Abstract

Firing-rate models provide an attractive approach for studying large neural networks because they can be simulated rapidly and are amenable to mathematical analysis. Traditional firing-rate models assume a simple form in which the dynamics are governed by a single time constant. These models fail to replicate certain dynamic features of populations of spiking neurons, especially those involving synchronization. We present a complex-valued firing-rate model derived from an eigenfunction expansion of the Fokker-Planck equation and apply it to the linear, quadratic and exponential integrate-and-fire models. Despite being almost as simple as a traditional firing-rate description, this model can reproduce firing-rate dynamics due to partial synchronization of the action potentials in a spiking model, and it successfully predicts the transition to spike synchronization in networks of coupled excitatory and inhibitory neurons.

Highlights

  • Descriptions of neuronal spiking in terms of firing rates are widely used for both data analysis and modeling

  • Neuronal responses are often characterized by the rate at which action potentials are generated rather than by the timing of individual spikes

  • By expanding the range of dynamic phenomena that can be described by simple firing-rate equations, this model should be useful in guiding intuition about and understanding of neural circuit function

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Summary

Introduction

Descriptions of neuronal spiking in terms of firing rates are widely used for both data analysis and modeling. In much the same spirit, firing-rate models are useful because they provide a simpler description of neural dynamics than a large network of spiking model neurons. At best, an approximation of spiking activity, they are often a sufficient description to gain insight into how neural circuits operate. Toward these approaches, it is important to develop firing-rate models that capture as much of the dynamics of spiking networks as possible. The resulting models involve a compromise between accuracy and simplicity Such models describe firing-rate dynamics as fluctuations around a steady-state firing rate r?(x). Given a constant input x, after a sufficiently long time, the firing rate will be given by r?(x)

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