Giant increase of diffusion by small rise of friction

Fuente: arXiv
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Auteurs principaux: Marchenko, I. G., Marchenko, I. I., Aksenova, V., Łuczka, J., Spiechowicz, J.
Format: Preprint
Publié: 2024
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author Marchenko, I. G.
Marchenko, I. I.
Aksenova, V.
Łuczka, J.
Spiechowicz, J.
author_facet Marchenko, I. G.
Marchenko, I. I.
Aksenova, V.
Łuczka, J.
Spiechowicz, J.
contents Diffusion coefficient usually decreases when friction increases. We analyze the opposite behavior in the paradigmatic system consisting of an inertial Brownian particle moving in a symmetric spatially periodic potential and driven by an unbiased time periodic force. For tailored parameter set in strong dissipation regime the particle spreading can be giantly amplified: if the friction is twice as large then the diffusion grows up to five orders of magnitude. The mechanism lying behind this effect is related to bifurcation of periodic orbits oscillating around the potential maximum and their symmetric displacement towards the adjacent potential minima when the friction coefficient increases. On the other hand, in the weak dissipation regime, where the increase of diffusion vs friction is also observed, the effect is induced by a non-monotonic change of population of the running orbits. However, in this regime the enhancement of diffusion is much smaller.
format Preprint
id arxiv_https___arxiv_org_abs_2407_18592
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Giant increase of diffusion by small rise of friction
Marchenko, I. G.
Marchenko, I. I.
Aksenova, V.
Łuczka, J.
Spiechowicz, J.
Statistical Mechanics
Mesoscale and Nanoscale Physics
Soft Condensed Matter
Diffusion coefficient usually decreases when friction increases. We analyze the opposite behavior in the paradigmatic system consisting of an inertial Brownian particle moving in a symmetric spatially periodic potential and driven by an unbiased time periodic force. For tailored parameter set in strong dissipation regime the particle spreading can be giantly amplified: if the friction is twice as large then the diffusion grows up to five orders of magnitude. The mechanism lying behind this effect is related to bifurcation of periodic orbits oscillating around the potential maximum and their symmetric displacement towards the adjacent potential minima when the friction coefficient increases. On the other hand, in the weak dissipation regime, where the increase of diffusion vs friction is also observed, the effect is induced by a non-monotonic change of population of the running orbits. However, in this regime the enhancement of diffusion is much smaller.
title Giant increase of diffusion by small rise of friction
topic Statistical Mechanics
Mesoscale and Nanoscale Physics
Soft Condensed Matter
url https://arxiv.org/abs/2407.18592