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dc.contributor.authorWedgwood, KC
dc.contributor.authorLin, KK
dc.contributor.authorThul, R
dc.contributor.authorCoombes, S
dc.date.accessioned2017-08-10T11:36:19Z
dc.date.issued2013-01-24
dc.description.abstractPhase 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.citationVol. 3, article 2en_GB
dc.identifier.doi10.1186/2190-8567-3-2
dc.identifier.urihttp://hdl.handle.net/10871/28859
dc.language.isoenen_GB
dc.publisherBioMed Centralen_GB
dc.relation.urlhttps://www.ncbi.nlm.nih.gov/pubmed/23347723en_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.subjectPhase-amplitudeen_GB
dc.subjectOscillatoren_GB
dc.subjectChaosen_GB
dc.subjectNon-weak couplingen_GB
dc.titlePhase-amplitude descriptions of neural oscillator modelsen_GB
dc.typeArticleen_GB
dc.date.available2017-08-10T11:36:19Z
dc.identifier.issn2190-8567
exeter.place-of-publicationGermanyen_GB
dc.descriptionThis is the author accepted manuscript. The final version is available from BioMed Central via the DOI in this recorden_GB
dc.identifier.journalJournal of Mathematical Neuroscienceen_GB
dc.rights.urihttp://creativecommons.org/licenses/by/2.0


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© 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.
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.