Publication record · 18.cifr/1995.vicsek.flocking-phase-transition
18.cifr/1995.vicsek.flocking-phase-transitionA simple model with a novel type of dynamics is introduced in order to investigate the emergence of self-ordered motion in systems of particles with biologically motivated interaction. In our model point particles with the same absolute velocity have a tendency to align their velocity with that of the neighbors. We show that this model results in a kinetic phase transition from no transport (zero average velocity) to finite net transport through spontaneous symmetry breaking of the rotational symmetry. The transition is continuous and the order parameter obeys scaling. This is in contrast to the usually observed first-order phase transitions in similar models.
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The universality class of the transition remains debated: Grégoire & Chaté (2004) showed it can be first-order for large systems, contradicting the original continuous-transition claim. Finite-size scaling analysis, 3-D extensions, heterogeneous speeds, and obstacles/boundaries are natural follow-ups. Analytical renormalization-group treatments of the broken continuous symmetry in the ordered phase (Toner & Tu theory) are an active research direction.