2013
DOI: 10.1007/s00422-013-0559-1
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Symmetric bursting behaviors in the generalized FitzHugh–Nagumo model

Abstract: In the current paper, we have investigated the generalized FitzHugh-Nagumo model. We have shown that symmetric bursting behaviors of different types could be observed in this model with an appropriate recovery term. A modified version of this system is used to construct bursting activities. Furthermore, we have shown some numerical examples of delayed Hopf bifurcation and canard phenomenon in the symmetric bursting of super-Hopf/homoclinic type near its super-Hopf and homoclinic bifurcations, respectively.

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Cited by 21 publications
(8 citation statements)
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“…Abstractly, one may think of our (effective) “third equation” as the integrated effects resulting from coupling the center cell to the rest of the cable. Unlike other conventional models for bursting [ 37 , 38 ], we find bursting to arise in this intrinsically two-variable system through coupling of the cell to an extended system. Interestingly, it has previously been pointed out that within a three-variable model bursting may emerge as a similarly transient phenomenon before the system settles into periodic spiking.…”
Section: Resultscontrasting
confidence: 73%
“…Abstractly, one may think of our (effective) “third equation” as the integrated effects resulting from coupling the center cell to the rest of the cable. Unlike other conventional models for bursting [ 37 , 38 ], we find bursting to arise in this intrinsically two-variable system through coupling of the cell to an extended system. Interestingly, it has previously been pointed out that within a three-variable model bursting may emerge as a similarly transient phenomenon before the system settles into periodic spiking.…”
Section: Resultscontrasting
confidence: 73%
“…A more convenient and complete classification of bursters was proposed by Izhikevich, who suggested to name bursters according to the two bifurcations occurring in the fast subsystem that lead to the appearance and disappearance of repetitive spiking in the review [Izhikevich, 2000], where 12 codimension-1 bifurcations of a quiescent state that lead to repetitive spiking and 10 codimension-1 bifurcations of a spiking attractor that lead to quiescence were summed up, which thus gave rise to 120 different types of codimension-1 fast-slow bursters. By now, Izhikevich's classification method has been widely used in bursting research, see [Abbasian et al, 2013;Duan et al, 2008;Lu et al, 2008;Lu et al, 2009;Straube et al, 2006;Wagemakers et al, 2006;Zhang et al, 2013] for example.…”
Section: Introductionmentioning
confidence: 99%
“…Some mathematical models for biological neurons which represent neuronal behavior in terms of membrane potentials have been developed such as Hodgkin-Huxley model (1952), FitzHugh model (1969), Morris-Lecar model (1981), Hindmarsh-Rose model (1984), especially Hodgkin-Huxley model which is the motivation for the FitzHugh-Nagumo equation that extracts the essential behavior in a simple form [1][2][3]. A. Yazdan, G. Mehrdad and M. Ghasem have used the cellular automata method to simulate the pattern formation of FitzHugh-Nagumo model and considered the effects of different parameters of the FitzHugh-Nagumo model on changing the initial pattern [4].…”
Section: Introductionmentioning
confidence: 99%