An excitable electronic circuit as a sensory neuron model
An electronic circuit device, inspired on the FitzHughNagumo model of neuronal excitability, was constructed and shown to operate with characteristics compatible with those of biological sensory neurons. The nonlinear dynamical model of the electronics quantitatively reproduces the experimental obse...
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World Scientific Publishing Co. Pte Ltd
2012
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001 | PAPER-9275 | ||
003 | AR-BaUEN | ||
005 | 20230518203910.0 | ||
008 | 190411s2012 xx ||||fo|||| 00| 0 eng|d | ||
024 | 7 | |2 scopus |a 2-s2.0-84868470677 | |
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
100 | 1 | |a Medeiros, B.N.S. | |
245 | 1 | 3 | |a An excitable electronic circuit as a sensory neuron model |
260 | |b World Scientific Publishing Co. Pte Ltd |c 2012 | ||
270 | 1 | 0 | |m Medeiros, B.N.S.; Departamento de Física, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil |
506 | |2 openaire |e Política editorial | ||
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520 | 3 | |a An electronic circuit device, inspired on the FitzHughNagumo model of neuronal excitability, was constructed and shown to operate with characteristics compatible with those of biological sensory neurons. The nonlinear dynamical model of the electronics quantitatively reproduces the experimental observations on the circuit, including the Hopf bifurcation at the onset of tonic spiking. Moreover, we have implemented an analog noise generator as a source to study the variability of the spike trains. When the circuit is in the excitable regime, coherence resonance is observed. At sufficiently low noise intensity the spike trains have Poisson statistics, as in many biological neurons. The transfer function of the stochastic spike trains has a dynamic range of 6 dB, close to experimental values for real olfactory receptor neurons. © 2012 World Scientific Publishing Company. |l eng | |
536 | |a Detalles de la financiación: Conselho Nacional de Desenvolvimento Científico e Tecnológico, CNPq | ||
536 | |a Detalles de la financiación: Coordenação de Aperfeiçoamento de Pessoal de Nível Superior | ||
536 | |a Detalles de la financiación: Fundação de Amparo à Ciência e Tecnologia do Estado de Pernambuco | ||
536 | |a Detalles de la financiación: National Institutes of Health | ||
536 | |a Detalles de la financiación: B. N. S. Medeiros, M. Copelli and J. R. Rios Leite acknowledge financial support from Brazilian agencies CNPq, FACEPE, CAPES and special programs PRONEX, PRONEM and INCEMAQ. G. B. Mindlin acknowledges support from NIH. It is a pleasure to thank Hugo L. D. S. Cavalcante for enlightening discussions during the preparation of this work, as well as Marcos Nascimento for technical support. | ||
593 | |a Departamento de Física, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil | ||
593 | |a Department of Cognitive Neuroscience, University of California San Diego, San Diego, CA 92093-0515, United States | ||
593 | |a Departamento de Física, FCEN, Ciudad Universitaria, Pab. I, 1428 Buenos Aires, Argentina | ||
690 | 1 | 0 | |a COHERENCE RESONANCE |
690 | 1 | 0 | |a DYNAMIC RANGE |
690 | 1 | 0 | |a ELECTRONIC CIRCUIT |
690 | 1 | 0 | |a EXCITABLE ELEMENT |
690 | 1 | 0 | |a HOPF BIFURCATION |
690 | 1 | 0 | |a NETWORKS (CIRCUITS) |
690 | 1 | 0 | |a STOCHASTIC SYSTEMS |
690 | 1 | 0 | |a TIMING CIRCUITS |
690 | 1 | 0 | |a COHERENCE RESONANCE |
690 | 1 | 0 | |a DYNAMIC RANGE |
690 | 1 | 0 | |a EXCITABLE ELEMENT |
690 | 1 | 0 | |a EXPERIMENTAL VALUES |
690 | 1 | 0 | |a FITZHUGH-NAGUMO MODEL |
690 | 1 | 0 | |a NONLINEAR DYNAMICAL MODELS |
690 | 1 | 0 | |a OLFACTORY RECEPTOR NEURONS |
690 | 1 | 0 | |a POISSON STATISTIC |
690 | 1 | 0 | |a NEURONS |
700 | 1 | |a Minces, V. | |
700 | 1 | |a Mindlin, G.B. | |
700 | 1 | |a Copelli, M. | |
700 | 1 | |a Leite, J.R.R. | |
773 | 0 | |d World Scientific Publishing Co. Pte Ltd, 2012 |g v. 22 |k n. 10 |p Int. J. Bifurcation Chaos |x 02181274 |w (AR-BaUEN)CENRE-5216 |t International Journal of Bifurcation and Chaos | |
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