Understanding particle transport is a
problem of theoretical and practical importance in plasma physics,
geophysical fluid dynamics, laboratory experiments and engineering.
Because of the intrinsic unpredictability that particle trajectories
typically exhibit, one has to abandon the idea of studying individual
trajectories, and consider instead an statistical approach in which
transport is characterized by ensemble averaged properties of
particle motion. A commonly used statistical measures of transport is
the variance,
is the particle displacement, and < > denotes average over an
ensemble of particles. One of the most basic transport problems is
the study of the long-time behavior of the variance and of the
probability density function (PDF) of particle displacement, A naive
approach of this problem would assume that, at long times
is
a Gaussian distribution evolving in time according to an
advection-diffusion equation with a mean transport velocity, and an
effective diffusivity,
.Although
this approach has been fruitful in the study of passive scalar
transport in homogeneous isotropic turbulence, and in the study of
Brownian motion, it fails when there is anomalous diffusion.Anomalous
diffusion occurs when there is not a well-defined diffusion
coefficient, i.e. when
in which case D is either zero or infinite. Our general goal is to
study anomalous diffusion due to coherent structures (e.g. zonal
flows and vortices) in systems of interest to plasma physics and
geophysical fluid dynamics.

Anomalous diffusion and Levy flights in two-dimensional rotating flows
Asymmetric transport and non-Gaussian statistics of passive scalars