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成对最大熵模型中的双稳性、非遍历性和抑制作用。

Bistability, non-ergodicity, and inhibition in pairwise maximum-entropy models.

作者信息

Rostami Vahid, Porta Mana PierGianLuca, Grün Sonja, Helias Moritz

机构信息

Institute of Neuroscience and Medicine (INM-6) and Institute for Advanced Simulation (IAS-6) and JARA BRAIN Institute I, Jülich Research Centre, Jülich, Germany.

Theoretical Systems Neurobiology, RWTH Aachen University, Aachen, Germany.

出版信息

PLoS Comput Biol. 2017 Oct 2;13(10):e1005762. doi: 10.1371/journal.pcbi.1005762. eCollection 2017 Oct.

DOI:10.1371/journal.pcbi.1005762
PMID:28968396
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5645158/
Abstract

Pairwise maximum-entropy models have been used in neuroscience to predict the activity of neuronal populations, given only the time-averaged correlations of the neuron activities. This paper provides evidence that the pairwise model, applied to experimental recordings, would produce a bimodal distribution for the population-averaged activity, and for some population sizes the second mode would peak at high activities, that experimentally would be equivalent to 90% of the neuron population active within time-windows of few milliseconds. Several problems are connected with this bimodality: 1. The presence of the high-activity mode is unrealistic in view of observed neuronal activity and on neurobiological grounds. 2. Boltzmann learning becomes non-ergodic, hence the pairwise maximum-entropy distribution cannot be found: in fact, Boltzmann learning would produce an incorrect distribution; similarly, common variants of mean-field approximations also produce an incorrect distribution. 3. The Glauber dynamics associated with the model is unrealistically bistable and cannot be used to generate realistic surrogate data. This bimodality problem is first demonstrated for an experimental dataset from 159 neurons in the motor cortex of macaque monkey. Evidence is then provided that this problem affects typical neural recordings of population sizes of a couple of hundreds or more neurons. The cause of the bimodality problem is identified as the inability of standard maximum-entropy distributions with a uniform reference measure to model neuronal inhibition. To eliminate this problem a modified maximum-entropy model is presented, which reflects a basic effect of inhibition in the form of a simple but non-uniform reference measure. This model does not lead to unrealistic bimodalities, can be found with Boltzmann learning, and has an associated Glauber dynamics which incorporates a minimal asymmetric inhibition.

摘要

成对最大熵模型已被用于神经科学领域,用于仅根据神经元活动的时间平均相关性来预测神经元群体的活动。本文提供的证据表明,将成对模型应用于实验记录时,群体平均活动会产生双峰分布,并且对于某些群体规模,第二个峰将出现在高活动水平,在实验中这相当于在几毫秒的时间窗口内90%的神经元群体处于活跃状态。这种双峰性存在几个问题:1. 从观察到的神经元活动以及神经生物学角度来看,高活动模式的存在是不现实的。2. 玻尔兹曼学习变得非遍历性,因此无法找到成对最大熵分布:实际上,玻尔兹曼学习会产生不正确的分布;类似地,平均场近似的常见变体也会产生不正确的分布。3. 与该模型相关的格劳伯动力学是不现实的双稳态,不能用于生成现实的替代数据。首先针对猕猴运动皮层中159个神经元的实验数据集证明了这种双峰性问题。然后提供的证据表明,这个问题会影响几百个或更多神经元群体规模的典型神经记录。双峰性问题的原因被确定为具有均匀参考测度的标准最大熵分布无法对神经元抑制进行建模。为了消除这个问题,提出了一种改进的最大熵模型,该模型以简单但非均匀的参考测度形式反映了抑制的基本作用。这个模型不会导致不现实的双峰性,可以通过玻尔兹曼学习找到,并且具有包含最小不对称抑制的相关格劳伯动力学。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/d03f1e270b86/pcbi.1005762.g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/597c66223760/pcbi.1005762.g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/c2e30aab0773/pcbi.1005762.g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/f94f2feafec7/pcbi.1005762.g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/296cf9561be2/pcbi.1005762.g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/4de81037e847/pcbi.1005762.g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/8b0c18b35475/pcbi.1005762.g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/636c1f3f435a/pcbi.1005762.g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/8cde40d72a6b/pcbi.1005762.g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/d03f1e270b86/pcbi.1005762.g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/597c66223760/pcbi.1005762.g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/c2e30aab0773/pcbi.1005762.g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/f94f2feafec7/pcbi.1005762.g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/296cf9561be2/pcbi.1005762.g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/4de81037e847/pcbi.1005762.g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/8b0c18b35475/pcbi.1005762.g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/636c1f3f435a/pcbi.1005762.g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/8cde40d72a6b/pcbi.1005762.g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9993/5645158/d03f1e270b86/pcbi.1005762.g009.jpg

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