SearcharxivSearch

arXiv · 1307.2129

Finite size effects in the correlation structure of stochastic neural networks: analysis of different connectivity matrices and failure of the mean-field theory

Abstract

We quantify the finite size effects in a stochastic network made up of rate neurons, for several kinds of recurrent connectivity matrices. This analysis is performed by means of a perturbative expansion of the neural equations, where the perturbative parameters are the intensities of the sources of randomness in the system. In detail, these parameters are the variances of the background or input noise, of the initial conditions and of the distribution of the synaptic weights. The technique developed in this article can be used to study systems which are invariant under the exchange of the neural indices and it allows us to quantify the correlation structure of the network, in terms of pairwise and higher order correlations between the neurons. We also determine the relation between the correlation and the external input of the network, showing that strong signals coming from the environment reduce significantly the amount of correlation between the neurons. Moreover we prove that in general the phenomenon of propagation of chaos does not occur, even in the thermodynamic limit, due to the correlation structure of the 3 sources of randomness considered in the model. Furthermore, we show that the propagation of chaos does not depend only on the number of neurons in the network, but also and mainly on the number of incoming connections per neuron. To conclude, we prove that for special values of the parameters of the system the neurons become perfectly correlated, a phenomenon that we have called stochastic synchronization. These discoveries clearly prevent the use of the mean-field theory in the description of the neural network.

Explore related subjects

Keep this discovery

BibTeXRIS

D. Fasoli, O. Faugeras. 2013-07-08. Finite size effects in the correlation structure of stochastic neural networks: analysis of different connectivity matrices and failure of the mean-field theory. https://arxiv.org/abs/1307.2129

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Admissible Fourier Lengths, KAM Reducibility, and Spectral Applications

We develop a perturbative KAM reducibility theory for one-frequency $\mathrm{SL}(2,\mathbb{R})$ cocycles based on an admissible Fourier length $\ell$. The regularity relevant to the iteration is measured by positive adapted Fourier width rather than ordinary smoothness in the Euclidean length $|n|$. The same length governs Fourier decay, truncation and resonance scales, and the arithmetic condition controlling the small divisors. This framework contains the classical analytic and Gevrey settings, while non-monotone choices of $\ell$ allow classical nowhere differentiable Weierstrass-type perturbations and continuous perturbations outside every positive H\"older class. As spectral applications, we obtain purely absolutely continuous spectrum for every phase and $1/2$-H\"older continuity of the integrated density of states for the associated quasiperiodic Schr\"odinger operators. The Aubry dual has pure point spectrum for Lebesgue almost every dual phase, with eigenfunctions exponentially localized in the metric induced by $\ell$. We also construct nowhere differentiable quasiperiodic potentials with purely absolutely continuous Cantor spectrum.

math.DS

Dynamics inside the attracting basins of some skew products

Polynomial skew products in $\mathbb{C}^2$ are maps of the form $F(z,w)=(P(z),Q(z,w))$, where $P$ and $Q$ are polynomials. Their local dynamics have been widely investigated. In this paper, we study the global dynamics inside Fatou components of some skew products. We consider all the inverse images in a Fatou component of a given point and use the Kobayashi metric to measure the distance between points. In the cases we consider, there are always arbitrarily large Kobayashi balls in the complement of these inverse sets.

math.DS

Ergodicity of dynamical systems without uniqueness of orbits

Recently, there has been considerable interest in the study of non-deterministic dynamical systems. To analyze the chaotic behavior of such systems from a measure-theoretic viewpoint, it is desirable to consider ergodicity. However, the classical definition of ergodicity involves invariant sets, whose definition is not unique for non-deterministic dynamical systems. Thus, we are led to the question of which invariance yields an interesting definition of ergodicity. Here, we propose a definition based on the strong backward invariance and show that analogs of classical results hold. We also consider implications of the Birkhoff ergodic theorem for systems without uniqueness of orbits.

math.DS