2025.104849
Armand Bernou , Mitia Duerinckx , Matthieu Ménard
We consider a system of N Brownian particles, with or without inertia, interacting in the mean-field regime via a weak, smooth, long-range potential, and starting initially from an arbitrary exchangeable N-particle distribution. In this model framework, we establish a fine version of the so-called creation-of-chaos phenomenon: in weak norms, the mean-field approximation for a typical particle is shown to hold with an accuracy O(N1) up to an error due solely to initial pair correlations, which is damped exponentially over time. Corresponding higher-order results are also derived in the form of higher-order correlation estimates. The approach is new and easily adaptable: we start from suboptimal correlation estimates obtained from an elementary use of Itô’s calculus on moments of the empirical measure, together with ergodic properties of the mean-field dynamics, and these bounds are then made optimal after combination with PDE estimates on the BBGKY hierarchy.
我们考虑一个由N个布朗粒子组成的系统,有或没有惯性,通过弱的、光滑的、远距离的势在平均场中相互作用,并从一个任意可交换的N粒子分布开始。在这个模型框架中,我们建立了所谓的混沌产生现象的精细版本:在弱规范中,典型粒子的平均场近似显示出精度为O(N−1),直至仅由初始对相关性引起的误差,该误差随时间呈指数衰减。相应的高阶结果也以高阶相关估计的形式导出。该方法新颖且易于适应:我们从对经验测度的矩的Itô演算的基本使用获得的次优相关估计开始,连同平均场动力学的遍历性质,然后在结合BBGKY层次上的PDE估计后使这些边界最优。
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引用次数: 0
Non-local Hamilton–Jacobi–Bellman equations for the stochastic optimal control of path-dependent piecewise deterministic processes 路径相关分段确定性过程随机最优控制的非局部Hamilton-Jacobi-Bellman方程
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-10-24 DOI: 10.1016/j.spa.2025.104813
Elena Bandini , Christian Keller
We study the optimal control of path-dependent piecewise deterministic processes. An appropriate dynamic programming principle is established. We prove that the associated value function is the unique minimax solution of the corresponding non-local path-dependent Hamilton–Jacobi–Bellman equation. This is the first well-posedness result for nonsmooth solutions of fully nonlinear non-local path-dependent partial differential equations.
研究了路径相关分段确定性过程的最优控制问题。建立了合理的动态规划原则。证明了相关值函数是相应的非局部路径相关Hamilton-Jacobi-Bellman方程的唯一极大极小解。这是完全非线性非局部路径相关偏微分方程非光滑解的第一个适定性结果。
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引用次数: 0
Local properties for 1-dimensional critical branching Lévy process 一维临界分支lsamvy过程的局部性质
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-11-15 DOI: 10.1016/j.spa.2025.104834
Haojie Hou , Yan-Xia Ren , Renming Song
<div><div>Consider a one dimensional critical branching Lévy process <span><math><mrow><mo>(</mo><msub><mrow><mrow><mo>(</mo><msub><mrow><mi>Z</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>)</mo></mrow></mrow><mrow><mi>t</mi><mo>≥</mo><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>x</mi></mrow></msub><mo>)</mo></mrow></math></span>. Assume that the offspring distribution either has finite second moment or belongs to the domain of attraction of some <span><math><mi>α</mi></math></span>-stable distribution with <span><math><mrow><mi>α</mi><mo>∈</mo><mrow><mo>(</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></mrow></mrow></math></span>, and that the underlying Lévy process <span><math><msub><mrow><mrow><mo>(</mo><msub><mrow><mi>ξ</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>)</mo></mrow></mrow><mrow><mi>t</mi><mo>≥</mo><mn>0</mn></mrow></msub></math></span> is non-lattice and has finite <span><math><mrow><mn>2</mn><mo>+</mo><msup><mrow><mi>δ</mi></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span> moment for some <span><math><mrow><msup><mrow><mi>δ</mi></mrow><mrow><mo>∗</mo></mrow></msup><mo>></mo><mn>0</mn></mrow></math></span>. We first prove that <span><span><span><math><mrow><msup><mrow><mi>t</mi></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup><mfenced><mrow><mn>1</mn><mo>−</mo><msub><mrow><mi>E</mi></mrow><mrow><msqrt><mrow><mi>t</mi></mrow></msqrt><mi>y</mi></mrow></msub><mfenced><mrow><mo>exp</mo><mfenced><mrow><mo>−</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mi>t</mi></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac><mo>−</mo><mfrac><mrow><mn>1</mn></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup></mrow></mfrac><mo>∫</mo><mi>h</mi><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><msub><mrow><mi>Z</mi></mrow><mrow><mi>t</mi></mrow></msub><mrow><mo>(</mo><mi>d</mi><mi>x</mi><mo>)</mo></mrow><mo>−</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mi>t</mi></mrow><mrow><mfrac><mrow><mn>1</mn></mrow><mrow><mi>α</mi><mo>−</mo><mn>1</mn></mrow></mfrac></mrow></msup></mrow></mfrac><mo>∫</mo><mi>g</mi><mfenced><mrow><mfrac><mrow><mi>x</mi></mrow><mrow><msqrt><mrow><mi>t</mi></mrow></msqrt></mrow></mfrac></mrow></mfenced><msub><mrow><mi>Z</mi></mrow><mrow><mi>t</mi></mrow></msub><mrow><mo>(</mo><mi>d</mi><mi>x</mi><mo>)</mo></mrow></mrow></mfenced></mrow></mfenced></mrow></mfenced></mrow></math></span></span></span>converges