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HAL Id: inserm-00842317

https://www.hal.inserm.fr/inserm-00842317

Submitted on 8 Jul 2013

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Multistability in large scale models of brain activity

Mathieu Golos, Viktor Jirsa, Emmanuel Daucé

To cite this version:

Mathieu Golos, Viktor Jirsa, Emmanuel Daucé. Multistability in large scale models of brain activity.

the Twenty Second Annual Computational Neuroscience Meeting: CNS*2013, Jul 2013, paris, France.

pp.P84. �inserm-00842317�

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P O S T E R P R E S E N T A T I O N

Open Access

Multistability in large scale models of brain

activity

Mathieu Golos

1

, Viktor K Jirsa

1

, Emmanuel Daucé

1,2*

From

Twenty Second Annual Computational Neuroscience Meeting: CNS*2013

Paris, France. 13-18 July 2013

Rich spatiotemporal dynamical patterns, observed in the brain at rest, reveal several large-scale functional net-works, presumably involved in different brain functions. In parallel, structural networks obtained by Diffusion Spectrum Imaging ("connectome”) identify several

interconnected sub-networks that overlap with the func-tional networks [3]. Neural mass model simulations aim at developing realistic models of the brain activity. In particular, multiple fixed-point attractors can be identi-fied and spontaneous alternation between several brain

* Correspondence: Emmanuel.Dauce@centrale-marseille.fr

1Inserm, Aix-Marseille Université, INS UMR 1106, Marseille 13005, France

Full list of author information is available at the end of the article

Figure 1Number of attractors obtained for different (Ω, ||W||) couples with g = 30. Attractor patterns isodensity lines are indicated in black Golos et al. BMC Neuroscience 2013, 14(Suppl 1):P84

http://www.biomedcentral.com/1471-2202/14/S1/P84

© 2013 Golos et al; licensee BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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“states” can be obtained [2]. The number and the orga-nization of the “fixed-point” attractors strongly vary depending of the parameters used in the model.

In order to provide a general view of connectome-based dynamical systems, we developed a simplified neural mass model inspired by the continuous Hopfield network [4], to which we add a stochastic component, and a dynamic threshold (eq.2) that prevents reaching the two trivial attractors of system (eq.1).

τdxi dt = −xi+ N  j=1 Wi,jϕxj, γ , θ + σ2ηi(t) (1) τθ dt = −θ +  N N  i=1 ϕ (xi, γ , θ ) (2) ϕ (xi, γ , θ ) = 1 2(1 + tanh (γ (xi− θ ))) (3)

where W is the N = 66 nodes human connectome [3], x is the node potential,  is the node output, θ is the adaptive threshold, h(t) is a white noise and s the diffu-sion parameter. Three main parameters (excitation strength ||W||, inhibition strength Ω and node excitabil-ity g) are systematically varied in order to identify the fixed points attractors of the dynamics (Figure 1).

The adaptive threshold plays the role of a global inhi-bition and allows stabilizing many attractors, where the Ω / ||W|| ratio controls the sparsity of the activity. Then multistable dynamical systems are obtained in a large region of the parameter space, allowing to identify many different attractor patterns. The number of attrac-tors is found to increase with the value of gamma (node excitability), at the expense of their intrinsic stability. Itinerant dynamics is obtained when a significant noise level is introduced in the system. Then, several “attrac-tive” patterns can be reached on a single trajectory, where the duration of the visit reflects the stability of the pattern.

The simple dynamical system we have implemented allows exploring a large region of the parameters space, but is also capable of reproducing some aspects of the brain’s spontaneous activity (switching between different attractors). The set of attractors we find in some regions of the parameters space share similarities with the dif-ferent functional modes observed in the resting-state activity [1].

Author details

1

Inserm, Aix-Marseille Université, INS UMR 1106, Marseille 13005, France.

2Ecole Centrale Marseille, Marseille 13013, France.

Published: 8 July 2013

References

1. Damoiseaux JS, Rombouts S, Barkhof F, Scheltens P, Stam C, Smith P, Beckmann C: Consistent resting-state networks across healthy subjects. PNAS2006.

2. Deco G, Jirsa VK: Ongoing cortical activity at rest: criticality, multistability and ghost attractors. J Neuroscience 2012.

3. Hagmann P, Cammoun L, Gigandet X, Meuli R, Honey C, Wedeen V, Sporns O: Mapping the structural core of human cerebral cortex. PLoS Biol2008.

4. Hopfield JJ: Neural networks and physical systems with emergent collective computational abilities. Proc Natl Acad Sci USA 1982.

doi:10.1186/1471-2202-14-S1-P84

Cite this article as: Golos et al.: Multistability in large scale models of brain activity. BMC Neuroscience 2013 14(Suppl 1):P84.

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Golos et al. BMC Neuroscience 2013, 14(Suppl 1):P84 http://www.biomedcentral.com/1471-2202/14/S1/P84

Figure

Figure 1 Number of attractors obtained for different (Ω, ||W||) couples with g = 30. Attractor patterns isodensity lines are indicated in blackGoloset al.BMC Neuroscience2013,14(Suppl 1):P84

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