# Stochastic Phenomena in One-Dimensional Rulkov Model of Neuronal Dynamics

Authors: Irina Bashkirtseva
Journal: Discrete Dynamics in Nature and Society
 (2015)

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## Abstract

We study the nonlinear Rulkov map-based neuron model forced by random disturbances. For this model, an overview of the variety of stochastic regimes is given. For the parametric analysis of these regimes, the stochastic sensitivity functions technique is used. In a period-doubling zone, we analyze backward stochastic bifurcations modelling changes of modality of noisy neuron spiking. Noise-induced
transitions in a zone of bistability are considered. It is shown how such random transitions can generate a new neuronal regime of the stochastic bursting and transfer the system from order to chaos. A transient zone of values of noise intensity corresponding to the onset of noise-induced bursting and chaotization is localized by the stochastic sensitivity functions technique.


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## Body

## 1. Introduction

Since the pioneering work of Hodgkin and Huxley [1], neuron models attract attention of many researchers [2]. Continuous-time systems for modeling of the excitable neuron systems are widely studied. Various regimes such as spiking, bursting, fast-slow dynamics, and Canard oscillations are subject to the active investigation on the base of continuous-time models of Hindmarsh-Rose, FitzHugh-Nagumo, Morris-Lecar, and others.Discrete-time dynamical neuron models began to be studied only recently [3, 4]. Rulkov system [5] is one of the discrete models which adequately reflect main phenomenological features of neuronal dynamics. The simple two-dimensional Rulkov map-based model exhibits three main types of neural activity, such as quiescence, tonic spiking, and bursting [6, 7]. Note that it is impossible to model bursting in a framework of two-dimensional continuous-time systems.Random noise is an inevitable attribute of any living system. In presence of stochastic disturbances, nonlinear system can exhibit unexpected regimes of dynamics which have no analogue in the deterministic case [8–12]. An analysis of noise-induced phenomena in neuron models is a challenging problem of the modern neurodynamics [13, 14].Full description of the dynamics of the probabilistic distribution is given by Fokker-Planck-Kolmogorov equation [15] for continuous-time systems and by Frobenius-Perron equation [16] for discrete systems. An analytical solution of these equations is possible only in very special cases. So, for the investigation of stochastic dynamics, a method of direct numerical simulation is widely used. This method is a time-consuming for the parametric analysis. Thus, a development of the asymptotic approximations is a highly relevant area of research. For the constructive analysis of the stochastic attractors of dynamical systems, a stochastic sensitivity functions technique was elaborated [17–19].In the present paper, we consider one-dimensional Rulkov model of the neuronal dynamics [5]. Even in the deterministic case, this model possesses a wide variety of dynamical regimes and bifurcations, such as regular and chaotic attractors, multistability, bifurcations of period-doubling, and crisis [3]. In particular, Rulkov model exhibits transitions from quiescence to spiking regime, both tonic (periodic) and chaotic. However, this deterministic system still cannot model the neuronal bursting. In what follows, we show how the neuronal bursting appears in presence of noise.In current paper for in Rulkov model, we study stochastic deformations of the spiking regime and suggest a constructive method for parametric analysis of the noise-induced bursting.In Section2, after the short overview of the deterministic attractors and bifurcations, we present stochastic phenomena in this model. Along with quantitative changes of the random states’ dispersion, increasing noise generates qualitative transformations of stochastic dynamics. In the stochastic Rulkov model, noise-induced transitions and stochastic bifurcations are observed. In particular, it is shown how random transitions between stable equilibrium and chaotic attractor cause noise-induced bursting.For the parametric analysis of these phenomena, the stochastic sensitivity functions technique and confidence domains method are used in Section3. Here, backward bifurcations of reducing of the multiplicity of stochastic cycles, and noise-induced bursting with transitions from order to chaos are studied.


