Fig. 5: Effects of time-varying interactions and lateral forces in swarmalators. | Nature Communications

Fig. 5: Effects of time-varying interactions and lateral forces in swarmalators.

From: Tunable colloidal swarmalators with hydrodynamic coupling

Fig. 5

a The mean fraction of swarmalators in clusters 〈fc〉 relaxes slower than the mean synchronization 〈σ〉 after a switch in Γ (the light colored areas show the SEM over multiple runs). We selected Γ = −05 and Γ = 0.2 here, because these values result in the same swarmalator motility (see Fig. S11; SI section 6). b Switching back and forth between two values of Γ results in a loop in the 〈fc〉–〈σ〉 space, because the system visits different states depending on the direction of the switching. 〈σ〉 and 〈fc〉 are averaged over multiple runs. c State loop in the 〈fc〉–〈σ〉 space in simulations, for slow switching (every 400δt) of Γ (gray, as in (b)) as well as for fast switching (every 200δt) from different initial Γ (purple and orange). 〈σ〉 and 〈fc〉 are averaged over 50 runs. d Illustration of the state loop with two smaller loops (purple and orange) that are a result of faster switching in Γ from different initial values of Γ (see inset). e Heat map of the averaged normal displacement \({\langle {d}_{\perp,ij}\rangle }_{ij}\) against the synchronization σij and reference point distance \(\left\vert {{{{\bf{q}}}}}_{ij}\right\vert\) between neighboring swarmalators in experiment. f The normal (perpendicular) displacement d,ij is defined as the component of the displacement di orthogonal to the direction to the neighboring reference point qij, multiplied by the sign of the angular velocity of i. g Snapshots of a rotating swarmalator cluster in simulations at different times (colors yellow to green to blue). h Mean and standard deviation of the angular velocity ω of a rotating cluster as a function of the number N of swarmalators in the system and the coupling parameter Γ in simulations In (g, h), the swarmalators were initialized on a hexagonal grid with a separation of 8 μm, the system was allowed to relax for 3000δt, and the data was collected and averaged over 30,000δt. In (a, b, c), the initial density is around 0.003 μm−2. Source data are provided as a Source data file.

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