Bifurcation sequence near SL/APC region leading to chaos
Characterize the sequence of bifurcations near the boundary of bistability between slalom and active-particle-preceding circular motion as the self-propulsion parameter f2 decreases, including transitions from slalom to circular slalom, to Lissajous-like trajectories, and finally to chaotic motion, by determining the underlying bifurcation mechanisms and parameter thresholds in the proposed model.
References
As the parameter f_2 decreased, the SL motion changed to the slalom motion along a circle as shown in Fig.~\ref{fig6}(d), and then to the circular slalom motion along a curve like the Lissajous figure as shown in Fig.~\ref{fig6}(c). With a further decrease in f_2, the chaotic motion was observed as shown in Fig.~\ref{fig6}(a,b). The detailed analyses of these series of bifurcation structure may be interesting from the viewpoint of dynamical systems, though we leave them as future study.
An open question here would be the characterization of `chaotic'' motion, perhaps at large P
eclet numbers, as seen in experiments~\citep{Hokmabad2021}, 3D simulations of unbounded isotropic active particles~\citep{Hu2022} and 2D simulations ofactive discs'~\citep{Li2022}.