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Fokker-Planck approach to stochastic delay differential equations.

机译:随机延迟微分方程的Fokker-Planck方法。

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摘要

Models written in terms of stochastic delay differential equations (SDDE's) have recently appeared in a number of fields, such as physiology, optics, and climatology. Unfortunately, the development of a Fokker-Planck approach for these equations is being hampered by their non-Markovian nature. In this thesis, an exact Fokker-Planck equation (FPE) is formulated for univariate SDDE's involving Gaussian white noise. Although this FPE is not self-sufficient, it is found to be helpful in at least two different contexts: with a short delay approximation and under an appropriate separation of time scales.; In the short delay approximation, a Taylor expansion is applied to an SDDE with nondelayed diffusion and yields a nondelayed stochastic differential equation. The aforementioned FPE then allows the derivation of an alternate and complementary approximation of the original SDDE. This method is illustrated with linear and logistic SDDE's.; Under the separation of time scales assumption, the FPE of a bistable system is reduced to a form that is uniquely determined by the steady-state probability density when the diffusion term of the SDDE is nondelayed. In the context of an overdamped particle with delayed coupling to a symmetrical and stochastically driven potential, the resulting FPE is used with standard techniques to express the transition rate between wells in terms of the noise amplitude and of the steady-state probability density. The same is also accomplished for the mean first passage time from one point to another. This whole approach is then applied to the case of a quartic potential, for which all realisations eventually stabilise on an oscillatory trajectory with an ever increasing amplitude. Although this latter phenomenon prevents the existence of a steady-state limit, a pseudo-steady-state probability density can be defined and used instead of the non-existent steady-state one when the transition rate to these unbounded oscillatory trajectories is sufficiently small. The transition to this peculiar attractor is investigated in more detail for a family of single-well potentials, and interestingly, the transition rate follows Arrhenius' law when the noise amplitude is small.; Overall, it is found that the Fokker-Planck approach can play a significant role in the analysis of SDDE's.
机译:用随机延迟微分方程(SDDE)编写的模型最近出现在许多领域,例如生理学,光学和气候学。不幸的是,这些方程式的非马尔可夫性质阻碍了福克-普朗克方法的发展。本文针对包含高斯白噪声的单变量SDDE,建立了精确的Fokker-Planck方程(FPE)。尽管该FPE不能自给自足,但发现它在至少两种不同的情况下是有帮助的:采用短时延近似和在适当的时间尺度分隔下进行。在短延迟近似中,将泰勒展开应用于具有无延迟扩散的SDDE,并产生无延迟随机微分方程。然后,上述FPE允许推导原始SDDE的交替和互补近似。用线性和逻辑SDDE说明了该方法。在时间尺度分离的假设下,当SDDE的扩散项不延迟时,双稳态系统的FPE减小为由稳态概率密度唯一确定的形式。在过阻尼的粒子与延迟耦合到对称且随机驱动的电势的情况下,所得的FPE与标准技术一起用于根据噪声幅度和稳态概率密度来表示孔之间的转换速率。从一个点到另一个点的平均第一次通过时间也是如此。然后将整个方法应用于四次电位的情况,为此,所有实现最终都稳定在振幅不断增加的振荡轨迹上。尽管后一种现象阻止了稳态极限的存在,但是当向这些无界振荡轨迹的过渡速率足够小时,可以定义并使用伪稳态概率密度来代替不存在的稳态概率密度。对于一个单阱电势家族,将更详细地研究向该奇异吸引子的跃迁,有趣的是,当噪声幅度较小时,跃迁速率遵循阿伦尼乌斯定律。总体而言,发现福克-普朗克方法可以在SDDE的分析中发挥重要作用。

著录项

  • 作者

    Guillouzic, Steve.;

  • 作者单位

    University of Ottawa (Canada).;

  • 授予单位 University of Ottawa (Canada).;
  • 学科 Physics General.
  • 学位 Ph.D.
  • 年度 2001
  • 页码 100 p.
  • 总页数 100
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 物理学;
  • 关键词

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