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. 2015 Jun 19;6:7470. doi: 10.1038/ncomms8470

Figure 4. Collective-dynamics simulations.

Figure 4

(a) The numerical phase diagram of the confined population is composed of three regions: isotropic gas (low φ0, small b), swarm coexisting with a gaseous phase (intermediate φ0 and b) and vortex state (high φ0 and b). Rc=0.5 mm. (b) Snapshot of a vortex state. Numerical simulation for φ0=0.1 and b=5a. (c) Snapshot of a swarm. Numerical simulation for φ0=4.5 × 10−2 and b=2a. (d) Variation of the density correlation length as a function of Rc. Above Rc=1 mm, ξ plateaus and a vortex is reached (φ0=3 × 10−2, b=3a). (e) Four numerical snapshots of rollers interacting via: alignment interactions only (A), alignment interactions and repulsive torques (A+B, where the magnitude of B is five times the experimental value), alignment and excluded volume interactions (A+b, where the repulsion distance is b=5a), alignment and the C-term in equation 3 (A+C). Polarized vortices emerge solely when repulsive couplings exist (A+B and A+b).