arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2005.11740math.PRcs.NAmath.APmath.NA
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相互作用粒子系统随机批处理方法的平均场极限

On the mean field limit of the Random Batch Method for interacting particle systems

Shi Jin, Lei Li

摘要:

在我们以前的工作中提出的随机批处理方法[Jin等人,J. Comput.物理、400(1),2020]不仅是研究相互作用粒子系统及其平均场极限的数值方法,而且可以看作是粒子与随机选择的小批量粒子在离散时间相互作用的粒子系统模型。在本文中,我们研究了该模型的平均场极限作为粒子数$N \to \infty$。与经典的相互作用粒子系统的平均场极限不同,在经典的平均场极限中,大数定律起作用,混沌传播到以后的时间,平均场极限现在不依赖于大数定律,混沌在每个离散时间被施加。尽管如此,我们将不仅证明这个平均场极限(离散的时间),但也将表明,限制,作为离散的时间间隔$τ\to 0$,方法的解决方案的非线性福克-普朗克方程所产生的平均场极限的原始相互作用粒子系统在Wasserstein距离。

英文摘要:

The Random Batch Method proposed in our previous work [Jin et al., J. Comput. Phys., 400(1), 2020] is not only a numerical method for interacting particle systems and its mean-field limit, but also can be viewed as a model of particle system in which particles interact, at discrete time, with randomly selected mini-batch of particles. In this paper we investigate the mean-field limit of this model as the number of particles $N \to \infty$. Unlike the classical mean field limit for interacting particle systems where the law of large numbers plays the role and the chaos is propagated to later times, the mean field limit now does not rely on the law of large numbers and chaos is imposed at every discrete time. Despite this, we will not only justify this mean-field limit (discrete in time) but will also show that the limit, as the discrete time interval $τ\to 0$, approaches to the solution of a nonlinear Fokker-Planck equation arising as the mean-field limit of the original interacting particle system in Wasserstein distance.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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