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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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. |
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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 |
Author_xml | – sequence: 1 givenname: Gabriel surname: Baglietto fullname: Baglietto, Gabriel organization: Instituto de Física de Líquidos y Sistemas Biológicos (UNLP-CONICET) IFLYSIB, 1900 La Plata, Argentina – sequence: 2 givenname: Federico surname: Vazquez fullname: Vazquez, Federico email: fede.vazmin@gmail.com organization: Instituto de Física de Líquidos y Sistemas Biológicos (UNLP-CONICET) IFLYSIB, 1900 La Plata, Argentina |
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CitedBy_id | crossref_primary_10_1103_PhysRevE_109_054609 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 |
Cites_doi | 10.1073/pnas.0711437105 10.1006/jtbi.1996.0053 10.1140/epjb/e2008-00391-6 10.1006/tpbi.2002.1597 10.1103/RevModPhys.85.1143 10.1103/RevModPhys.81.591 10.1016/j.physrep.2012.03.004 10.1103/PhysRevLett.108.238001 10.1103/PhysRevE.78.061127 10.1103/PhysRevE.77.046113 10.1126/science.1125142 10.1103/PhysRevE.80.050103 10.1103/PhysRevE.96.032313 10.1214/aop/1176996130 10.1016/j.physa.2006.07.036 10.1103/PhysRevA.45.1067 10.1103/PhysRevLett.105.168103 10.1103/PhysRevE.93.032318 10.1103/PhysRevE.95.052308 10.1103/PhysRevE.82.010103 10.1007/s10955-013-0827-4 10.1103/PhysRevE.73.046120 10.1103/PhysRevLett.109.098101 10.1103/PhysRevE.74.056108 10.1103/PhysRevLett.95.098101 10.1103/PhysRevLett.101.018701 10.1016/j.physrep.2014.10.001 10.1103/PhysRevLett.94.230601 10.1126/science.1210280 10.1103/PhysRevLett.100.108702 10.1103/PhysRevLett.96.188104 10.1103/PhysRevLett.75.1226 10.1103/PhysRevE.91.022117 10.1007/978-1-4614-6729-8_5 10.1103/PhysRevE.71.046102 10.1103/PhysRevLett.91.028701 10.1103/PhysRevLett.98.095702 10.1093/biomet/60.3.581 10.1103/PhysRevE.91.022103 10.1103/PhysRevE.53.R3009 10.1088/1742-5468/2012/10/p10027 |
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