Nervous system
Cellular and network mechanisms of electrographic seizures

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Epileptic seizures constitute a complex multiscale phenomenon that is characterized by synchronized hyperexcitation of neurons in neuronal networks. Recent progress in understanding pathological seizure dynamics provides crucial insights into underlying mechanisms and possible new avenues for the development of novel treatment modalities. Here we review some recent work that combines in vivo experiments and computational modeling to unravel the pathophysiology of seizures of cortical origin. We focus particularly on how activity-dependent changes in extracellular potassium concentration affect the intrinsic dynamics of neurons involved in cortical seizures characterized by spike/wave complexes and fast runs.

Section editor:

Gabriel A. Silva – Bioengineering and Ophthalmology, University of California, San Diego, La Jolla, CA, USA

Introduction

It is widely accepted that the development of epileptiform activity can result from a shift in the balance between synaptic excitation and inhibition toward excitation [1, 2, 3, 4]. In fact, an easy way to elicit acute seizures experimentally is to block synaptic inhibition [5, 6, 7, 8, 9, 10, 11]. Accordingly, the traditional point of view is that the key intracellular correlate of epileptiform activity, the paroxysmal depolarizing shift (PDS), consists of a giant EPSP [12] enhanced by the activation of voltage-regulated intrinsic currents [1, 13, 14, 15, 16, 17]. It was therefore a surprise when more recent evidence showed that synaptic inhibition remains functional in many forms of paroxysmal activities [18, 19, 20, 21, 22, 23, 24, 25, 26]. Also, disruption of inhibitory function does not affect neocortical kindling [27], which is associated with an increase in synaptic strength that mediates recruitment of larger cortical areas [28]. Furthermore, the firing of fast-spiking inhibitory interneurons (INs) during cortically generated seizures is much stronger than the activity of other types of cortical neurons [24]. Therefore, a decrease or even the absence of synaptic inhibition in the presence of synaptic excitation cannot serve as a general mechanism of cortical epileptic seizures.

Extracellular potassium concentration [K+]o increases during neuronal activity. In the presence of neuronal hyperexcitability, the [K+]o apparatus fails to maintain [K+]o homeostasis (Grafstain, [100]; Somjen, [101]; Frohlich, [102]). The resulting increase in [K+]o depolarizes the reversal potential of K+ currents and can also affect the maximal conductances of some depolarizing currents such as the hyperpolarization-activated depolarizing current (Ih) [29] and the persistent sodium current (INa(p)) [30]. Thus, the overall effect of an increase in [K+]o is an upregulation of neuronal excitability. Indeed, periodic bursting was found in vitro after increasing [K+]o [31, 32, 33]. Thus, changes in [K+]o may play a crucial role in seizure dynamics.

The complexity of the interaction dynamics between neuronal networks and ion concentrations during epileptiform activity requires a combined approach of experimental work and computational models. Here, we discuss recent modeling results regarding mechanisms of epileptic seizures in cortex. First, we present an analysis of the network and cellular mechanisms of electrographic seizures in vivo. Then, we discuss the results from computational models that incorporate extracellular K+ concentration dynamics based on experimental data. Our findings suggest that (1) changes in [K+]o activate latent intrinsic burst dynamics that result in paroxysmal bursting and (2) the dynamic interaction between network activity and [K+]o causes the emergence of a stable paroxysmal network state in the form of selfsustained oscillations. We conclude with specific predictions derived from our model and propose that molecular mechanisms responsible for [K+]o regulation should be examined as novel targets for pharmacological intervention in patients suffering from epilepsy.

Section snippets

Cortical origin of paroxysmal oscillations generated within the thalamocortical system

The origin of electrical seizures that accompany various types of epilepsy is largely unknown, especially for cortically generated seizures. Recent experimental studies strongly implicate a neocortical origin of spike–wave (SW) electroencephalographic (EEG) complexes at ∼3 Hz, as in petit-mal epilepsy and seizures with the EEG pattern of the Lennox-Gastaut syndrome [11, 34, 35, 36, 37, 38]. The etiologies of cortically generated seizures include cortical dysplasia, traumatic injury and other

Cellular mechanisms mediating spike and wave discharges

The EEG ‘spike’ of SW complexes corresponds to the PDS of the membrane voltage in intracellular recordings (reviewed in [26, 48, 49]). Initially, PDSs have been regarded as giant EPSPs [12, 50], enhanced by the activation of voltage-gated intrinsic (high-threshold Ca2+ and persistent Na+) currents [1, 13, 15, 17]. Specifically, the EPSPs initiate the PDS by depolarizing the postsynaptic neurons to the level of activation of the persistent Na+ current that maintains and enhances the achieved

Changes in the extracellular milieu and epileptogenesis

Modulation of extracellular ionic concentrations has a profound impact on the excitability of neurons and neuronal networks. According to Grafstein's hypothesis [81], K+ released during intense neuronal firing may accumulate in the interstitial space, depolarize neurons and lead to spike inactivation. During seizures, the increase in [K+]o reaches 16 mM in the case of 4-AP-induced epileptiform discharges in hippocampus [82] and 7–12 mM in case of spontaneous electrographic seizures in neocortex [

Effects of intrinsic conductances on K+-induced oscillations

In agreement with in vivo results (see Fig. 3), high-threshold Ca2+ and persistent Na+ currents were important in creating periodic bursting in our model of neocortical activity in moderately elevated [K+]o (Fig. 5). After oscillations were induced by long DC stimulation, sufficiently high maximal conductances for INa(p) and ICa were required to maintain periodic bursting. On the gCa(gNa(p)) plane (see Fig. 5a, left) the region for bursting was bounded by two curves. Below the bottom curve, no

Synchronization during fast runs and slow bursting

We recently reported very low levels of both short- and long-range synchronization during paroxysmal fast runs [89]. To study synchrony of population oscillations during different oscillatory regimes, we used computer simulations of network models composed of 100 PY neurons and 25 INs. Without synaptic coupling, the model neurons fired independently because of random variability of the model parameters across neurons and different initial conditions (Fig. 6a, top). Upon termination of a

Selfsustained oscillations mediated by extracellular K+ dynamics

In our modeling studies, the occurrence of oscillatory patterns displayed by cortical neurons (slow bursting or fast run) depended on the absolute level of [K+]o [88, 90]. In the model of an isolated cortical neuron, fast runs were the only stable firing pattern in the presence of moderately elevated levels of [K+]o ([K+]o < [K+]ocr1  5.75 mM). For higher [K+]o levels ([K+]o > [K+]ocr2  6.4 mM), slow bursting was the only stable firing pattern. Importantly, for an intermediate range of [K+]o, these two

Conclusion

Epileptic seizures are commonly considered unstable runaway dynamics of neuronal networks. Specifically, it has been suggested that positive feedback interaction between extracellular potassium and neural activity mediates cortical seizures. In a series of studies, reviewed here, we showed that epileptic seizures might represent a stable (or quasi-stable) cortical state caused by extracellular potassium concentration dynamics. This pathological state consisted of alternating epochs of tonic

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