Continuous-time random walk

In mathematics, a continuous-time random walk (CTRW) is a generalization of a random walk where the wandering particle waits for a random time between jumps. It is a stochastic jump process with arbitrary distributions of jump lengths and waiting times.[1][2][3] More generally it can be seen to be a special case of a Markov renewal process.

Motivation

CTRW was introduced by Montroll and Weiss [4] as a generalization of physical diffusion process to effectively describe anomalous diffusion, i.e., the super- and sub-diffusive cases. An equivalent formulation of the CTRW is given by generalized master equations. [5] A connection between CTRWs and diffusion equations with fractional time derivatives has been established. [6] Similarly, time-space fractional diffusion equations can be considered as CTRWs with continuously distributed jumps or continuum approximations of CTRWs on lattices. [7]

Formulation

A simple formulation of a CTRW is to consider the stochastic process X(t) defined by


X(t) = X_0 + \sum_{i=1}^{N(t)} \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_{n=0}^\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 of \psi(\tau) is defined by


\tilde{\psi}(s)=\int_0^{\infty} d\tau \, e^{-\tau s} \psi(\tau).

Similarly, the characteristic function of the jump distribution  f(\Delta X) is given by its Fourier transform:


\hat{f}(k)=\int_\Omega d(\Delta X) \, e^{i k\Delta X} f(\Delta X).

One can show that the Laplace-Fourier transform of the probability P(X,t) is given by


\hat{\tilde{P}}(k,s) = \frac{1-\tilde{\psi}(s)}{s} \frac{1}{1-\tilde{\psi}(s)\hat{f}(k)}.

The above is called Montroll-Weiss formula.

Examples

The Wiener process is the standard example of a continuous time random walk in which the waiting times are exponential and the jumps are continuous and normally distributed.

References

  1. Klages, Rainer; Radons, Guenther; Sokolov, Igor M. Anomalous Transport: Foundations and Applications.
  2. Paul, Wolfgang; Baschnagel, Jörg (2013-07-11). Stochastic Processes: From Physics to Finance. Springer Science & Business Media. pp. 72–. ISBN 9783319003276. Retrieved 25 July 2014.
  3. Slanina, Frantisek (2013-12-05). Essentials of Econophysics Modelling. OUP Oxford. pp. 89–. ISBN 9780191009075. Retrieved 25 July 2014.
  4. Elliott W. Montroll and George H. Weiss (1965). "Random Walks on Lattices. II". J. Math. Phys. 6: 167. doi:10.1063/1.1704269.
  5. . M. Kenkre, E. W. Montroll, M. F. Shlesinger (1973). "Generalized master equations for continuous-time random walks". Journal of Statistical Physics 9 (1): 45–50. doi:10.1007/BF01016796.
  6. Hilfer, R. and Anton, L. (1995). "Fractional master equations and fractal time random walks". Phys. Rev. E 51 (2): R848––R851. doi:10.1103/PhysRevE.51.R848.
  7. Gorenflo, Rudolf; Mainardi, Francesco; Vivoli, Alessandro (2005). "Continuous-time random walk and parametric subordination in fractional diffusion". Chaos, Solitons \& Fractals (Elsevier) 34 (1): 87–103. doi:10.1016/j.chaos.2007.01.052.


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