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 inJournal of statistical mechanics Vol. 2018; no. 3; pp. 33403 - 33419
Main Authors Baglietto, Gabriel, Vazquez, Federico
Format Journal Article
LanguageEnglish
Published IOP Publishing and SISSA 12.03.2018
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ISSN1742-5468
1742-5468
DOI10.1088/1742-5468/aaac3e

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Abstract 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.
AbstractList 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.
Author Vazquez, Federico
Baglietto, Gabriel
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crossref_primary_10_1103_PhysRevE_100_042301
crossref_primary_10_1103_PhysRevE_104_034111
crossref_primary_10_1103_PhysRevE_103_032406
crossref_primary_10_1038_s41567_020_0787_y
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Snippet 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...
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