振荡化学系统中大波动的奇异特征

IF 2.781
M. I. Dykman, V. N. Smelyanskiy, R. S. Maier, M. Silverstein
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引用次数: 5

摘要

我们研究了在一个振荡的、空间均匀的化学系统中发生大波动的方式。从一个主方程出发,我们研究了这类系统远离其极限环的平稳概率密度和其物种集中空间的最优(最可能)波动路径。最优波动路径的流场可能包含奇异点,如开关线。一条“切换线”分隔了沿不同拓扑类型的波动路径高概率到达的物种集中空间区域。当不稳定焦点位于极限环内时,在不稳定焦点附近的最优波动路径模式是奇异的和自相似的。事实上,切换线是螺旋向下到焦点的。平稳概率密度的对数在焦点附近也具有自相似的奇异结构。对于齐次Selkov模型,我们给出了最优波动路径模式的数值分析,并与解析结果进行了比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Singular Features of Large Fluctuations in Oscillating Chemical Systems†

We investigate the way in which large fluctuations in an oscillating, spatially homogeneous chemical system take place. Starting from a master equation, we study both the stationary probability density of such a system far from its limit cycle and the optimal (most probable) fluctuational paths in its space of species concentrations. The flow field of optimal fluctuational paths may contain singularities, such as switching lines. A “switching line” separates regions in the space of species concentrations that are reached, with high probability, along topologically different sorts of fluctuational paths. If an unstable focus lies inside the limit cycle, the pattern of optimal fluctuational paths is singular and self-similar near the unstable focus. In fact, a switching line spirals down to the focus. The logarithm of the stationary probability density has a self-similar singular structure near the focus as well. For a homogeneous Selkov model, we provide a numerical analysis of the pattern of optimal fluctuational paths and compare it with analytic results.

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