Anomalous diffusion

Mean squared displacement ${\displaystyle \langle r^{2}(\tau )\rangle }$ for different types of anomalous diffusion

Anomalous diffusion is a diffusion process with a non-linear relationship between the mean squared displacement (MSD), ${\displaystyle \langle r^{2}(\tau )\rangle }$, and time. This behavior is in stark contrast to Brownian motion, the typical diffusion process described by Einstein and Smoluchowski, where the MSD is a linear in time (namely, ${\displaystyle \langle r^{2}(\tau )\rangle =2dD\tau }$ with d being the number of dimensions and D the diffusion coefficient).^[1][2] Examples of anomalous diffusion in nature have been observed in biology in the cell nucleus, plasma membrane and cytoplasm.^[3]

Unlike typical diffusion, anomalous diffusion is described by a power law,^[4][5] ${\displaystyle \langle r^{2}(\tau )\rangle =K_{\alpha }\tau ^{\alpha }}$where ${\displaystyle K_{\alpha }}$ is the so-called generalized diffusion coefficient and ${\displaystyle \tau }$ is the elapsed time. In Brownian motion, α = 1. If α > 1, the process is superdiffusive. Superdiffusion can be the result of active cellular transport processes or due to jumps with a heavy-tail distribution. If α < 1, the particle undergoes subdiffusion. ^[6]

The role of anomalous diffusion has received attention within the literature to describe many physical scenarios, most prominently within crowded systems, for example protein diffusion within cells, or diffusion through porous media. Subdiffusion has been proposed as a measure of macromolecular crowding in the cytoplasm. It has been found that equations describing normal diffusion are not capable of characterizing some complex diffusion processes, for instance, diffusion process in inhomogeneous or heterogeneous medium, e.g. porous media. Fractional diffusion equations were introduced in order to characterize anomalous diffusion phenomena.

Recently, anomalous diffusion was found in several systems including ultra-cold atoms,^[7] scalar mixing in the interstellar medium, ^[8] telomeres in the nucleus of cells,^[9] ion channels in the plasma membrane,^[10] colloidal particle in the cytoplasm,^[11][12] moisture transport in cement-based materials,^[13] and worm-like micellar solutions.^[14] Anomalous diffusion was also found in other biological systems, including heartbeat intervals and in DNA sequences.^[15]

The daily fluctuations of climate variables such as temperature can be regarded as steps of a random walker or diffusion and have been found to be anomalous.^[16]

In 1926, using weather balloons, Lewis Fry Richardson demonstrated that the atmosphere exhibits super-diffusion.^[17] In a bounded system, the mixing length (which determines the scale of dominant mixing motions) is given by the Von Kármán constant according to the equation ${\displaystyle l_{m}={\kappa }z}$, where ${\displaystyle l_{m}}$ is the mixing length, ${\displaystyle {\kappa }}$ is the Von Kármán constant, and ${\displaystyle z}$ is the distance to the nearest boundary.^[18] Because the scale of motions in the atmosphere is not limited, as in rivers or the subsurface, a plume continues to experience larger mixing motions as it increases in size, which also increases its diffusivity, resulting in super-diffusion.^[19]

Types of anomalous diffusion[]

Of interest within the scientific community, when an anomalous-type diffusion process is discovered, the challenge is to understand the underlying mechanism which causes it. There are a number of frameworks which give rise to anomalous diffusion that are currently in vogue within the statistical physics community. These are long range correlations between the signals ^[20] continuous-time random walks (CTRW ^[21]) and fractional Brownian motion (fBm), and diffusion in disordered media.^[22][23]

Currently the most studied types of anomalous diffusion processes are those involving the following

• Generalizations of Brownian motion, such as the fractional Brownian motion and scaled Brownian motion
• Diffusion in fractals and percolation in porous media
• Continuous time random walks

These processes have growing interest in cell biophysics where the mechanism behind anomalous diffusion has direct physiological importance. Of particular interest, works by the groups of Eli Barkai, Maria Garcia Parajo, Joseph Klafter, Diego Krapf, and Ralf Metzler have shown that the motion of molecules in live cells often show a type of anomalous diffusion that breaks the ergodic hypothesis.^[6][24][25] This type of motion require novel formalisms for the underlying statistical physics because approaches using microcanonical ensemble and Wiener Khinchin theorem break down.

Hyper-ballistic diffusion[]

One important class of anomalous diffusion refers to the case when the scaling exponent of the MSD increases with value greater than 2. Such case is called hyper-ballistic diffusion and it has been observed in optical systems.^[26]

See also[]

• Lévy flight – random walk with heavy-tailed step lengths
• Random walk – Mathematical formalization of a path that consists of a succession of random steps
• Percolation – Filtration of fluids through porous materials
• Long term correlations^{[clarification needed]}
• long range dependencies
• Hurst exponent – A measure of the long-range dependence of a time series
• Detrended fluctuation analysis (DFA)
• Fractal – Self similar mathematical structures

References[]

• Weiss, Matthias; Elsner, Markus; Kartberg, Fredrik; Nilsson, Tommy (2004). "Anomalous Subdiffusion Is a Measure for Cytoplasmic Crowding in Living Cells". Biophysical Journal. 87 (5): 3518–3524. Bibcode:2004BpJ....87.3518W. doi:10.1529/biophysj.104.044263. PMC 1304817. PMID 15339818.
• Bouchaud, Jean-Philippe; Georges, Antoine (1990). "Anomalous diffusion in disordered media". Physics Reports. 195 (4–5): 127–293. Bibcode:1990PhR...195..127B. doi:10.1016/0370-1573(90)90099-N.
• von Kameke, A.; et al. (2010). "Propagation of a chemical wave front in a quasi-two-dimensional superdiffusive flow". Phys. Rev. E. 81 (6): 066211. Bibcode:2010PhRvE..81f6211V. doi:10.1103/physreve.81.066211. PMID 20866505. S2CID 23202701.
• Chen, Wen; Sun, HongGuang; Zhang, Xiaodi; Korosak, Dean (2010). "Anomalous diffusion modeling by fractal and fractional derivatives". Computers and Mathematics with Applications. 59 (5): 1754–1758. doi:10.1016/j.camwa.2009.08.020.
• Sun, HongGuang; Meerschaert, Mark M.; Zhang, Yong; Zhu, Jianting; Chen, Wen (2013). "A fractal Richards' equation to capture the non-Boltzmann scaling of water transport in unsaturated media". Advances in Water Resources. 52: 292–295. Bibcode:2013AdWR...52..292S. doi:10.1016/j.advwatres.2012.11.005. PMC 3686513. PMID 23794783.
• Metzler, Ralf; Jeon, Jae-Hyung; Cherstvy, Andrey G.; Barkai, Eli (2014). "Anomalous diffusion models and their properties: non-stationarity, non-ergodicity, and ageing at the centenary of single particle tracking". Phys. Chem. Chem. Phys. 16 (44): 24128–24164. Bibcode:2014PCCP...1624128M. doi:10.1039/c4cp03465a. ISSN 1463-9076. PMID 25297814.
• Krapf, Diego (2015), "Mechanisms Underlying Anomalous Diffusion in the Plasma Membrane", Lipid Domains, Current Topics in Membranes, 75, Elsevier, pp. 167–207, doi:10.1016/bs.ctm.2015.03.002, ISBN 9780128032954, PMID 26015283, retrieved 2018-08-13

External links[]

• Boltzmann's transformation, Parabolic law (animation)
• Anomalous interface shift kinetics (Computer simulations and Experiments)