The synchrony phenomenon is widely observed in various systems, like nervous (e.g. the firing of the neurons), biological (e.g. synchronous flashing fireflies), social (e.g.the, the perception of social bonding) and etc. systems. A coupled oscillator system, a typical real non-equilibrium system, is an ideal and abstract model of interacting elements to model synchronisation. The Kuramoto model is one of the most profound and classical toy models of coupled phase oscillators. Although this model can successfully produce various synchrony phenomena, its phase transition analysis is limited to mean-field approximation, which is characterised by the order parameter. However, it is hard to define a single variable to represent the order for a real system where the Hamiltonian function is unknown, heterogeneity exists, and the states of each interacting component are available. To better understand the real-world synchronisation phenomenon without a well-defined order parameter, we apply the Eigen Microstate Method to revisit the globally coupled Kuramoto model, of which the calculation of mean-field approximation is valid. Therefore, after exploring the finite-size scaling near the onset of the phase transition, we can compare the scaling exponents of both methods.
I am also looking at the Kuramoto model on the networks with different coupling strengths between communities. This new setting will introduce the fruitful phase transition phenomenon: the explosive phase transition, asynchronisation with different communities.
The emergence of synchronisation through coupling dynamics creates orders. However, as an isolated system, how can the entropy, which describes the possible configurations, decrease?
The answer can be found in the information perspective, which implies that through interaction, mutual information or interdependency is created.