ID: nlin/0610007

Noise-induced cooperative dynamics and its control in coupled neuron models

October 4, 2006

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Noise Induced Complexity: From Subthreshold Oscillations to Spiking in Coupled Excitable Systems

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M. Zaks, X. Sailer, ... , Neiman A.
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We study stochastic dynamics of an ensemble of N globally coupled excitable elements. Each element is modeled by a FitzHugh-Nagumo oscillator and is disturbed by independent Gaussian noise. In simulations of the Langevin dynamics we characterize the collective behavior of the ensemble in terms of its mean field and show that with the increase of noise the mean field displays a transition from a steady equilibrium to global oscillations and then, for sufficiently large noise, ...

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Mass synchronization: Occurrence and its control with possible applications to brain dynamics

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V. K. Chandrasekar, Jane H. Sheeba, M. Lakshmanan
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Occurrence of strong or mass synchronization of a large number of neuronal populations in the brain characterizes its pathological states. In order to establish an understanding of the mechanism underlying such pathological synchronization we present a model of coupled populations of phase oscillators representing the interacting neuronal populations. Through numerical analysis, we discuss the occurrence of mass synchronization in the model, where a source population which ge...

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Oscillations and Random Perturbations of a FitzHugh-Nagumo System

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Catherine LJLL Doss, Michèle PMA Thieullen
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We consider a stochastic perturbation of a FitzHugh-Nagumo system. We show that it is possible to generate oscillations for values of parameters which do not allow oscillations for the deterministic system. We also study the appearance of a new equilibrium point and new bifurcation parameters due to the noisy component.

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Control of coherence resonance by self-induced stochastic resonance in a multiplex neural network

May 23, 2019

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Yamakou E. Marius, Juergen Jost
Adaptation and Self-Organizi...

We consider a two-layer multiplex network of diffusively coupled FitzHugh-Nagumo (FHN) neurons in the excitable regime. It is shown, in contrast to SISR in a single isolated FHN neuron, that the maximum noise amplitude at which SISR occurs in the network of coupled FHN neurons is controllable, especially in the regime of strong coupling forces and long time delays. In order to use SISR in the first layer of the multiplex network to control CR in the second layer, we first cho...

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Effects of multiplicative noises on synchronization in finite $N$-unit stochastic ensembles: Augmented moment approach

January 17, 2006

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Hideo Tokyo Gakugei Univ. Hasegawa
Disordered Systems and Neura...

We have studied the synchronization in finite $N$-unit FitzHugh-Nagumo neuron ensembles subjected to additive and multiplicative noises, by using the augmented moment method (AMM) which is reformulated with the use of the Fokker-Planck equation. It has been shown that for diffusive couplings, the synchronization may be enhanced by multiplicative noises while additive noises are detrimental to the synchronization. In contrast, for sigmoid coupling, both additive and multiplica...

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Weak-noise-induced transitions with inhibition and modulation of neural oscillations

June 1, 2017

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Marius E. Yamakou, Jürgen Jost
Dynamical Systems

We analyze the effect of weak-noise-induced transitions on the dynamics of the FitzHugh-Nagumo neuron model in a bistable state consisting of a stable fixed point and a stable unforced limit cycle. Bifurcation and slow-fast analysis give conditions on the parameter space for the establishment of this bi-stability. In the parametric zone of bi-stability, weak-noise amplitudes may strongly inhibit the neuron's spiking activity. Surprisingly, increasing the noise strength leads ...

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Simulating brain rhythms using an ODE with stochastically varying coefficients

June 7, 2020

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Benjamin Ambrosio, Lai-Sang Young
Dynamical Systems
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The brain produces rhythms in a variety of frequency bands. Some are likely by-products of neuronal processes; others are thought to be top-down. Produced entirely naturally, these rhythms have clearly recognizable beats, but they are very far from periodic in the sense of mathematics. They produce signals that are broad-band, episodic, wandering in magnitude, in frequency and in phase; the rhythm comes and goes, degrading and regenerating. Rhythms with these characteristics ...

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Synchrony suppression in ensembles of coupled oscillators via adaptive vanishing feedback

May 19, 2013

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Ghazal Montaseri, Mohammad Javad Yazdanpanah, ... , Rosenblum Michael
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Synchronization and emergence of a collective mode is a general phenomenon, frequently observed in ensembles of coupled self-sustained oscillators of various natures. In several circumstances, in particular in cases of neurological pathologies, this state of the active medium is undesirable. Destruction of this state by a specially designed stimulation is a challenge of high clinical relevance. Typically, the precise effect of an external action on the ensemble is unknown, si...

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Synchronised firing induced by network dynamics in excitable systems

June 29, 2012

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Claudio J. Tessone, Damián H. Zanette
Statistical Mechanics
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We study the collective dynamics of an ensemble of coupled identical FitzHugh--Nagumo elements in their excitable regime. We show that collective firing, where all the elements perform their individual firing cycle synchronously, can be induced by random changes in the interaction pattern. Specifically, on a sparse evolving network where, at any time, each element is connected with at most one partner, collective firing occurs for intermediate values of the rewiring frequency...

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Noise-induced inhibitory suppression of malfunction neural oscillators

August 3, 2005

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C. J. Tessone, E. Ullner, A. A. Zaikin, ... , Toral R.
Disordered Systems and Neura...

Motivated by the aim to find new medical strategies to suppress undesirable neural synchronization we study the control of oscillations in a system of inhibitory coupled noisy oscillators. Using dynamical properties of inhibition, we find regimes when the malfunction oscillations can be suppressed but the information signal of a certain frequency can be transmitted through the system. The mechanism of this phenomenon is a resonant interplay of noise and the transmission signa...

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