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Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model

The power spectrum of brain activity is composed by peaks at characteristic frequencies superimposed to a background that decays as a power law of the frequency, [Formula: see text] , with an exponent [Formula: see text] close to 1 (pink noise). This exponent is predicted to be connected with the ex...

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Autores principales: Apicella, I., Scarpetta, S., de Arcangelis, L., Sarracino, A., de Candia, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9763404/
https://www.ncbi.nlm.nih.gov/pubmed/36536058
http://dx.doi.org/10.1038/s41598-022-26392-8
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author Apicella, I.
Scarpetta, S.
de Arcangelis, L.
Sarracino, A.
de Candia, A.
author_facet Apicella, I.
Scarpetta, S.
de Arcangelis, L.
Sarracino, A.
de Candia, A.
author_sort Apicella, I.
collection PubMed
description The power spectrum of brain activity is composed by peaks at characteristic frequencies superimposed to a background that decays as a power law of the frequency, [Formula: see text] , with an exponent [Formula: see text] close to 1 (pink noise). This exponent is predicted to be connected with the exponent [Formula: see text] related to the scaling of the average size with the duration of avalanches of activity. “Mean field” models of neural dynamics predict exponents [Formula: see text] and [Formula: see text] equal or near 2 at criticality (brown noise), including the simple branching model and the fully-connected stochastic Wilson–Cowan model. We here show that a 2D version of the stochastic Wilson–Cowan model, where neuron connections decay exponentially with the distance, is characterized by exponents [Formula: see text] and [Formula: see text] markedly different from those of mean field, respectively around 1 and 1.3. The exponents [Formula: see text] and [Formula: see text] of avalanche size and duration distributions, equal to 1.5 and 2 in mean field, decrease respectively to [Formula: see text] and [Formula: see text] . This seems to suggest the possibility of a different universality class for the model in finite dimension.
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spelling pubmed-97634042022-12-21 Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model Apicella, I. Scarpetta, S. de Arcangelis, L. Sarracino, A. de Candia, A. Sci Rep Article The power spectrum of brain activity is composed by peaks at characteristic frequencies superimposed to a background that decays as a power law of the frequency, [Formula: see text] , with an exponent [Formula: see text] close to 1 (pink noise). This exponent is predicted to be connected with the exponent [Formula: see text] related to the scaling of the average size with the duration of avalanches of activity. “Mean field” models of neural dynamics predict exponents [Formula: see text] and [Formula: see text] equal or near 2 at criticality (brown noise), including the simple branching model and the fully-connected stochastic Wilson–Cowan model. We here show that a 2D version of the stochastic Wilson–Cowan model, where neuron connections decay exponentially with the distance, is characterized by exponents [Formula: see text] and [Formula: see text] markedly different from those of mean field, respectively around 1 and 1.3. The exponents [Formula: see text] and [Formula: see text] of avalanche size and duration distributions, equal to 1.5 and 2 in mean field, decrease respectively to [Formula: see text] and [Formula: see text] . This seems to suggest the possibility of a different universality class for the model in finite dimension. Nature Publishing Group UK 2022-12-19 /pmc/articles/PMC9763404/ /pubmed/36536058 http://dx.doi.org/10.1038/s41598-022-26392-8 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open AccessThis 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 licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence 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 licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Apicella, I.
Scarpetta, S.
de Arcangelis, L.
Sarracino, A.
de Candia, A.
Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title_full Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title_fullStr Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title_full_unstemmed Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title_short Power spectrum and critical exponents in the 2D stochastic Wilson–Cowan model
title_sort power spectrum and critical exponents in the 2d stochastic wilson–cowan model
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9763404/
https://www.ncbi.nlm.nih.gov/pubmed/36536058
http://dx.doi.org/10.1038/s41598-022-26392-8
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