Flocking dynamics with voter-like interactions
We study the collective motion of a large set of self-propelled particles subject to voter-like interactions. Each particle moves on a 2D space at a constant speed in a direction that is randomly assigned initially. Then, at every step of the dynamics, each particle adopts the direction of motion of...
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Published in | Journal of statistical mechanics Vol. 2018; no. 3; pp. 33403 - 33419 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
IOP Publishing and SISSA
12.03.2018
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Online Access | Get full text |
ISSN | 1742-5468 1742-5468 |
DOI | 10.1088/1742-5468/aaac3e |
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Summary: | We study the collective motion of a large set of self-propelled particles subject to voter-like interactions. Each particle moves on a 2D space at a constant speed in a direction that is randomly assigned initially. Then, at every step of the dynamics, each particle adopts the direction of motion of a randomly chosen neighboring particle. We investigate the time evolution of the global alignment of particles measured by the order parameter , until complete order φ=1.0 is reached (polar consensus). We find that increases as t1/2 for short times and approaches 1.0 exponentially fast for longer times. Also, the mean time to consensus τ varies non-monotonically with the density of particles ρ, reaching a minimum at some intermediate density ρmin. At ρmin, the mean consensus time scales with the system size N as τmin∼N0.765, and thus the consensus is faster than in the case of all-to-all interactions (large ρ) where τ=2N. We show that the fast consensus, also observed at intermediate and high densities, is a consequence of the segregation of the system into clusters of equally-oriented particles which breaks the balance of transitions between directional states in well mixed systems. |
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Bibliography: | JSTAT_023P_1117 |
ISSN: | 1742-5468 1742-5468 |
DOI: | 10.1088/1742-5468/aaac3e |