Abstract

Point neuron models with a Heaviside firing rate function can be ill-posed. That is, the initial-condition-to-solution map might become discontinuous in finite time. If a Lipschitz continuous but steep firing rate function is employed, then standard ODE theory implies that such models are well-posed and can thus, approximately, be solved with finite precision arithmetic. We investigate whether the solution of this well-posed model converges to a solution of the ill-posed limit problem as the steepness parameter of the firing rate function tends to infinity. Our argument employs the Arzelà–Ascoli theorem and also yields the existence of a solution of the limit problem. However, we only obtain convergence of a subsequence of the regularized solutions. This is consistent with the fact that models with a Heaviside firing rate function can have several solutions, as we show. Our analysis assumes that the vector-valued limit function v, provided by the Arzelà–Ascoli theorem, is threshold simple: That is, the set containing the times when one or more of the component functions of v equal the threshold value for firing, has zero Lebesgue measure. If this assumption does not hold, we argue that the regularized solutions may not converge to a solution of the limit problem with a Heaviside firing function.

Highlights

  • It is important to note that this ill-posed nature of the model is a fundamentally different mathematical property from the possible existence of unstable equilibria, which typically occur if a firing rate function with moderate steepness is used

  • The existence of a solution matter for point neuron models with a Heaviside firing rate function is summarized in the following theorem

  • We will first explain why the uniqueness question is a subtle issue for point neuron models with a Heaviside firing rate function

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Summary

Introduction

The limit process β → ∞, using different techniques, is studied in [18, 19] for the stationary solutions of neural field equations It has been observed [20] for the Wilson–Cowan model that this transition is a subtle matter: Using a steep sigmoid firing rate function instead of the Heaviside mapping can lead to significant changes in a Hopf bifurcation point. Smoothening techniques for discontinuous vector fields, which are similar to the regularization method considered in this paper, have been proposed and analyzed for rather general phase spaces [22,23,24] These studies consider qualitative properties of large classes of problems, whereas we focus on a quantitative analysis of a very special system of ODEs. For the sake of easy notation, we will sometimes write (1) in the form τ u (t) = −u(t) + ωSβ u(t) − uθ + q(t), t ∈ (0, T ], (3). For the sake of simplicity, use the same threshold value uθ for all the units in the network; see (4)

Assumptions
Uniformly Bounded and Equicontinuous
Threshold Terminology
Preparations
Convergence of the Integral
Limit Problem
Uniqueness
Example
Enforcing Uniqueness
Convergence of the Entire Sequence
Entire Sequence
Discussion and Conclusions
Full Text
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