In a bistable FitzHugh-Nagumo neuron, genuine inverse stochastic resonance occurs when the quasi-potential barrier for leaving the spiking state exceeds that for leaving the resting state, provided the fitted noise exponent is negative.
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Analysis of inverse stochastic resonance: Effects of neural excitability and timescale separation
In a bistable FitzHugh-Nagumo neuron, genuine inverse stochastic resonance occurs when the quasi-potential barrier for leaving the spiking state exceeds that for leaving the resting state, provided the fitted noise exponent is negative.