Abstract

The generation of abnormal excitations in pathological regions of the heart is a main trigger for lethal cardiac arrhythmias. Such abnormal excitations, also called ectopic activity, often arise from areas with local tissue heterogeneity or damage accompanied by localized depolarization. Finding the conditions that lead to ectopy is important to understand the basic biophysical principles underlying arrhythmia initiation and might further refine clinical procedures. In this study, we are the first to address the question of how geometry of the abnormal region affects the onset of ectopy using a combination of experimental, in silico, and theoretical approaches. We paradoxically find that, for any studied geometry of the depolarized region in optogenetically modified monolayers of cardiac cells, primary ectopic excitation originates at areas of maximal curvature of the boundary, where the stimulating electrotonic currents are minimal. It contradicts the standard critical nucleation theory applied to nonlinear waves in reaction-diffusion systems, where a higher stimulus is expected to produce excitation more easily. Our in silico studies reveal that the nonconventional ectopic activity is caused by an oscillatory instability at the boundary of the damaged region, the occurrence of which depends on the curvature of that boundary. The onset of this instability is confirmed using the Schrödinger equation methodology proposed by Rinzel and Keener [SIAM J. Appl. Math. 43, 907 (1983)]. Overall, we show distinctively novel insight into how the geometry of a heterogeneous cardiac region determines ectopic activity, which can be used in the future to predict the conditions that can trigger cardiac arrhythmias.

Highlights

  • Arrhythmias are the most common cause of sudden cardiac death worldwide, accounting for an estimated 6 million deaths annually [1]

  • The ectopic activity originated from the boundary of a quasistable depolarized (QSD) region

  • Using in silico models and an analytical approach, we demonstrate that the mechanism of this effect is closely related to the occurrence of oscillatory (i.e., Hopf) instability at these sites

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Summary

Introduction

Arrhythmias are the most common cause of sudden cardiac death worldwide, accounting for an estimated 6 million deaths annually [1]. The underlying mechanisms are still not completely understood. From a practical point of view, it is of paramount importance to understand the mechanisms of arrhythmia initiation, since by removing the triggers, arrhythmic events can be avoided. Multiple recordings have shown that, in many cases, lethal cardiac arrhythmias are triggered by so-called ectopic beats, i.e., ill-timed electrical pulses originating from damaged tissue, which disturb normal cardiac. Rhythm [2,3]. Despite their practical importance, the mesoscopic biophysical mechanisms of ectopic activity remain largely unknown [4]. In a very general sense, ectopic activity occurs when a depolarized region in the heart produces depolarizing currents strong enough to initiate propagating waves

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