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分层威尔逊-考恩模型与连接矩阵。

Hierarchical Wilson-Cowan Models and Connection Matrices.

作者信息

Zúñiga-Galindo W A, Zambrano-Luna B A

机构信息

School of Mathematical & Statistical Sciences, University of Texas Rio Grande Valley, One West University Blvd., Brownsville, TX 78520, USA.

出版信息

Entropy (Basel). 2023 Jun 16;25(6):949. doi: 10.3390/e25060949.

DOI:10.3390/e25060949
PMID:37372293
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10297397/
Abstract

This work aims to study the interplay between the Wilson-Cowan model and connection matrices. These matrices describe cortical neural wiring, while Wilson-Cowan equations provide a dynamical description of neural interaction. We formulate Wilson-Cowan equations on locally compact Abelian groups. We show that the Cauchy problem is well posed. We then select a type of group that allows us to incorporate the experimental information provided by the connection matrices. We argue that the classical Wilson-Cowan model is incompatible with the small-world property. A necessary condition to have this property is that the Wilson-Cowan equations be formulated on a compact group. We propose a -adic version of the Wilson-Cowan model, a hierarchical version in which the neurons are organized into an infinite rooted tree. We present several numerical simulations showing that the -adic version matches the predictions of the classical version in relevant experiments. The -adic version allows the incorporation of the connection matrices into the Wilson-Cowan model. We present several numerical simulations using a neural network model that incorporates a -adic approximation of the connection matrix of the cat cortex.

摘要

这项工作旨在研究威尔逊 - 考恩模型与连接矩阵之间的相互作用。这些矩阵描述了皮质神经布线,而威尔逊 - 考恩方程提供了神经相互作用的动态描述。我们在局部紧阿贝尔群上建立威尔逊 - 考恩方程。我们证明了柯西问题是适定的。然后,我们选择一种类型的群,使我们能够纳入连接矩阵提供的实验信息。我们认为经典的威尔逊 - 考恩模型与小世界性质不兼容。具有此性质的一个必要条件是威尔逊 - 考恩方程要在紧群上建立。我们提出了威尔逊 - 考恩模型的 - 进数版本,这是一个层次版本,其中神经元被组织成一棵无限根树。我们给出了几个数值模拟,表明 - 进数版本在相关实验中与经典版本的预测相匹配。 - 进数版本允许将连接矩阵纳入威尔逊 - 考恩模型。我们使用一个神经网络模型进行了几个数值模拟,该模型纳入了猫皮质连接矩阵的 - 进数近似。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/281b8f2f8b53/entropy-25-00949-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/73602a2c4fb1/entropy-25-00949-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/9a075b94b077/entropy-25-00949-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/cc647262c5e4/entropy-25-00949-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/71688cad7633/entropy-25-00949-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/f7f8b1beea60/entropy-25-00949-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/cb3e24e983f8/entropy-25-00949-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/ac0c7287aa67/entropy-25-00949-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/4a2a42ad0343/entropy-25-00949-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/87e83c3a24b4/entropy-25-00949-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/281b8f2f8b53/entropy-25-00949-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/73602a2c4fb1/entropy-25-00949-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/9a075b94b077/entropy-25-00949-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/cc647262c5e4/entropy-25-00949-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/71688cad7633/entropy-25-00949-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/f7f8b1beea60/entropy-25-00949-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/cb3e24e983f8/entropy-25-00949-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/ac0c7287aa67/entropy-25-00949-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/4a2a42ad0343/entropy-25-00949-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/87e83c3a24b4/entropy-25-00949-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9a2/10297397/281b8f2f8b53/entropy-25-00949-g010.jpg

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