Oct 2026· Journal of Physics A: Mathematical and Theoretical· Vol 59, pp. 435002· 0 citations· 74 references
Physics
Abstract
As random displacements of many biological entities such as animals and cells often display statistical characteristics that depart from diffusion, over the years various mathematical representations to describe the so-called anomalous movement statistics have been developed. In the subdiffusive regime, that is when the variance of the occupation probability grows sublinearly in time, the fractional diffusion formalism has been employed extensively, both when space is homogeneous and in the presence of a deterministic potential. But when subdiffusive motion occurs in a spatially disordered environment, the literature is still in its infancy. Here we help to fill this gap by studying the dynamics of a subdiffusive particle in the presence of a simple spatial heterogeneity, namely a thin permeable barrier. We do so by extending to subdiffusion a recent birth–death coupled equation approach to represent diffusive barrier crossing, and by deriving a generalisation of the so-called permeable boundary condition. By using the defect technique with coupled fractional diffusion equations we are able to find analytically the dynamics of the occupation probability in space and Laplace domain, and the temporal dependence at long times of the first and second moment. As an application we consider a system composed of an infinite array of periodically placed asymmetric identical permeable barriers and study its long time dynamics. When the permeability of the barriers is unequal, despite the intrinsic motion of the particle being subdiffusive, we identify a transition from sub to superdiffusive in the growth exponent of the mean square displacement due to the coupling between the effective drift of the asymmetric barriers and subdiffusive waiting times.
The advection–diffusion equation is the canonical continuum description of transport, yet it fails for a broad class of systems in which particle motion is non-Fickian. Fractional-order advection–diffusion equations replace integer derivatives with operators of non-integer order and, in doing so, encode long-range spat...
Wei-Guang Huang· International Journal of Cre...· 0 citations
We propose a new fractional threshold-dynamics algorithm for subdiffusive interface motion and apply it to multiphase grain-growth simulations. The method combines the L1 discretization of the Caputo time derivative with a Helmholtz-resolvent thresholding step. At each time level, the L1 convolution produces a convex h...
We investigate martingale properties of heat dissipated by generic non-equilibrium overdamped Langevin dynamics with multiple dimensions and transport coefficients that may depend explicitly on time and/or space. We find quantitative criteria that establish that heat dissipation may exhibit transient martingale (time-c...
We study the large-scale behavior of critical and nearly critical space-time Hawkes processes initialized by a prescribed Poisson field of past events. The density of this initial field separates three macroscopic regimes. In the high-density regime, fluctuations average out and the event measure converges to a hydrody...
We study the time-asymptotic behaviour of solutions to a singular perturbation of the inviscid Burgers problem describing sound propagation in a radiating gas. This radiating gas model exhibits the interesting phenomenon known as metastability that has been first identified for the viscous Burgers equation. Precisely,...
We introduce and analyse an arbitrary order spatial discontinuous Galerkin (dG) method for the Dean--Kawasaki equation, a highly singular SPDE modelling density fluctuations of $N$ diffusing particles in the regime of large particle number $N \gg 1$. Our starting point is a general procedure for discretising multiplica...
Kamran Arora, Federico Cornalba, Tony Shardlow· 0 citations
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