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Published on: November 16, 2013
Biswas-Chatterjee-Sen Model Defined on Solomon Networks in (1 ≤ D ≤ 6)-Dimensional Lattices
Gessineide Sousa Oliveira1, David Santana Alencar1, Tayroni Alencar Alves1
1Dietrich Stauffer Computational Physics Lab, Departamento de Física, Universidade Federal do Piauí, Teresina 64049-550, PI, Brazil.
This study investigates the Biswas-Chatterjee-Sen model on hypercubic Solomon networks. Monte Carlo simulations reveal a second-order phase transition across dimensions, with critical exponents varying with network dimensionality.
Area of Science:
- Statistical Physics
- Complex Networks
- Dynamical Systems
Background:
- The Biswas-Chatterjee-Sen model is a discrete dynamical system.
- Understanding phase transitions in complex networks is crucial.
- Hypercubic Solomon networks provide a framework for studying network dynamics.
Purpose of the Study:
- To analyze the phase transition of the discrete Biswas-Chatterjee-Sen model on D-dimensional hypercubic Solomon networks.
- To determine the critical behavior and critical exponents for varying dimensions (1≤D≤6).
- To investigate the influence of external noise probability on the system's dynamics.
Main Methods:
- Extensive Monte Carlo simulations were employed.
- Thermodynamic-like variables were computed as a function of external noise probability.
- Finite-size scaling theory was applied to analyze the phase transition in the thermodynamic limit.
Main Results:
- The model exhibits a second-order phase transition for all investigated dimensions.
- The system appears to lack an upper critical dimension as critical exponents change with D.
- Critical exponent ratios and critical noise probability were determined, achieving the scaling regime.
Conclusions:
- The Biswas-Chatterjee-Sen model on hypercubic Solomon networks demonstrates complex phase transition behavior.
- The dimensionality of the network significantly influences the critical exponents, deviating from mean-field predictions.
- Further research on higher dimensions is limited by computational resources but the scaling regime was established.
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