Mean Field Theory Based on the Spike Time Response Curve for Synchronization Within and Between Two Alternating Populations of Neural Oscillators with Delays.

ArXiv Pub Date : 2026-10-07
Ananth Vedururu Srinivas, Carmen C Canavier
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Abstract

In order to study oscillators coupled by pulses emitted at discrete times, it is generally assumed that the effect of each pulse is an instantaneous phase shift, with a possible conduction delay between emission and receipt. However, we are interested in neural oscillators in which each pulse (action potential) activates a biexponential synapse, and at high frequencies, the duration of the synaptic conductance may be greater than the network period. Therefore, the effect of received pulses can summate over the course of several cycles. To overcome this limitation, we previously defined a mean field approach for a single synchronous population. Here, we extend it to two alternating synchronous populations by assuming a perturbation of a single oscillator from one of the synchronous populations which is represented by a single self-connected neural oscillator. The train of delayed biexponential synapses emitted by each oscillator is divided into a tonic and a phasic component. Because of the continuous rather than pulsatile nature of the input, we had to drop the concept of oscillator phase and derive self-consistent criteria for the existence and stability of an alternating firing pattern between two synchronous populations based solely on the perturbation of time intervals from their steady state values. Simulations showed that for high frequency oscillations as defined above, the mean field approach predicts the existence and stability of phase-locking between two synchronous populations better than the instantaneous phase shift approach. This approach may generalize to other forms of coupling amongst non-neural oscillators.

基于脉冲时间响应曲线的平均场理论在两个有延迟的神经振子交替种群内和之间的同步。
为了研究由离散时间发射的脉冲耦合的振子,通常假设每个脉冲的影响是瞬时相移,在发射和接收之间可能存在传导延迟。然而,我们对每个脉冲(动作电位)激活双指数突触的神经振荡器感兴趣,并且在高频率下,突触传导的持续时间可能大于网络周期。因此,接收到的脉冲效应可以在几个周期的过程中叠加。为了克服这一限制,我们之前为单个同步种群定义了平均场方法。在这里,我们将其扩展到两个交替的同步种群,通过假设其中一个同步种群的单个振荡器的扰动,该种群由单个自连接神经振荡器表示。由每个振荡器发出的延迟双指数突触序列分为强音和相位分量。由于输入是连续的而不是脉动的性质,我们不得不放弃振荡器相位的概念,仅仅基于两个同步种群的稳态值对时间间隔的扰动,推导出两个同步种群之间交替发射模式存在和稳定性的自洽准则。仿真结果表明,对于上述高频振荡,平均场法比瞬时移相法更好地预测了两个同步种群之间锁相的存在性和稳定性。这种方法可以推广到非神经振荡器之间的其他形式的耦合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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