Abstract

Gamma (30–80 Hz) rhythms in hippocampus and neocortex resulting from the interaction of excitatory and inhibitory cells (E- and I-cells), called Pyramidal-Interneuronal Network Gamma (PING), require that the I-cells respond to the E-cells, but don't fire on their own. In idealized models, there is a sharp boundary between a parameter regime where the I-cells have weak-enough drive for PING, and one where they have so much drive that they fire without being prompted by the E-cells. In the latter regime, they often de-synchronize and suppress the E-cells; the boundary was therefore called the “suppression boundary” by Börgers and Kopell (2005). The model I-cells used in the earlier work by Börgers and Kopell have a “type 1” phase response, i.e., excitatory input always advances them. However, fast-spiking inhibitory basket cells often have a “type 2” phase response: Excitatory input arriving soon after they fire delays them. We study the effect of the phase response type on the suppression transition, under the additional assumption that the I-cells are kept synchronous by gap junctions. When many E-cells participate on a given cycle, the resulting excitation advances the I-cells on the next cycle if their phase response is of type 1, and this can result in suppression of more E-cells on the next cycle. Therefore, strong E-cell spike volleys tend to be followed by weaker ones, and vice versa. This often results in erratic fluctuations in the strengths of the E-cell spike volleys. When the phase response of the I-cells is of type 2, the opposite happens: strong E-cell spike volleys delay the inhibition on the next cycle, therefore tend to be followed by yet stronger ones. The strengths of the E-cell spike volleys don't oscillate, and there is a nearly abrupt transition from PING to ING (a rhythm involving I-cells only).

Highlights

  • Gamma-frequency (30–80 Hz) oscillations in hippocampus and neocortex are known to result, in many instances, from the interaction of excitatory pyramidal cells (E-cells) and fastspiking inhibitory interneurons (I-cells) (Whittington et al, 2000; Börgers and Kopell, 2003; Bartos et al, 2007; Traub and Whittington, 2010)

  • There can be a sharp boundary in parameter space between a regime in which the I-cells have weakenough drive for Pyramidal-Interneuronal Network Gamma (PING), and a regime in which they have so much drive that they fire without being prompted by the E-cells

  • If type 2 I-cells are introduced in the models of Börgers and Kopell (2005) and Börgers et al (2005), but without gapjunctional coupling, or if the type 1 I-cells are kept, but coupled by synchronizing gap junctions, we find that the suppression transition becomes considerably less tight

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Summary

INTRODUCTION

Gamma-frequency (30–80 Hz) oscillations in hippocampus and neocortex are known to result, in many instances, from the interaction of excitatory pyramidal cells (E-cells) and fastspiking inhibitory interneurons (I-cells) (Whittington et al, 2000; Börgers and Kopell, 2003; Bartos et al, 2007; Traub and Whittington, 2010). There can be a sharp boundary in parameter space between a regime in which the I-cells have weakenough drive for PING, and a regime in which they have so much drive that they fire without being prompted by the E-cells In the latter regime, they often de-synchronize, and suppress the E-cells altogether; the boundary in parameter space was called the “suppression boundary” in Börgers and Kopell (2005). We study the effect on the suppression transition of introducing I-cells with type 2 phase response, and coupling them with gap junctions strong enough to keep them synchronous (Kopell and Ermentrout, 2004; Ostojic et al, 2009). The idea that the suppression transition may play a central role in attentional processing remains intact when the I-cells are of type 2, connected by gap junctions

MODELS
SIMULATION RESULTS FOR LARGE NETWORKS
NETWORKS WITHOUT GAP-JUNCTIONAL COUPLING AMONG THE I-CELLS
DISCUSSION
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