2021
DOI: 10.1007/s11467-020-1022-0
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Non-Gaussian normal diffusion in low dimensional systems

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Cited by 9 publications
(3 citation statements)
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“…[13][14][15] In liquids, however, a general theoretical description of the nanoparticle transport is still lacking, 16,17 despite the fact that considerable progress has been achieved over the past decades. [18][19][20] A particle moving in a fluid experiences a drag force, which governs the particle transport. 21 According to the Einstein relationship, the diffusion coefficient of a particle in a fluid is proportional to the drag force coefficient.…”
Section: Introductionmentioning
confidence: 99%
“…[13][14][15] In liquids, however, a general theoretical description of the nanoparticle transport is still lacking, 16,17 despite the fact that considerable progress has been achieved over the past decades. [18][19][20] A particle moving in a fluid experiences a drag force, which governs the particle transport. 21 According to the Einstein relationship, the diffusion coefficient of a particle in a fluid is proportional to the drag force coefficient.…”
Section: Introductionmentioning
confidence: 99%
“…Microscopic models have also been proposed, where they have rigorously, mathematically studied interesting physical scenarios such as the study of diffusion of ellipsoidal particles, active particles, diffusion of colloidal particles in fluctuating corrugated channels, and Brownian motion in arrays of planar convective rolls [ 23 ]; non-Gaussian diffusion in static disordered media via a quenched trap model, where the diffusivity is spatially correlated [ 24 ]; and the Hitchhiker model [ 25 ].…”
Section: Introductionmentioning
confidence: 99%
“…Einstein’s theory of Brownian diffusion predicts that the displacement of a group of particles follows a Gaussian distribution, with the variance increasing linearly with time t. However, in materials close to the glass and jamming transitions, exponential decay of P ( x , t ) was observed. Interestingly, the exponential decay of P ( x , t ) was found in a wide variety of scenarios: desorption-mediated diffusion on solid–liquid interfaces, Brownian motion in polymer solutions, , cellular environments, active systems, heterogeneously crowded and confined media, and even the fluctuations of price–time series in the stock market . Well-designed theories and simulations have been put forward to rationalize the appearance of the exponential tail, such as the “diffusing diffusivity” model, superstatistical approaches, the quenched trap model, and the hitchhiker-type model. More recently, the large deviation theory was applied to a continuous-time random walk (CTRW) model to describe the exponential decay of P ( x , t ). A CTRW process comprises intermittent switching between random immobile trapping periods and jumping steps. The trapping duration dictates the random fluctuations in the number of displacement steps at a given t , which leads to an exponential decay of P ( x , t ). ,, …”
mentioning
confidence: 99%