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Mean Field Limits for Interacting Diffusions in a Two-Scale Potential

机译:用于双尺度潜力的相互作用扩散的平均场限值

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In this paper, we study the combined mean field and homogenization limits for a system of weakly interacting diffusions moving in a two-scale, locally periodic confining potential, of the form considered in Duncan et al. (Brownian motion in an N-scale periodic potential, arXiv:1605.05854, 2016b). We show that, although the mean field and homogenization limits commute for finite times, they do not, in general, commute in the long time limit. In particular, the bifurcation diagrams for the stationary states can be different depending on the order with which we take the two limits. Furthermore, we construct the bifurcation diagram for the stationary McKean-Vlasov equation in a two-scale potential, before passing to the homogenization limit, and we analyze the effect of the multiple local minima in the confining potential on the number and the stability of stationary solutions.
机译:在本文中,我们研究了在Duncan等人中考虑的形式的双模,局部周期性限制潜力中移动的弱交互扩散系统的组合平均场和均匀化限制。 (布朗运动在N级周期性潜力,arxiv:1605.05854,2016b)。 我们表明,尽管平均场和均匀化限制了有限时间,但通常在很长的时间限制上通勤。 特别地,静止状态的分叉图可以根据我们采取两个限制的顺序而不同。 此外,在通过均质限制之前,在双尺度电位中构建静止McKean-Vlasov方程的分叉图,我们分析了多个局部最小值在限制潜力和静止的稳定性的效果 解决方案。

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