Synchronization of globally coupled two-state stochastic oscillators with a state dependent refractory period
arXiv:1206.1664 · doi:10.1103/PhysRevE.86.011131
Abstract
We present a model of identical coupled two-state stochastic units each of which in isolation is governed by a fixed refractory period. The nonlinear coupling between units directly affects the refractory period, which now depends on the global state of the system and can therefore itself become time dependent. At weak coupling the array settles into a quiescent stationary state. Increasing coupling strength leads to a saddle node bifurcation, beyond which the quiescent state coexists with a stable limit cycle of nonlinear coherent oscillations. We explicitly determine the critical coupling constant for this transition.
References in corpus (6)
- Universal emission intermittency in quantum dots, nanorods, and nanowires
- Thermodynamic limit of the first-order phase transition in the Kuramoto model
- Time delay in the Kuramoto model with bimodal frequency distribution
- Critical behavior and synchronization of discrete stochastic phase coupled oscillators
- Continuous and discontinuous phase transitions and partial synchronization in stochastic three-state oscillators
- Collective oscillations of excitable elements: order parameters, bistability and the role of stochasticity
Cited by in corpus (5)
- Arrays of stochastic oscillators: Nonlocal coupling, clustering, and wave formation
- Synchronization of coupled noisy oscillators: Coarse-graining from continuous to discrete phases
- Synchronization and phase redistribution in self-replicating populations of coupled oscillators and excitable elements
- Tristable and multiple bistable activity in complex random binary networks of two-state units
- Damped oscillations of the probability of random events followed by absolute refractory period: exact analytical results