Elsevier

Neurocomputing

Volume 69, Issues 10–12, June 2006, Pages 1062-1065
Neurocomputing

Dependence of the spike-triggered average voltage on membrane response properties

https://doi.org/10.1016/j.neucom.2005.12.046Get rights and content

Abstract

The spike-triggered average voltage (STV) is an experimentally measurable quantity that is determined by both the membrane response properties and the statistics of the synaptic drive. Here, the form of the STV is modelled for neurons with three distinct types of subthreshold dynamics; passive decay, h-current sag, and damped oscillations. Analytical expressions for the STV are first obtained in the low-noise limit, identifying how the subthreshold dynamics of the cell affect its form. A second result is then derived that captures the power-law behaviour of the STV near the spike threshold.

Introduction

Reverse-correlation methods are a standard tool in the neurosciences [2]. The spike-triggered average voltage (STV) is a quantity that contains information about both the statistics of the synaptic drive and the response properties of the neuron, and can be readily extracted from intracellular voltage traces. An analytical understanding of the processes that shape the STV can be used to classify the response characteristics of neurons and the synaptic drive to which they are subjected [1].

Typically, the neuronal models that have been used to investigate the STV are of the integrate-and-fire (IF) type with leaky, passive dynamics [1], [8]. The IF model, however, misses many important features of biological neurons such as the h-current sag seen in cortical and hippocampal pyramidal cells, as well as more complex behaviour such as damped oscillations seen in certain entorhinal cortical cells [4].

Here the form of the spike-triggered average will be investigated for model neurons with biologically more realistic dynamics. Two methods will be used: the first involves a low-noise approximation, which, in the context of spiking neurons, corresponds to low-noise, noise-driven spike generation; the second method captures the power-law behaviour of the STV near threshold—a feature missed by low-noise approximations.

Section snippets

The model

The subthreshold voltage dynamics are described by a two-variable IF model [3], [5], [9], [10] which is sufficient to capture the response of neurons with passive dynamics, h-current sag response and damped oscillations. The model comprises a variable v for the membrane voltage, with time-scale τv and a second variable w proportional to the excess current flowing through voltage-gated trans-membrane channels, with time-scale τw and coupled with strength γ to the voltage. Thus,τvv˙=μ-v-γw+τvσξ(t)

Low-noise approximation

Our calculation is based on a principle which states that for a set of equations of the type (1), the most likely trajectory followed by the system when moving from one point to another is obtained by maximising the probability of the synaptic input τvσξ(t) that would yield such a transition. This optimisation is carried through the minimisation of a cost function that will now be derived (the informal derivation given here follows the well-known principle of minimum available noise energy [7]).

Discussion

We have derived analytical expressions for the spike-triggered average voltage (STV) of three model neurons with subthreshold dynamics corresponding to those seen in biological neurons: passive decay, h-current sag and damped oscillations. Our analyses demonstrate that (i) the form of the STV is closely related to the subthreshold membrane dynamics, and (ii) for a hard-threshold model with white noise the STV behaves as a t power-law near threshold. The distinct forms for the STV derived here

Acknowledgements

We thank Liam Paninski for useful discussions. This work was supported by Grant no. 200020-108093/1 of the Swiss National Science Foundation.

Wulfram Gerstner received his Ph.D. degree in theoretical physics from the TU Munich, Germany, in 1993, after studies in Tübingen, Berkeley, and Munich. He is a Professor and Head of the Laboratory of Computational Neuroscience, EPFL, Switzerland.

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Wulfram Gerstner received his Ph.D. degree in theoretical physics from the TU Munich, Germany, in 1993, after studies in Tübingen, Berkeley, and Munich. He is a Professor and Head of the Laboratory of Computational Neuroscience, EPFL, Switzerland.

Laurent Badel is a Ph.D. student at the Laboratory of Computational Neuroscience (LCN) at the EPFL. He received his M.Sc. in physics from the EPFL in march 2003. His current research interests are mathematical and statistical approaches to the analysis of neuronal systems.

Magnus Richardson obtained his D-Phil in theoretical physics in 1997 at the University of Oxford. Since then he has worked on various subjects in the neurosciences and is currently interested in how neuronal properties lead to emergent states at the level of neural networks.

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