as <span><math><mrow><mi>t</mi><mo>→</mo><mi>∞</mi></mrow></math></span> for any non-negative bounded Lipschitz function <span><math><mi>g</mi></math></span> and any non-negative directly Riemann integrable function <span><math><mi>h</mi></math></span> of compact support. Then for any <span><math><mrow><mi>y</mi><mo>∈</mo><mi>R</mi></mrow></math></span> and bounded Borel set <span><math><mi>A</mi></math></span> of positive Lebesgue measure with its boundary having zero Lebesgue measure,
考虑一个一维临界分支lcv过程((Zt)t≥0,Px)。假设子代分布具有有限的二阶矩或属于α∈(1,2)的α-稳定分布的吸引域,并且底层的l过程(ξt)t≥0是非晶格的,并且对于某些δ∗>;0具有有限的2+δ∗矩。首先证明了t1α−11−Etyexp−1t1α−1−12∫h(x)Zt(dx)−1t1α−1∫gxtZt(dx)对于紧支持的任意非负有界Lipschitz函数g和任意非负直接Riemann可积函数h收敛于t→∞。然后,对于任意y∈R和边界为零勒贝格测度的正勒贝格测度的有界Borel集合A,在ξ上的高矩条件下,我们求出概率Pty(Zt(A)>0)的衰减率。作为应用,我们证明了Zt在条件律Pty(⋅|Zt(A)>0)下的一些收敛结果。
{"title":"Local properties for 1-dimensional critical branching Lévy process","authors":"Haojie Hou ,&nbsp;Yan-Xia Ren ,&nbsp;Renming Song","doi":"10.1016/j.spa.2025.104834","DOIUrl":"10.1016/j.spa.2025.104834","url":null,"abstract":"&lt;div&gt;&lt;div&gt;Consider a one dimensional critical branching Lévy process &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&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;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. Assume that the offspring distribution either has finite second moment or belongs to the domain of attraction of some &lt;span&gt;&lt;math&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;-stable distribution with &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, and that the underlying Lévy process &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ξ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; is non-lattice and has finite &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;δ&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;/math&gt;&lt;/span&gt; moment for some &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;δ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. We first prove that &lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;E&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msqrt&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msqrt&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mo&gt;exp&lt;/mo&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;∫&lt;/mo&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;msqrt&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msqrt&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;converges as &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;→&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for any non-negative bounded Lipschitz function &lt;span&gt;&lt;math&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; and any non-negative directly Riemann integrable function &lt;span&gt;&lt;math&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; of compact support. Then for any &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;y&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and bounded Borel set &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; of positive Lebesgue measure with its boundary having zero Lebesgue measure, ","PeriodicalId":51160,"journal":{"name":"Stochastic Processes and their Applications","volume":"192 ","pages":"Article 104834"},"PeriodicalIF":1.2,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145578989","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
Exponential ergodicity of CBIRE-processes with competition and catastrophes 具有竞争和灾难的cbre过程的指数遍历性
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-10-21 DOI: 10.1016/j.spa.2025.104807
Shukai Chen , Rongjuan Fang , Lina Ji , Jian Wang
We establish the exponential ergodicity in a weighted total variation distance of continuous-state branching processes with immigration in random environments with competition and catastrophes, under a Lyapunov-type condition and other mild assumptions. The proof is based on a Markov coupling process along with some delicate estimates for the associated coupling generator. In particular, the main result indicates whether and how the competition mechanism, the random environment and the catastrophe could balance the branching mechanism respectively to guarantee the exponential ergodicity of the processes.
