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
Summary
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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