Abstract

An unnoticed chaotic firing pattern, lying between period-1 and period-2 firing patterns, has received little attention over the past 20 years since it was first simulated in the Hindmarsh-Rose (HR) model. In the present study, the rat sciatic nerve model of chronic constriction injury (CCI) was used as an experimental neural pacemaker to investigate the transition regularities of spontaneous firing patterns. Chaotic firing lying between period-1 and period-2 firings was observed located in four bifurcation scenarios in different, isolated neural pacemakers. These bifurcation scenarios were induced by decreasing extracellular calcium concentrations. The behaviors after period-2 firing pattern in the four scenarios were period-doubling bifurcation not to chaos, period-doubling bifurcation to chaos, period-adding sequences with chaotic firings, and period-adding sequences with stochastic firings. The deterministic structure of the chaotic firing pattern was identified by the first return map of interspike intervals and a short-term prediction using nonlinear prediction. The experimental observations closely match those simulated in a two-dimensional parameter space using the HR model, providing strong evidences of the existence of chaotic firing lying between period-1 and period-2 firing patterns in the actual nervous system. The results also present relationships in the parameter space between this chaotic firing and other firing patterns, such as the chaotic firings that appear after period-2 firing pattern located within the well-known comb-shaped region, periodic firing patterns and stochastic firing patterns, as predicted by the HR model. We hope that this study can focus attention on and help to further the understanding of the unnoticed chaotic neural firing pattern.

Highlights

  • It has been suggested that various complex oscillation patterns play important roles in excitable biological systems [1,2]

  • Multiple examples of chaotic firing lying between period-1 firing and period-2 firings observed in the biological experiment performed on isolated neural pacemakers are provided

  • We hope that this study will enhance interest on the unknown chaotic firing pattern lying between period-1 and period-2 firings

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Summary

Introduction

It has been suggested that various complex oscillation patterns play important roles in excitable biological systems [1,2]. With the help of nonlinear dynamics, the complex oscillations including chaos have been analyzed in depth. Chaos and bifurcations have been observed in actual nervous systems [3,4,5,6]. They have been simulated in many theoretical neuronal models [7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24]. The HR model is composed of three nonlinear, ordinary differential equations: dx ~y{ax3zbx2{zzI ð1Þ dt dy ~c{dx2{y ð2Þ dt dz dt ~r1⁄2s(x{x0){zŠ

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