在具有竞争和突变的随机环境中,在lyapunov型条件和其他温和假设下,建立了具有迁移的连续状态分支过程的加权总变异距离的指数遍历性。该证明是基于马尔可夫耦合过程以及对相关耦合发生器的一些精细估计。特别是,主要结果表明竞争机制、随机环境和突变机制是否以及如何分别平衡分支机制以保证过程的指数遍历性。
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引用次数: 0
Near-optimal shattering in the Ising pure p-spin and rarity of solutions returned by stable algorithms 伊辛纯p自旋的近最优破碎和稳定算法返回的解的稀有性
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-10-24 DOI: 10.1016/j.spa.2025.104792
Ahmed El Alaoui
We show that in the Ising pure p-spin model of spin glasses, shattering takes place at all inverse temperatures β((2logp)/p,2log2) when p is sufficiently large as a function of β. Of special interest is the lower boundary of this interval which matches the large p asymptotics of the inverse temperature marking the hypothetical dynamical transition predicted in statistical physics. We show this as a consequence of a ‘soft’ version of the overlap gap property which asserts the existence of a distance gap of points of typical energy from a typical sample from the Gibbs measure. We further show that this latter property implies that stable algorithms seeking to return a point of at least typical energy are confined to an exponentially rare subset of that super-level set, provided that their success probability is not vanishingly small.
我们证明了在自旋玻璃的Ising纯p-自旋模型中,当p作为β的函数足够大时,在所有逆温度β∈((2logp)/p,2log2)下都会发生破碎。特别令人感兴趣的是这个区间的下边界,它与逆温度的大p渐近性相匹配,这标志着统计物理学中预测的假设动力跃迁。我们将此作为重叠间隙特性的“软”版本的结果,该特性断言从吉布斯测量的典型样本中存在典型能量点的距离间隙。我们进一步表明,后一种性质意味着寻求返回至少具有典型能量的点的稳定算法仅限于该超水平集的指数稀有子集,只要它们的成功概率不是很小。
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引用次数: 0
Scaling limit for small blocks in the Chinese restaurant process 中餐馆过程中小块的缩放限制
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-10-14 DOI: 10.1016/j.spa.2025.104793
Oleksii Galganov , Andrii Ilienko
The Chinese restaurant process is a basic sequential construction of consistent random partitions. We consider random point measures describing the composition of small blocks in such partitions and show that their scaling limit is given by the projective limit of certain inhomogeneous Poisson measures on cones of increasing dimension. This result makes it possible to derive classical and functional limit theorems in the Skorokhod topology for various characteristics of the Chinese restaurant process.
中餐馆的过程是一个基本的顺序建设,一致的随机分区。我们考虑了描述这些分区中小块组成的随机点测度,并证明了它们的尺度极限是由增加维数的锥上的某些非齐次泊松测度的投影极限给出的。这一结果使得在Skorokhod拓扑中推导出适合中国餐饮过程各种特征的经典极限定理和泛函极限定理成为可能。
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引用次数: 0
Sticky diffusions on star graphs: Characterization and Itô formula 星图上的粘性扩散:表征和Itô公式
IF 1.2 2区 数学 Q3 STATISTICS & PROBABILITY Pub Date : 2026-02-01 Epub Date: 2025-10-16 DOI: 10.1016/j.spa.2025.104795
Jules Berry , Fausto Colantoni
In this paper, we investigate continuous diffusions on star graphs with sticky behaviour at the vertex. These are Markov processes with continuous paths having a positive occupation time at the vertex. We characterize the sticky diffusions as time changed nonsticky diffusions by adapting the classical technique of Itô and McKean. We prove a form of Itô formula, also known as Freidlin–Sheu formula, for this type of process. As an intermediate step, we also obtain a stochastic differential equation satisfied by the radial component of the process. These results generalize those already known for sticky diffusions on a half-line and skew sticky diffusions on the real line.
本文研究了顶点具有粘性的星图上的连续扩散问题。这些是具有连续路径的马尔可夫过程在顶点处占用时间为正。我们采用Itô和McKean的经典方法将粘性扩散表征为随时间变化的非粘性扩散。对于这类过程,我们证明了Itô公式的一种形式,也称为Freidlin-Sheu公式。作为中间步骤,我们还得到了过程径向分量所满足的随机微分方程。这些结果推广了已知的半线上的粘性扩散和实线上的偏粘性扩散。
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引用次数: 0
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