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Stationary distribution of the quorum-sensing active particle (QSAP) model

Determine the stationary probability distribution of the quorum-sensing active particle system consisting of N one-dimensional particles in an asymmetric quartic potential U with metastable states at positions a and c, evolving under overdamped Langevin dynamics with thermal noise at inverse temperature β and an interaction kernel η^i(X_t) that assigns an active run-and-tumble velocity of magnitude v0 governed by a telegraph process with rate λ when particle i has no neighbor within cutoff distance ℓ, and otherwise suppresses activity.

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Background

To design minimally dissipative control protocols for switching a QSAP system between metastable wells, the authors require source and target distributions. Because the stationary distribution of the active, interacting system under the specified run-and-tumble quorum-sensing rule is unknown, they approximate it using Gaussian expansions of the equilibrium (activity-free) distribution near the well centers.

A precise characterization of the stationary distribution would enable more accurate benchmarking of control protocols and tighter thermodynamic bounds for the active interacting particle system.

References

Since the stationary distribution of the QSAP system is not known, we define the source and target distributions to be the Gaussian expansion of the activity-free equilibrium distribution near the well centers

Universal energy-speed-accuracy trade-offs in driven nonequilibrium systems (2402.17931 - Klinger et al., 27 Feb 2024) in Subsection “Applications to multimodal distributions and interacting particle systems,” paragraph “Scalable control of active interacting particles”; see also Appendix “QSAP Dynamics”