Conservative, Dissipative and Super-diffusive Behavior of a Particle Propelled in a Regular Flow

TL;DR

This paper investigates a model of self-propelled particles in vortices, revealing how super-diffusive Le9vy walk-like behavior arises from trajectory sticking and long-term dissipative effects.

Contribution

It provides a combined analytical and numerical study showing how super-diffusion and dissipative behaviors emerge in a reversible, non-volume-preserving chaotic system.

Findings

Super-diffusion results from trajectory sticking to elliptic islands.

Long-term dissipation occurs due to coexistence of islands and stable periodic orbits.

The model offers a new perspective on Le9vy walks in chaotic systems.

Abstract

A recent model of Ariel et al. [1] for explaining the observation of L\'evy walks in swarming bacteria suggests that self-propelled, elongated particles in a periodic array of regular vortices perform a super-diffusion that is consistent with L\'evy walks. The equations of motion, which are reversible in time but not volume preserving, demonstrate a new route to L'evy walking in chaotic systems. Here, the dynamics of the model is studied both analytically and numerically. It is shown that the apparent super-diffusion is due to "sticking" of trajectories to elliptic islands, regions of quasi-periodic orbits reminiscent of those seen in conservative systems. However, for certain parameter values, these islands coexist with asymptotically stable periodic trajectories, causing dissipative behavior on very long time scales.