Continuous-time random walk
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In mathematics, a continuous-time random walk (CTRW) is a generalization of a
random walk In mathematics, a random walk is a random process that describes a path that consists of a succession of random steps on some mathematical space. An elementary example of a random walk is the random walk on the integer number line \mathbb Z ...
where the wandering particle waits for a random time between jumps. It is a
stochastic Stochastic (, ) refers to the property of being well described by a random probability distribution. Although stochasticity and randomness are distinct in that the former refers to a modeling approach and the latter refers to phenomena themselv ...
jump process with arbitrary distributions of jump lengths and waiting times. More generally it can be seen to be a special case of a
Markov renewal process In probability and statistics, a Markov renewal process (MRP) is a random process that generalizes the notion of Markov jump processes. Other random processes like Markov chains, Poisson processes and renewal processes can be derived as special ...
.


Motivation

CTRW was introduced by Montroll and Weiss as a generalization of physical diffusion process to effectively describe
anomalous diffusion Anomalous diffusion is a diffusion process with a non-linear relationship between the mean squared displacement (MSD), \langle r^(\tau )\rangle , and time. This behavior is in stark contrast to Brownian motion, the typical diffusion process descri ...
, i.e., the super- and sub-diffusive cases. An equivalent formulation of the CTRW is given by generalized master equations. A connection between CTRWs and diffusion equations with fractional time derivatives has been established. Similarly, time-space fractional diffusion equations can be considered as CTRWs with continuously distributed jumps or continuum approximations of CTRWs on lattices.


Formulation

A simple formulation of a CTRW is to consider the stochastic process X(t) defined by : X(t) = X_0 + \sum_^ \Delta X_i, whose increments \Delta X_i are iid random variables taking values in a domain \Omega and N(t) is the number of jumps in the interval (0,t). The probability for the process taking the value X at time t is then given by : P(X,t) = \sum_^\infty P(n,t) P_n(X). Here P_n(X) is the probability for the process taking the value X after n jumps, and P(n,t) is the probability of having n jumps after time t.


Montroll–Weiss formula

We denote by \tau the waiting time in between two jumps of N(t) and by \psi(\tau) its distribution. The
Laplace transform In mathematics, the Laplace transform, named after its discoverer Pierre-Simon Laplace (), is an integral transform that converts a function of a real variable (usually t, in the '' time domain'') to a function of a complex variable s (in the ...
of \psi(\tau) is defined by : \tilde(s)=\int_0^ d\tau \, e^ \psi(\tau). Similarly, the
characteristic function In mathematics, the term "characteristic function" can refer to any of several distinct concepts: * The indicator function of a subset, that is the function ::\mathbf_A\colon X \to \, :which for a given subset ''A'' of ''X'', has value 1 at points ...
of the jump distribution f(\Delta X) is given by its
Fourier transform A Fourier transform (FT) is a mathematical transform that decomposes functions into frequency components, which are represented by the output of the transform as a function of frequency. Most commonly functions of time or space are transformed ...
: : \hat(k)=\int_\Omega d(\Delta X) \, e^ f(\Delta X). One can show that the Laplace–Fourier transform of the probability P(X,t) is given by : \hat(k,s) = \frac \frac. The above is called MontrollWeiss formula.


Examples


References

{{Stochastic processes Variants of random walks