## 2. Stochastic Phenomena in Rulkov Model

Consider a stochastic Rulkov system:(1)
x
t
+
1
=
α
1
+
x
t
2
+
γ
+
ɛ
ξ
t
,where x is a membrane voltage in a neuron and γ is a gating-ion concentration. Random fluctuations in γ are modelled by the uncorrelated Gaussian process ξ
t with parameters E
(
ξ
t
)
=
0
,
E
(
ξ
t
2
)
=
1; ɛ is the noise intensity.The deterministic system (1) (with ɛ
=
0 wherein) was introduced in [5] as a fast part of two-dimensional fast-slow system modeling bursting. In the present paper, we fix the parameter α
=
4.1 and vary the parameter γ.In Figure1, attractors of the deterministic Rulkov model are shown for -
5
<
γ
<
1. As one can see, this one-dimensional simple model demonstrates a wide variety of dynamical regimes. Denote γ
1
=
-
4.162, γ
2
=
-
3.3, γ
3
=
-
2.849,  and γ
4
=
-
2.729. In the interval -
5
<
γ
<
γ
4, the system has a stable equilibrium M
1 (see lower curve in Figure 1). Points γ
1 and γ
4 mark the saddle-node bifurcations. When the parameter γ passes γ
1 from the left to right, a stable equilibrium M
2 and unstable equilibrium M
3 are born. Unstable equilibrium M
3 is shown for γ
1
<
γ
<
γ
4 by red dashed line. At γ
=
γ
4, the equilibria M
1 and M
3 merge and annihilate.Figure 1
Attractors of the deterministic Rulkov model.Forγ
1
<
γ
<
γ
2 (see upper part in Figure 1), the deterministic Rulkov model exhibits standard Feigenbaum’s bifurcation “tree” with period doubling and intermittency of order and chaos. Similar tree of attractors is plotted in upper part of Figure 1 for γ
4
<
γ
<
1. These trees are separated by the interval (
γ
2
,
γ
3
) with boundary points γ
2 and γ
3 which mark crises. System is monostable for (
-
5
,
γ
1
)
∪
(
γ
2
,
γ
3
)
∪
(
γ
4
,
1
) and bistable for (
γ
1
,
γ
2
)
∪
(
γ
3
,
γ
4
).So, the deterministic Rulkov map-based system (1) can model the following basic regimes of neuronal activity: quiescence (equilibrium), tonic spiking (cycles), and chaotic spiking (chaotic attractors). Consider further how noise affects these regimes of neuronal activity.Under stochastic disturbances the solutions of system (1) leave the deterministic attractors and form some stationary probabilistic distributions around them. In Figure 2, random states x
t, (
t
=
1001
,
…
,
1200
) of system (1) solutions starting from x
0
=
0 are plotted for different values of the noise intensity. Weak noise slightly washes out the thin structure of deterministic attractors (see Figure 2(a) for ɛ
=
0.003). As noise intensity increases, a dispersion of random states grows. Along with quantitative changes of the dispersion, increasing noise implies qualitative transformations of stochastic dynamics.Figure 2
Random states of stochastic Rulkov model for (a)ɛ
=
0.003, (b) ɛ
=
0.01, (c) ɛ
=
0.04, and (d) ɛ
=
0.1.
(a)
(b)
(c)
(d)First, branches of multiple cycles merge. For example, forɛ
=
0.01, the only stochastic 2 cycles can be seen (Figure 2(b)). In Figure 2(c), for ɛ
=
0.04, the upper attractor looks like the stochastic equilibrium.Second, in the zone of bistability, noise-induced transitions between attractors occur. In this zone, the lower attractor (stable equilibrium) coexists with the upper attractor (regular or chaotic). In spite of the fact that the initial statex
0
=
0 belongs to basin of attraction of the upper attractor, under the random disturbances with superthreshold intensity, random trajectories jump across the separatrix and localize near the lower stable equilibrium (Figures 2(c) and 2(d)). As a result, random states leave a basin of attraction of the upper attractor and localize near the stable equilibrium M
1 (see Figure 2(d)). Such transition can be interpreted as noise-induced transformation from spiking regime to quiescence.It is worth noting that such one-way transitions downwards occur only in the left interval(
γ
1
,
γ
2
) of the bistability zone. For the right interval (
γ
3
,
γ
4
), mutual transitions are observed. In Figure 3 for γ
=
-
2.8, it is shown how separate deterministic attractors, equilibrium (lower) and chaotic (upper) (Figure 3(a)), combine into a single stochastic attractor (Figure 3(b)) under the noise of the intensity ɛ
=
0.15. Such transformation has an important interpretation from neuron activity point of view. Indeed, here noise generates a new bursting regime. Note that in the framework of the deterministic Rulkov model, more simple regimes of silence and spiking (periodic or chaotic) are observed only.Figure 3
Time series for Rulkov model withγ
=
-
2.8: (a) ɛ
=
0, and (b) ɛ
=
0.15.
(a)
(b)Stochastic phenomena, presented here on the base of direct numerical simulation, are studied in the next section with the help of the stochastic sensitivity function technique.


