{ "id": "2012.03142", "version": "v1", "published": "2020-12-05T23:25:52.000Z", "updated": "2020-12-05T23:25:52.000Z", "title": "Probability density of fractional Brownian motion and the fractional Langevin equation with absorbing walls", "authors": [ "Thomas Vojta", "Alex Warhover" ], "comment": "26 pages, 11 figures included", "categories": [ "cond-mat.stat-mech", "physics.bio-ph" ], "abstract": "Fractional Brownian motion and the fractional Langevin equation are models of anomalous diffusion processes characterized by long-range power-law correlations in time. We employ large-scale computer simulations to study these models in two geometries, (i) the spreading of particles on a semi-infinite domain with an absorbing wall at one end and (ii) the stationary state on a finite interval with absorbing boundaries at both ends and a source in the center. For both stochastic processes and both geometries, we find that the probability density close to an absorbing wall behaves as $P(x) \\sim x^\\kappa$ with the distance $x$ from the wall in the long-time limit. In the case of fractional Brownian motion, $\\kappa$ varies with the anomalous diffusion exponent $\\alpha$ as $\\kappa=2/\\alpha -1$, as was conjectured previously. The probability density of the fractional Langevin equation can be mapped onto that of fractional Brownian motion driven by the same noise by replacing $\\alpha$ with $2-\\alpha$. We also contrast the behavior near absorbing walls with the strong accumulation and depletion effects recently observed for fractional Brownian motion and the fractional Langevin equation near reflecting boundaries.", "revisions": [ { "version": "v1", "updated": "2020-12-05T23:25:52.000Z" } ], "analyses": { "keywords": [ "fractional langevin equation", "absorbing wall", "employ large-scale computer simulations", "fractional brownian motion driven", "long-range power-law correlations" ], "note": { "typesetting": "TeX", "pages": 26, "language": "en", "license": "arXiv", "status": "editable" } } }