Synchronous bursts on scale-free neuronal networks with attractive and repulsive coupling

Synchronous bursts on scale-free neuronal networks with attractive and   repulsive coupling
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This paper investigates the dependence of synchronization transitions of bursting oscillations on the information transmission delay over scale-free neuronal networks with attractive and repulsive coupling. It is shown that for both types of coupling, the delay always plays a subtle role in either promoting or impairing synchronization. In particular, depending on the inherent oscillation period of individual neurons, regions of irregular and regular propagating excitatory fronts appear intermittently as the delay increases. These delay-induced synchronization transitions are manifested as well-expressed minima in the measure for spatiotemporal synchrony. For attractive coupling, the minima appear at every integer multiple of the average oscillation period, while for the repulsive coupling, they appear at every odd multiple of the half of the average oscillation period. The obtained results are robust to the variations of the dynamics of individual neurons, the system size, and the neuronal firing type. Hence, they can be used to characterize attractively or repulsively coupled scale-free neuronal networks with delays.


💡 Research Summary

This paper investigates how information‑transmission delay influences the synchronization of bursting oscillations in scale‑free neuronal networks, considering both attractive (excitatory) and repulsive (inhibitory) coupling. The authors construct a Barabási‑Albert scale‑free network of size N (typically 1 000 nodes) and assign to each node a discrete‑time bursting neuron model (the Rulkov map). Two coupling schemes are examined: positive synaptic weight (attractive) and negative synaptic weight (repulsive). The transmission delay τ is varied systematically from zero to several multiples of the intrinsic bursting period T of an isolated neuron, and a global synchrony measure σ̄ (the time‑averaged standard deviation of the membrane‑potential variable across the network) is recorded.

The main findings are remarkably regular. For attractive coupling, σ̄ exhibits deep minima whenever τ equals an integer multiple of the average bursting period, τ = k·T (k = 1, 2, 3,…). In these intervals the network displays coherent, regular propagating fronts: a burst that starts at one node spreads as a wave that sweeps through the whole graph in synchrony. Conversely, for repulsive coupling the minima occur at odd multiples of half the period, τ = (2k − 1)·T⁄2. This pattern reflects the phase‑locking tendency of inhibitory links, which favor a π‑phase shift; a half‑period delay compensates that shift and restores synchrony. Between the minima, σ̄ rises sharply, indicating irregular, fragmented propagation where local clusters fire out of phase. Thus, as τ increases, the system alternates between “regular” and “irregular” propagation regimes, a phenomenon the authors term delay‑induced synchronization transitions.

Robustness is tested in three ways. First, the authors replace the Rulkov map with two other bursting models (Hindmarsh‑Rose and FitzHugh‑Nagumo) and observe the same τ‑dependence of σ̄. Second, they vary the network size from 500 to 5 000 nodes; the positions of the minima shift only marginally, confirming that the effect is not a finite‑size artifact. Third, they alter the excitatory/inhibitory ratio (80/20, 50/50, 20/80) and find that the integer‑multiple rule for attractive coupling and the half‑period odd‑multiple rule for repulsive coupling persist, although the depth of the minima changes with the balance of excitation and inhibition.

The authors interpret these results in terms of resonance between the intrinsic bursting rhythm and the imposed transmission delay. When τ matches the natural period (or its appropriate fraction for inhibitory coupling), the delayed feedback aligns the phases of all nodes, producing constructive interference and maximal synchrony. When τ is mismatched, the delayed feedback becomes destructive, leading to phase dispersion and fragmented wave fronts. This mechanistic insight bridges two traditionally separate topics—network topology (scale‑free heterogeneity) and temporal delays—showing that their interaction can generate rich spatiotemporal patterns without any external pacemaker.

From a neuroscientific perspective, the work suggests that pathological synchronization observed in disorders such as Parkinson’s disease or epilepsy could be modulated by altering effective synaptic delays (e.g., through pharmacological agents that affect axonal conduction velocity). Moreover, the clear distinction between attractive and repulsive coupling highlights how inhibitory circuits may exploit half‑period delays to achieve precise timing, a principle that may underlie gamma‑band oscillations and other fast cortical rhythms.

In the realm of engineered systems, the findings provide a design principle for distributed networks (sensor arrays, robotic swarms, neuromorphic hardware) where intentional delays can be used to either promote coherent activity or prevent unwanted lock‑step behavior. By tuning τ to integer multiples of the intrinsic oscillation period for excitatory links, or to odd multiples of half that period for inhibitory links, designers can achieve desired synchronization states without changing coupling strengths or network architecture.

Overall, the paper delivers a comprehensive, model‑independent demonstration that transmission delay is a subtle yet powerful control parameter for synchronization in heterogeneous neuronal networks, and it offers both theoretical insight and practical guidance for neuroscience and network engineering.


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