The mean first exit time, escape probability and transitional probability densities are utilized to quantify dynamical behaviors of stochastic differential equations with non-Gaussian, α-stable type Lévy motions. Taking advantage of the Toeplitz matrix structure of the time-space discretization, a fast and accurate numerical algorithm is proposed to simulate the nonlocal Fokker-Planck equations on either a bounded or infinite domain. Under a specified condition, the scheme is shown to satisfy a discrete maximum principle and to be convergent. The numerical results for two prototypical stochastic systems, the Ornstein-Uhlenbeck system and the double-well system are shown
The lecture outlines the most important mathematical facts about stochastic processes which are desc...
Minimal models for the explanation of decision-making in computational neuroscience are based on the...
The aim of this talk is the analysis of various stability issues for numerical methods designed to s...
The solution of an n-dimensional stochastic differential equation driven by Gaussian white noises is...
The mean exit time and transition probability density function are macroscopic quantities used to de...
The purpose of this report is to introduce the engineer to the area of stochastic differential equat...
The response of a dynamical system modelled by differential equations with white noise as the forcin...
We consider stochastic differential equations for a variable q with multiplicative white and non...
The Euler scheme is a well-known method of approximation of solutions of stochastic differential equ...
Fokker-Planck equations, along with stochastic differential equations, play vital roles in physics, ...
Abstract. Construction of splitting-step methods and properties of related non-negativity and bounda...
Abstract. Construction of splitting-step methods and properties of related non-negativity and bounda...
A stochastic process or sometimes called random process is the counterpart to a deterministic proces...
Three types of quantitative structures, stochastic inertial manifolds, random invariant foliations, ...
We described the first passage time distribution associated to the stochastic evolution fr...
The lecture outlines the most important mathematical facts about stochastic processes which are desc...
Minimal models for the explanation of decision-making in computational neuroscience are based on the...
The aim of this talk is the analysis of various stability issues for numerical methods designed to s...
The solution of an n-dimensional stochastic differential equation driven by Gaussian white noises is...
The mean exit time and transition probability density function are macroscopic quantities used to de...
The purpose of this report is to introduce the engineer to the area of stochastic differential equat...
The response of a dynamical system modelled by differential equations with white noise as the forcin...
We consider stochastic differential equations for a variable q with multiplicative white and non...
The Euler scheme is a well-known method of approximation of solutions of stochastic differential equ...
Fokker-Planck equations, along with stochastic differential equations, play vital roles in physics, ...
Abstract. Construction of splitting-step methods and properties of related non-negativity and bounda...
Abstract. Construction of splitting-step methods and properties of related non-negativity and bounda...
A stochastic process or sometimes called random process is the counterpart to a deterministic proces...
Three types of quantitative structures, stochastic inertial manifolds, random invariant foliations, ...
We described the first passage time distribution associated to the stochastic evolution fr...
The lecture outlines the most important mathematical facts about stochastic processes which are desc...
Minimal models for the explanation of decision-making in computational neuroscience are based on the...
The aim of this talk is the analysis of various stability issues for numerical methods designed to s...