Gaussian approximation of dynamic cavity equations for linearly-coupled stochastic dynamics

Mattia Tarabolo, Luca Dall'Asta
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Abstract

Stochastic dynamics on sparse graphs and disordered systems often lead to complex behaviors characterized by heterogeneity in time and spatial scales, slow relaxation, localization, and aging phenomena. The mathematical tools and approximation techniques required to analyze these complex systems are still under development, posing significant technical challenges and resulting in a reliance on numerical simulations. We introduce a novel computational framework for investigating the dynamics of sparse disordered systems with continuous degrees of freedom. Starting with a graphical model representation of the dynamic partition function for a system of linearly-coupled stochastic differential equations, we use dynamic cavity equations on locally tree-like factor graphs to approximate the stochastic measure. Here, cavity marginals are identified with local functionals of single-site trajectories. Our primary approximation involves a second-order truncation of a small-coupling expansion, leading to a Gaussian form for the cavity marginals. For linear dynamics with additive noise, this method yields a closed set of causal integro-differential equations for cavity versions of one-time and two-time averages. These equations provide an exact dynamical description within the local tree-like approximation, retrieving classical results for the spectral density of sparse random matrices. Global constraints, non-linear forces, and state-dependent noise terms can be addressed using a self-consistent perturbative closure technique. The resulting equations resemble those of dynamical mean-field theory in the mode-coupling approximation used for fully-connected models. However, due to their cavity formulation, the present method can also be applied to ensembles of sparse random graphs and employed as a message-passing algorithm on specific graph instances.
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线性耦合随机动力学的动态空腔方程的高斯近似值
稀疏图和无序系统上的随机动力学常常导致复杂的行为,其特点是时间和空间尺度的异质性、缓慢弛豫、局部化和老化现象。分析这些复杂系统所需的数学工具和近似技术仍处于发展阶段,这带来了巨大的技术挑战,并导致对数值模拟的依赖。我们介绍了一种新的计算框架,用于研究具有连续自由度的稀疏无序系统的动力学。从线性耦合随机微分方程系统的动态分配函数的图形模型表示开始,我们使用局部树状因子图上的动态空穴方程来近似随机度量。在这里,空洞边际与单点轨迹的局部函数相一致。我们的主要近似方法是对小耦合扩展进行二阶截断,从而得到高斯形式的空洞边际。对于具有附加噪声的线性动力学,这种方法可以得到一组封闭的因果积分微分方程,用于空腔版本的一次平均和两次平均。这些方程在局部树状近似中提供了精确的动力学描述,检索了稀疏随机矩阵谱密度的经典结果。全局约束、非线性力和与状态相关的噪声项可以通过自洽的扰动闭合技术来解决。然而,由于其空腔形式,本方法也可应用于稀疏随机图集合,并在特定图实例上用作消息传递算法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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