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-1] (Φ+ 1a), where ε is a small positional displacement (Ref.). If we choose ε = log a+1 (1+ε ), then we have the affine linear PRC Δ (Φ) =Φ (Φ+ 1 a ), which is approximated by Eq. when a is large. In addition, PRCs for the leaky integrate-and-fire neuron model are approximately affine linear when the ratio of the oscillator period and membrane time constant is small (Ref.).
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