2009
DOI: 10.1134/s1064226909020089
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Dynamics of two neuronlike elements with inhibitory feedback

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Cited by 14 publications
(12 citation statements)
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“…In view of the arbitrarily high dimensional critical manifolds of the RS solution, which were observed in this paper, it seems to be worth studying such computational abilities for an oscillator with delayed pulsatile feedback. An electronic implementation of such systems is relatively uncomplicated [7,42,64].…”
Section: Discussionmentioning
confidence: 99%
“…In view of the arbitrarily high dimensional critical manifolds of the RS solution, which were observed in this paper, it seems to be worth studying such computational abilities for an oscillator with delayed pulsatile feedback. An electronic implementation of such systems is relatively uncomplicated [7,42,64].…”
Section: Discussionmentioning
confidence: 99%
“…The experimental setup is described in detail in the Supplemental materials. It was based on the electronic FitzHugh-Nagumo oscillator [53,54]. When the output voltage exceeds a threshold value, a spike is produced and sent to a delay line.…”
mentioning
confidence: 99%
“…In order to simulate neural dynamics, we explored two FHN neuron generators with cubic nonlinearity constructed using diodes [ 7 , 22 ]. The dynamics of the presynaptic FHN neuron was modeled by the normalized equations obtained with the Kirchhoff law [ 21 ] as follows: where u 1 is the membrane potential of the presynaptic neuron, ν 1 is the “recovery” variable related to the ion current, f ( u 1 ) = u 1 u 1 3 /3 is the cubic nonlinearity, I 1 is the depolarization parameter characterizing the excitation threshold, and ε is a small coefficient.…”
Section: Methodsmentioning
confidence: 99%
“…The dynamics of the presynaptic FHN neuron was modeled by the normalized equations obtained with the Kirchhoff law [ 21 ] as follows: where u 1 is the membrane potential of the presynaptic neuron, ν 1 is the “recovery” variable related to the ion current, f ( u 1 ) = u 1 u 1 3 /3 is the cubic nonlinearity, I 1 is the depolarization parameter characterizing the excitation threshold, and ε is a small coefficient. If u 1 < 0, the function g ( u 1 ) = αu 1 , and if u 1 ≥ 0, g ( u 1 ) = βu 1 ( α , β being the parameters that control, respectively, the shape and location of the ν -nullcline [ 22 ]).…”
Section: Methodsmentioning
confidence: 99%
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