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Updated: Oct 16, 2025

The HoneyComb Paradigm for Research on Collective Human Behavior
Published on: January 19, 2019
Noisy multistate voter model for flocking in finite dimensions.
Ernesto S Loscar1, Gabriel Baglietto1, Federico Vazquez2
1Instituto de Física de Líquidos y Sistemas Biológicos (IFLYSIB), UNLP, CCT La Plata-CONICET, Calle 59 no. 789, B1900BTE La Plata, Argentina.
Collective behavior in self-propelled particles is studied. Particle motion enables global order, overcoming noise, unlike static systems where noise causes disorder. This reveals a key order-disorder phase transition.
Area of Science:
- Statistical physics
- Complex systems
- Collective behavior
Background:
- Self-propelled particles exhibit complex collective behaviors.
- Voter models describe opinion dynamics and alignment.
- Noise and particle motion significantly influence system order.
Purpose of the Study:
- To investigate the impact of particle motion and noise on collective alignment.
- To analyze the order-disorder phase transition in a model of self-propelled particles.
- To determine how particle speed and noise amplitude affect global order.
Main Methods:
- Simulating a model of self-propelled particles with pairwise copying interactions and noise.
- Analyzing the system's steady states in static (v=0) and dynamic (v>0) scenarios.
- Investigating the finite-size scaling of the transition noise in 1D and 2D lattices.
Main Results:
- Static particles (v=0) exhibit complete disorder for any positive noise (η>0) in the thermodynamic limit.
- Full order is achieved for static particles only in the absence of noise (η=0).
- Moving particles (v>0) enable an ordered phase, with an order-disorder phase transition at a critical noise amplitude (η_c > 0) proportional to particle speed (v).
Conclusions:
- Particle motion is crucial for sustaining global order in systems with voter-like interactions.
- The emergence of an ordered phase is a direct consequence of particle dynamics.
- The study provides insights into phase transitions driven by motion in interacting particle systems.
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