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An excitable electronic circuit as a sensory neuron model
Biological Physics · Submitted 3 Oct 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim An electronic circuit device, inspired on the FitzHugh-Nagumo model of neuronal excitability, was constructed and shown to operate with characteristics compatible with those of biological sensory neurons.
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The abstract, sentence by sentence
An electronic circuit device, inspired on the FitzHugh-Nagumo 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.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | An electronic circuit device, inspired on the FitzHugh-Nagumo model of neuronal excitability, was constructed and shown to operate with characteristics compatible with those of biological sensory neurons. | contribution 0.95 | 0.94 | 0.79 | asserted 0.93 |
| s1 | 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. | result 0.87 | 0.90 | 0.12 | asserted 1.00 |
| s2 | Moreover, we have implemented an analog noise generator as a source to study the variability of the spike trains. | method 0.90 | 0.95 | 0.04 | asserted 1.00 |
| s3 | When the circuit is in the excitable regime, coherence resonance is observed. | result 1.00 | 0.91 | 0.09 | asserted 1.00 |
| s4 | At sufficiently low noise intensity the spike trains have Poisson statistics, as in many biological neurons. | result 0.99 | 0.89 | 0.07 | asserted 1.00 |
| s5 | The transfer function of the stochastic spike trains has a dynamic range of 6 dB, close to experimental values for real olfactory receptor neurons. | result 0.98 | 0.90 | 0.13 | asserted 1.00 |
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Original abstract
An electronic circuit device, inspired on the FitzHugh-Nagumo 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.
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