Phase-amplitude descriptions of neural oscillator models
dc.contributor.author | Wedgwood, KC | |
dc.contributor.author | Lin, KK | |
dc.contributor.author | Thul, R | |
dc.contributor.author | Coombes, S | |
dc.date.accessioned | 2017-08-10T11:36:19Z | |
dc.date.issued | 2013-01-24 | |
dc.description.abstract | Phase oscillators are a common starting point for the reduced description of many single neuron models that exhibit a strongly attracting limit cycle. The framework for analysing such models in response to weak perturbations is now particularly well advanced, and has allowed for the development of a theory of weakly connected neural networks. However, the strong-attraction assumption may well not be the natural one for many neural oscillator models. For example, the popular conductance based Morris-Lecar model is known to respond to periodic pulsatile stimulation in a chaotic fashion that cannot be adequately described with a phase reduction. In this paper, we generalise the phase description that allows one to track the evolution of distance from the cycle as well as phase on cycle. We use a classical technique from the theory of ordinary differential equations that makes use of a moving coordinate system to analyse periodic orbits. The subsequent phase-amplitude description is shown to be very well suited to understanding the response of the oscillator to external stimuli (which are not necessarily weak). We consider a number of examples of neural oscillator models, ranging from planar through to high dimensional models, to illustrate the effectiveness of this approach in providing an improvement over the standard phase-reduction technique. As an explicit application of this phase-amplitude framework, we consider in some detail the response of a generic planar model where the strong-attraction assumption does not hold, and examine the response of the system to periodic pulsatile forcing. In addition, we explore how the presence of dynamical shear can lead to a chaotic response. | en_GB |
dc.identifier.citation | Vol. 3, article 2 | en_GB |
dc.identifier.doi | 10.1186/2190-8567-3-2 | |
dc.identifier.uri | http://hdl.handle.net/10871/28859 | |
dc.language.iso | en | en_GB |
dc.publisher | BioMed Central | en_GB |
dc.relation.url | https://www.ncbi.nlm.nih.gov/pubmed/23347723 | en_GB |
dc.rights | © K.C.A. Wedgwood et al.; licensee Springer 2013. This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. | en_GB |
dc.subject | Phase-amplitude | en_GB |
dc.subject | Oscillator | en_GB |
dc.subject | Chaos | en_GB |
dc.subject | Non-weak coupling | en_GB |
dc.title | Phase-amplitude descriptions of neural oscillator models | en_GB |
dc.type | Article | en_GB |
dc.date.available | 2017-08-10T11:36:19Z | |
dc.identifier.issn | 2190-8567 | |
exeter.place-of-publication | Germany | en_GB |
dc.description | This is the author accepted manuscript. The final version is available from BioMed Central via the DOI in this record | en_GB |
dc.identifier.journal | Journal of Mathematical Neuroscience | en_GB |
dc.rights.uri | http://creativecommons.org/licenses/by/2.0 |
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Except where otherwise noted, this item's licence is described as © K.C.A. Wedgwood et al.; licensee Springer 2013. This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.