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Resonance phenomena controlled by external feedback signals and additive noise in neural systems
Chaotic resonance is a phenomenon that can replace the fluctuation source in stochastic resonance from additive noise to chaos. We previously developed a method to control the chaotic state for suitably generating chaotic resonance by external feedback even when the external adjustment of chaos is d...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6718685/ https://www.ncbi.nlm.nih.gov/pubmed/31477740 http://dx.doi.org/10.1038/s41598-019-48950-3 |
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author | Nobukawa, Sou Shibata, Natsusaku Nishimura, Haruhiko Doho, Hirotaka Wagatsuma, Nobuhiko Yamanishi, Teruya |
author_facet | Nobukawa, Sou Shibata, Natsusaku Nishimura, Haruhiko Doho, Hirotaka Wagatsuma, Nobuhiko Yamanishi, Teruya |
author_sort | Nobukawa, Sou |
collection | PubMed |
description | Chaotic resonance is a phenomenon that can replace the fluctuation source in stochastic resonance from additive noise to chaos. We previously developed a method to control the chaotic state for suitably generating chaotic resonance by external feedback even when the external adjustment of chaos is difficult, establishing a method named reduced region of orbit (RRO) feedback. However, a feedback signal was utilized only for dividing the merged attractor. In addition, the signal sensitivity in chaotic resonance induced by feedback signals and that of stochastic resonance by additive noise have not been compared. To merge the separated attractor, we propose a negative strength of the RRO feedback signal in a discrete neural system which is composed of excitatory and inhibitory neurons. We evaluate the features of chaotic resonance and compare it to stochastic resonance. The RRO feedback signal with negative strength can merge the separated attractor and induce chaotic resonance. We also confirm that additive noise induces stochastic resonance through attractor merging. The comparison of these resonance modalities verifies that chaotic resonance provides more applicability than stochastic resonance given its capability to handle attractor separation and merging. |
format | Online Article Text |
id | pubmed-6718685 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-67186852019-09-17 Resonance phenomena controlled by external feedback signals and additive noise in neural systems Nobukawa, Sou Shibata, Natsusaku Nishimura, Haruhiko Doho, Hirotaka Wagatsuma, Nobuhiko Yamanishi, Teruya Sci Rep Article Chaotic resonance is a phenomenon that can replace the fluctuation source in stochastic resonance from additive noise to chaos. We previously developed a method to control the chaotic state for suitably generating chaotic resonance by external feedback even when the external adjustment of chaos is difficult, establishing a method named reduced region of orbit (RRO) feedback. However, a feedback signal was utilized only for dividing the merged attractor. In addition, the signal sensitivity in chaotic resonance induced by feedback signals and that of stochastic resonance by additive noise have not been compared. To merge the separated attractor, we propose a negative strength of the RRO feedback signal in a discrete neural system which is composed of excitatory and inhibitory neurons. We evaluate the features of chaotic resonance and compare it to stochastic resonance. The RRO feedback signal with negative strength can merge the separated attractor and induce chaotic resonance. We also confirm that additive noise induces stochastic resonance through attractor merging. The comparison of these resonance modalities verifies that chaotic resonance provides more applicability than stochastic resonance given its capability to handle attractor separation and merging. Nature Publishing Group UK 2019-09-02 /pmc/articles/PMC6718685/ /pubmed/31477740 http://dx.doi.org/10.1038/s41598-019-48950-3 Text en © The Author(s) 2019 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Nobukawa, Sou Shibata, Natsusaku Nishimura, Haruhiko Doho, Hirotaka Wagatsuma, Nobuhiko Yamanishi, Teruya Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title | Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title_full | Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title_fullStr | Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title_full_unstemmed | Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title_short | Resonance phenomena controlled by external feedback signals and additive noise in neural systems |
title_sort | resonance phenomena controlled by external feedback signals and additive noise in neural systems |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6718685/ https://www.ncbi.nlm.nih.gov/pubmed/31477740 http://dx.doi.org/10.1038/s41598-019-48950-3 |
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