## 3. SSF Analysis of Stochastic Bifurcations

For the analysis of the dispersions of the random states, the approximations (see Appendix for details) based on the stochastic sensitivity functions technique are used.In Figure4, the stochastic sensitivity for equilibria and cycles is shown. The stochastic sensitivity function w
(
μ
) is plotted in Figure 4(a) for the equilibria M
1
(
μ
) (blue color) and M
2
(
μ
) (red color). As one can see, the stochastic sensitivity varies greatly at the edges of intervals of structural stability. Approaching the bifurcation points, this function unlimitedly increases.Figure 4
Stochastic sensitivity functions: (a) for equilibriaM
1, M
2, (b) for 2 cycles, and (c) for 4 cycles.
(a)
(b)
(c)The branches of the stochastic sensitivity function for the points of 2 cycles and 4 cycles are plotted in Figures4(b) and 4(c). It can be seen that different points of the cycle have a different response on the random disturbances. Details of this difference are clearly observed with the help of the probability density function. In Figure 5, plots of the probability density function are shown for 2 cycles of system (1) with γ
=
-
3.9 and three values of the noise intensity: ɛ
=
0.003 (red), ɛ
=
0.007 (green), and ɛ
=
0.02 (blue). Curves in Figure 5(a) were obtained by direct numerical simulation. In Figure 5(b), these curves were calculated by the formula (A.17) using the stochastic sensitivity function. A difference in the stochastic sensitivity of 2-cycle states implies the difference in the height and width of the peaks of the probability.Figure 5
Backward stochastic bifurcation forγ
=
-
3.9. Probability density functions for ɛ
=
0.003 (red), ɛ
=
0.007 (green), and ɛ
=
0.02 (blue).
(a)
(b)Consider a variation of the form of these peaks under increasing noise. For weak noise (ɛ
=
0.003), a curve of the probability density function ρ
(
x
) has two narrow peaks. As the noise intensity increases, a process of merging of these peaks is observed. As one can see, a local minimum of ρ
(
x
) increases but the general graphic shape remains bimodal and a number of local extreme points equals three. For some threshold value ɛ, a qualitative change of the shape of ρ
(
x
) occurs. A form of this curve becomes unimodal. Two separate peaks transform into one and the only maximum remains, and stochastic 2 cycles look like a stochastic equilibrium. Such transformation of ρ
(
x
) from bimodal to unimodal form can be specified as a backward stochastic bifurcation. Similar transformation is observed for 4 cycles too. In Figure 6, it is shown how the backward stochastic bifurcation “4 cycles → 2 cycles” occurs. Plots in Figure 6(a) were extracted from the extensive direct numerical simulations and, in Figure 6(b), were found with the help of the analytical approximation (A.17).Figure 6
Backward stochastic bifurcation forγ
=
-
3.74. Probability density functions for ɛ
=
0.003 (red) and ɛ
=
0.02 (blue).
(a)
(b)It is worth noting that SSF technique allows us to analyze parametrically backward stochastic bifurcations for the multiple cycles. Such analysis is important for the understanding of the probabilistic mechanism of the stochastic deformation of the modality for the spiking regime.In what follows, we show how this technique can be used for the study of noise-induced bursting.


## 4. Noise-Induced Bursting and Transition to Chaos

Consider Figure3 again. In Figure 3(a), two separated attractors of the deterministic model (stable equilibrium and chaotic attractor) present two coexisting regimes of neuronal activity (quiescence and spiking). In Figure 3(b), a new well-mixed joined stochastic attractor models the bursting regime in system (1) for the noise intensity ɛ
=
0.15. Now, consider details of such transformation.In Figure7, random states (grey color) of Rulkov model with γ
=
-
2.8 around the stable equilibrium (blue solid line) are plotted for the noise intensity 0
≤
ɛ
≤
0.2.Figure 7
Noise-induced bursting (a) and noise-induced chaotization (b) forγ
=
-
2.8.
(a)
(b)For smallɛ, a linear growth of the dispersion is observed. It can be seen that there exists some transient zone of noise intensity values where the dispersion of random states abruptly grows. In this zone, random solutions of system (1) with high probability can cross the separatrix (unstable equilibrium, red line) and form bursting oscillations. Using SSF technique, we can estimate a position of this transient zone.Boundaries of the confidence intervals around the stable equilibriumM
1 have been found by (A.8) and presented in Figure 7 by dashed lines. A point of the intersection of the upper boundary with the separatrix allows us to approximate a location of the transient zone of the onset of the bursting. As one can see, our theoretical method of the localization of the transient zone where the bursting oscillations appear is in a good agreement with results of the direct numerical simulations.Consider now how these qualitative changes in the stochastic dynamics of the Rulkov model are connected with the changes in the largest Lyapunov exponentΛ. The largest Lyapunov exponent is a generally used quantitative characteristics for both deterministic and stochastic systems. The change of the sign of the largest Lyapunov exponent is a criterion of the transition from order to chaos [11, 20–22].In Figure7(b), a curve of the function Λ
(
ɛ
) is plotted for the Rulkov model with γ
=
-
2.8. As noise intensity increases, a transition from the small-amplitude oscillations to large-amplitude bursts is accompanied by the change of the sign of Λ from negative to positive. Such change of the sign of Λ can be explained by the fact that the stochastic system spends a lot of time near the unstable equilibrium M
3 where the divergence dominates. In the transient zone, the fastest growth of Λ
(
ɛ
) is observed.So, the noise-induced bursting in the Rulkov model is accompanied by the transition from order to chaos.



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*Source: 495417-2015-04-14.xml*