具有约束势的动力学福克-普朗克方程的指数稳定性和次椭圆正则化

IF 1.3 3区 物理与天体物理 Q3 PHYSICS, MATHEMATICAL
Anton Arnold, Gayrat Toshpulatov
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引用次数: 0

摘要

本文涉及一种修正的熵方法,用于确定在整个空间中具有非二次约束势的动力学福克-普朗克方程向(唯一)稳态的大时间收敛性。我们通过分析耗散函数(广义费雪信息)中具有非常数权重矩阵的 Lyapunov 函数,扩展了之前的方法。我们在加权(H^1\)规范中建立了指数收敛性,在二次势的情况下,收敛率变得尖锐。在二次电位的缺陷情况下,即当漂移矩阵具有非三维约旦块时,福克-普朗克解与稳态之间的加权(L^2)-距离总是有一个阶为((mathcal O\big ( (1+t)e^{-t\nu /2}\big )\) 的急剧衰减估计值,其中((\nu \)为摩擦参数。提出的方法还给出了动力学福克-普朗克方程新的次椭圆正则化结果(从加权(L^2)空间到加权(H^1)空间)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Exponential Stability and Hypoelliptic Regularization for the Kinetic Fokker–Planck Equation with Confining Potential

This paper is concerned with a modified entropy method to establish the large-time convergence towards the (unique) steady state, for kinetic Fokker–Planck equations with non-quadratic confinement potentials in whole space. We extend previous approaches by analyzing Lyapunov functionals with non-constant weight matrices in the dissipation functional (a generalized Fisher information). We establish exponential convergence in a weighted \(H^1\)-norm with rates that become sharp in the case of quadratic potentials. In the defective case for quadratic potentials, i.e. when the drift matrix has non-trivial Jordan blocks, the weighted \(L^2\)-distance between a Fokker–Planck-solution and the steady state has always a sharp decay estimate of the order \(\mathcal O\big ( (1+t)e^{-t\nu /2}\big )\), with \(\nu \) the friction parameter. The presented method also gives new hypoelliptic regularization results for kinetic Fokker–Planck equations (from a weighted \(L^2\)-space to a weighted \(H^1\)-space).

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来源期刊
Journal of Statistical Physics
Journal of Statistical Physics 物理-物理:数学物理
CiteScore
3.10
自引率
12.50%
发文量
152
审稿时长
3-6 weeks
期刊介绍: The Journal of Statistical Physics publishes original and invited review papers in all areas of statistical physics as well as in related fields concerned with collective phenomena in physical systems.
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