# Tracer diffusion in active suspensions

## TL;DR

This paper investigates how active Brownian particles influence the diffusion of a probe particle, revealing a nonmonotonic transition in diffusivity enhancement driven by swimmer activity levels.

## Contribution

It introduces a theoretical framework for understanding probe diffusion in active suspensions, highlighting the scaling regimes and transition behaviors based on swimmer activity.

## Key findings

- Active diffusivity scales as Pe_s^2 for weak swimming.
- Active diffusivity scales as Pe_s for strong swimming.
- Transition between regimes is nonmonotonic.

## Abstract

We study the diffusion of a Brownian probe particle of size $R$ in a dilute dispersion of active Brownian particles (ABPs) of size $a$, characteristic swim speed $U_0$, reorientation time $\tau_R$, and mechanical energy $k_s T_s = \zeta_a U_0^2 \tau_R /6$, where $\zeta_a$ is the Stokes drag coefficient of a swimmer. The probe has a thermal diffusivity $D_P = k_B T/\zeta_P$, where $k_B T$ is the thermal energy of the solvent and $\zeta_P$ is the Stokes drag coefficient for the probe. When the swimmers are inactive, collisions between the probe and the swimmers sterically hinder the probe's diffusive motion. In competition with this steric hindrance is an enhancement driven by the activity of the swimmers. The strength of swimming relative to thermal diffusion is set by $Pe_s = U_0 a /D_P$. The active contribution to the diffusivity scales as $Pe_s^2$ for weak swimming and $Pe_s$ for strong swimming, but the transition between these two regimes is nonmonotonic. When fluctuations in the probe motion decay on the time scale $\tau_R$, the active diffusivity scales as $k_s T_s /\zeta_P$: the probe moves as if it were immersed in a solvent with energy $k_s T_s$ rather than $k_B T$.