两个耦合神经元

C. Pinto, I. Labouriau
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引用次数: 2

摘要

我们回顾了两个耦合神经元系统的动力学行为。我们考虑对称和非对称线性耦合。每个神经元的内部动力学由空间箝位霍奇金-赫胥黎方程建模。我们从对称的情况开始。文献中的结果表明,如果耦合足够强,两个神经元在任何时候都表现出相同的行为。它们可能周期性地尖峰或处于静止状态。我们将这些状态定义为完全同步。当耦合强度减小到很小的正值时,几乎完全保持同步。当我们接近负的耦合值时,两个神经元仍然同步,但以一种不同的方式,它们周期性地尖峰,彼此之间有半周期的相移。当我们趋向更低的负值时,系统变得完全不稳定。两个神经元同步的周期性状态也被定义为1:1锁相模式。将非对称耦合系统作为对称情况下的扰动来研究。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Two Coupled Neurons
We review the dynamical behaviour of a system of two coupled neurons. We consider symmetric and asymmetric linear coupling. The internal dynamics of each neuron is modeled by the space-clamped Hodgkin-Huxley equations. We start with the symmetric case. Results in the literature show that for strong enough coupling the two neurons show the same behaviour at all times. They may be periodically spiking or at rest. We define these states as perfect synchrony. When decreasing the coupling strength to small positive values almost perfect synchronization is retained. As we move towards negative values of the coupling the two neurons still synchronize but in a different way, they spike periodically with half-period phase shift from each other. As we go towards lower negative values, the system becomes totally unstable. Periodic states where the two neurons synchronize are also defined as 1:1 phase locked modes. The asymmetric coupled system is studied as a perturbation from the symmetric case.
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