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This article is part of the supplement: Eighteenth Annual Computational Neuroscience Meeting: CNS*2009

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Frequency control in neuronal oscillators using colored noise

Roberto F Galán

Author Affiliations

Department of Neurosciences, Case Western Reserve University, Cleveland, Ohio 44106, USA

BMC Neuroscience 2009, 10(Suppl 1):P252  doi:10.1186/1471-2202-10-S1-P252

The electronic version of this article is the complete one and can be found online at:

Published:13 July 2009

© 2009 Galán; licensee BioMed Central Ltd.


It is well-known that the natural frequency of nonlinear oscillators, like neurons, can be strongly affected when driven by a periodic force or when embedded in a network [1]. In contrast, the effects of stochastic forces on the frequency of nonlinear oscillators are incompletely understood. In this context, we have mathematically investigated how colored noise and its amplitude affect the firing frequency of neurons. Our result suggests that low-amplitude colored noise may be used in deep-brain stimulation protocols to control neuronal excitability efficiently.


The dynamics of a neuron firing spikes (or bursts) regularly can be studied in terms of a phase oscillator model [2], in which the temporal evolution of the phase, φ of the membrane potential between successive spikes is given by

where ω0 is the firing frequency (in radians per second) resulting from tonic inputs that arise from the DC component of input currents (synaptic or directly injected); Z(φ) is the phase-response curve of the neuron, also known as phase sensitivity; and I(t) is a zero-mean, fluctuating component of the input currents. Here we consider I(t) to be colored noise with autocorrelation time, τ, i.e., the autocorrelation function of I(t) decays as:

where σ2 is the variance of the colored noise, and the brackets denote averaging in time.


We can show mathematically that for a sinusoidal phase-response curve, Z(φ) which is a first approximation to the phase response observed in real and simulated neurons [2], the average frequency change due to the colored noise is:

Note that the average frequency change is always negative, indicating that the colored noise lowers the natural frequency of the oscillator. In the white-noise limit (τ→0), the net frequency change goes to zero. In the limit of slowly varying inputs (τ→∞), the net frequency change is -σ2/(2ω0). Thus, by combining the amplitude and time constant of the noise, one obtains a wide range for frequency control. This may have important implications for deep brain stimulation, in particular, to efficiently decrease neuronal excitability in hyperactive areas (e.g., the focus of an epileptic seizure) with minimal current injection.


This work has been supported by The Mount Sinai Health Care Foundation.


  1. Haken H: Advanced Synergetics: Instability Hierarchies of Self-Organizing Systems and Devices. Springer Series in Synergetics: Springer Verlag; 1983. OpenURL

  2. Galán RF, Ermentrout GB, Urban NN: Efficient estimation ofphase-resetting curves in real neurons and its significance forneural-network modeling.

    Phys Rev Lett 2005, 94:158101-158105. PubMed Abstract | Publisher Full Text | PubMed Central Full Text OpenURL