Above and Under
    Brownian Motion

Brownian Motion , Fractional Brownian
  Motion , Levy Flight, and beyond


  Seminar Talk at Beijing Normal University
              Xiong Wang 王雄
     Centre for Chaos and Complex Networks
          City University of Hong Kong        1
Outline
   Discrete Time Random walks
    Ordinary random walks
    Lévy flights
   Generalized central limit
    theorem
     Stable distribution
   Continuous time random walks
     Ordinary Diffusion Lévy Flights
    Fractional Brownian motion
    (subdiffusion) Ambivalent processes   2
Part 1

Discrete Time Random walks

                             3
Ordinary random walks




                        4
Central limit theorem




                        5
Lévy flights
Lévy flight scales
superdiffusively
Above under and beyond brownian motion talk
Part 2

Generalized central limit
theorem
                            9
Generalized central limit
theorem
   A generalization due to Gnedenko and
    Kolmogorov states that the sum of a number
    of random variables with power-law tail
    distributions decreasing as 1 / | x | α + 1 where
    0 < α < 2 (and therefore having infinite
    variance) will tend to a stable distribution
    f(x;α,0,c,0) as the number of variables grows.



                                                    10
Stable distribution
   In probability theory, a random variable is
    said to be stable (or to have a stable
    distribution) if it has the property that a linear
    combination of two independent copies of the
    variable has the same distribution, up to
    location and scale parameters.
   The stable distribution family is also
    sometimes referred to as the Lévy alpha-
    stable distribution.
                                                     11
   Such distributions form a four-parameter
    family of continuous probability distributions
    parametrized by location and scale
    parameters μ and c, respectively, and two
    shape parameters β and α, roughly
    corresponding to measures of asymmetry
    and concentration, respectively (see the
    figures).
   C:chaosTalklevyStableDensityFunction.cdf
Characteristic function of
Stable distribution
   A random variable X is called stable if its
    characteristic function is given by




                                                  13
Symmetric α-stable distributions
with unit scale factor




                                   14
Skewed centered stable
distributions with different β




                                 15
Unified normal and power law
   For α = 2 the distribution reduces to a Gaussian
    distribution with variance σ2 = 2c2 and mean μ; the
    skewness parameter β has no effect
   The asymptotic behavior is described, for α < 2




                                                          16
Log-log plot of skewed centered stable distribution PDF's showing the
power law behavior for large x. Again the slope of the linear portions
is equal to -(α+1)
Part 1

Continuous time random walks

                               18
spatial displacement ∆x and a
temporal increment ∆t
Above under and beyond brownian motion talk
Ordinary Diffusion
Lévy Flights
Fractional Brownian motion
(subdiffusion)
1d Fractional Brownian motion
2d Fractional Brownian motion
Ambivalent processes
Above under and beyond brownian motion talk
Concluding Remarks
The ratio of the exponents α/β resembles the
interplay between sub- and superdiffusion.
For β < 2α the ambivalent CTRW is effectively
superdiffusive,
for β > 2α effectively subdiffusive.
For β = 2α the process exhibits the same
scaling as ordinary Brownian motion, despite
the crucial difference of infinite moments and a
non-Gaussian shape of the pdf W(x, t).

                                              28
Xiong Wang 王雄
Centre for Chaos and Complex Networks
City University of Hong Kong
Email: wangxiong8686@gmail.com

                                        29

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Above under and beyond brownian motion talk

  • 1. Above and Under Brownian Motion Brownian Motion , Fractional Brownian Motion , Levy Flight, and beyond Seminar Talk at Beijing Normal University Xiong Wang 王雄 Centre for Chaos and Complex Networks City University of Hong Kong 1
  • 2. Outline  Discrete Time Random walks Ordinary random walks Lévy flights  Generalized central limit theorem Stable distribution  Continuous time random walks Ordinary Diffusion Lévy Flights Fractional Brownian motion (subdiffusion) Ambivalent processes 2
  • 3. Part 1 Discrete Time Random walks 3
  • 9. Part 2 Generalized central limit theorem 9
  • 10. Generalized central limit theorem  A generalization due to Gnedenko and Kolmogorov states that the sum of a number of random variables with power-law tail distributions decreasing as 1 / | x | α + 1 where 0 < α < 2 (and therefore having infinite variance) will tend to a stable distribution f(x;α,0,c,0) as the number of variables grows. 10
  • 11. Stable distribution  In probability theory, a random variable is said to be stable (or to have a stable distribution) if it has the property that a linear combination of two independent copies of the variable has the same distribution, up to location and scale parameters.  The stable distribution family is also sometimes referred to as the Lévy alpha- stable distribution. 11
  • 12. Such distributions form a four-parameter family of continuous probability distributions parametrized by location and scale parameters μ and c, respectively, and two shape parameters β and α, roughly corresponding to measures of asymmetry and concentration, respectively (see the figures).  C:chaosTalklevyStableDensityFunction.cdf
  • 13. Characteristic function of Stable distribution  A random variable X is called stable if its characteristic function is given by 13
  • 15. Skewed centered stable distributions with different β 15
  • 16. Unified normal and power law  For α = 2 the distribution reduces to a Gaussian distribution with variance σ2 = 2c2 and mean μ; the skewness parameter β has no effect  The asymptotic behavior is described, for α < 2 16
  • 17. Log-log plot of skewed centered stable distribution PDF's showing the power law behavior for large x. Again the slope of the linear portions is equal to -(α+1)
  • 18. Part 1 Continuous time random walks 18
  • 19. spatial displacement ∆x and a temporal increment ∆t
  • 28. Concluding Remarks The ratio of the exponents α/β resembles the interplay between sub- and superdiffusion. For β < 2α the ambivalent CTRW is effectively superdiffusive, for β > 2α effectively subdiffusive. For β = 2α the process exhibits the same scaling as ordinary Brownian motion, despite the crucial difference of infinite moments and a non-Gaussian shape of the pdf W(x, t). 28
  • 29. Xiong Wang 王雄 Centre for Chaos and Complex Networks City University of Hong Kong Email: wangxiong8686@gmail.com 29