2018
DOI: 10.1103/physreve.98.062610
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Non-Gaussian noise without memory in active matter

Abstract: Modeling the dynamics of an individual active particle invariably involves an isotropic noisy self-propulsion component, in the form of run-and-tumble motion or variations around it. This nonequilibrium source of noise is neither white-there is persistence-nor Gaussian. While emerging collective behavior in active matter has hitherto been attributed to the persistent ingredient, we focus on the non-Gaussian ingredient of self-propulsion. We show that by itself, that is without invoking any memory effect, it is… Show more

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Cited by 25 publications
(21 citation statements)
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“…As a result, the commonly used active Brownian particle model emerges in a way that allows us to disentangle chemical aspects of entropy production from coarse-grained ones. We thus have formalised the concept of active force [19,20,[87][88][89] and work [70,[83][84][85], previously used in theoretical models, from a thermodynamic perspective. Moreover, we have shown how the work that can be extracted on a macroscopic scale is related to this active work.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…As a result, the commonly used active Brownian particle model emerges in a way that allows us to disentangle chemical aspects of entropy production from coarse-grained ones. We thus have formalised the concept of active force [19,20,[87][88][89] and work [70,[83][84][85], previously used in theoretical models, from a thermodynamic perspective. Moreover, we have shown how the work that can be extracted on a macroscopic scale is related to this active work.…”
Section: Discussionmentioning
confidence: 99%
“…that is performed by an effective active force apparently providing propulsion in the direction of n i [70,[83][84][85]. Such an active force is commonly used ad hoc in theoretical models for active particles that discard the details of the self-propulsion mechanism [19,20,[86][87][88][89]. It can be determined phenomenologically as the force required to stall an active particle with persistent director n. Experimentally, the active force can also be measured for a single free active particle that undergoes rotational and translational diffusion.…”
Section: A Setting and Energeticsmentioning
confidence: 99%
“…Subsequent theoretical calculations for the τ → ∞ limit posited that a departure from equilibrium efficiencies requires noise not just with non-Gaussian statistics but also with memory, a feature typical of active baths due to the persistent motion of the particles 15 . In fact, when the bath noise is non-Gaussian and white, an effective temperature T eff defined through the variance of ρ ( x ) is thought to act like a bona fide temperature 15 , 16 and engines operating between such baths are expected to perform like thermal ones in the quasistatic limit. Whether this similarity persists when τ is reduced and irreversibility begins to set in is not known and is worth exploring since real heat engines never operate in the quasistatic limit as here their power P → 0.…”
Section: Introductionmentioning
confidence: 99%
“…Such models violate Einstein's locality principle in physics, and the nature of instantaneous jumps make it impractical, if not impossible, to deal with in interacting systems. The resolution of instantaneous jumps in overdamped Langevin dynamics (of ABP, RTP, AOUP) was discussed by Fodor et al [35], while active matter models based on Lévy flights were proposed in Cairoli and Lee [36]. On the other hand, Lévy walks involve particles that change direction at random times, but travel in each direction with bounded (e.g., constant) velocity for a persistent time sampled from a heavy-tailed distribution.…”
Section: Introductionmentioning
confidence: 99%