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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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Detalles Bibliográficos
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
Descripción
Sumario: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.