Abstract

A fundamental question in computational neuroscience is how to connect a network of spiking neurons to produce desired macroscopic or mean field dynamics. One possible approach is through the Neural Engineering Framework (NEF). The NEF approach requires quantities called decoders which are solved through an optimization problem requiring large matrix inversion. Here, we show how a decoder can be obtained analytically for type I and certain type II firing rates as a function of the heterogeneity of its associated neuron. These decoders generate approximants for functions that converge to the desired function in mean-squared error like 1/N, where N is the number of neurons in the network. We refer to these decoders as scale-invariant decoders due to their structure. These decoders generate weights for a network of neurons through the NEF formula for weights. These weights force the spiking network to have arbitrary and prescribed mean field dynamics. The weights generated with scale-invariant decoders all lie on low dimensional hypersurfaces asymptotically. We demonstrate the applicability of these scale-invariant decoders and weight surfaces by constructing networks of spiking theta neurons that replicate the dynamics of various well known dynamical systems such as the neural integrator, Van der Pol system and the Lorenz system. As these decoders are analytically determined and non-unique, the weights are also analytically determined and non-unique. We discuss the implications for measured weights of neuronal networks.

Highlights

  • There are many spiking models that exist in the literature that can be fit to reproduce the membrane potential and the firing rates of real neurons

  • If we allow α and β to be drawn from a random distribution, we can generate a network of neurons with firing rates f where αi, βi are drawn from some specified probability distribution ρα,β (α, β)

  • To simulate networks with arbitrary dynamics, we can use the decoders derived in the previous sections along with neurons that correspond to the appropriate firing rates (Eliasmith and Anderson, 2004)

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Summary

Introduction

There are many spiking models that exist in the literature that can be fit to reproduce the membrane potential and the firing rates of real neurons. Examples include the leaky integrate and fire neuron, the Izhikevich model (Izhikevich, 2003, 2007), the theta model (Ermentrout and Kopell, 1986), the quartic integrate and fire model (Touboul, 2008) and the adaptive exponential integrate and fire model (Brette and Gerstner, 2005; Naud et al, 2008) When these models are coupled together to form networks, one can predict the the macroscopic or mean field behavior of a network of Obtaining Prescribed Mean-Field Dynamics these neurons via a suitably derived mean field system (Nicola and Campbell, 2013a,b; Nesse et al, 2008). The NEF has been used to develop a wide variety of models, including the most behaviorally sophisticated spiking neural model to date (Eliasmith et al, 2012) as well as more specialized models of path integration (Conklin and Eliasmith, 2005), working memory (Singh and Eliasmith, 2006), visual attention (Bobier et al, 2014), motor control (DeWolf and Eliasmith, 2011), various cognitive functions (Bekolay et al, 2014; Rasmussen and Eliasmith, 2014), and many others

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