MIT Press

Figure 5:

Test data generated using the Connor-Stevens model with g¯A=0mScm-2. (Top) Current clamp experiment with a decreasing ramp of the current Iapp. (Bottom) Data used to evaluate the cost function, where points for which V>Vmax are removed. Vs is obtained by filtering V with a first-order linear low-pass filter and reset to Vs,r after every spike, and Iion is evaluated using these V and Vs.

Test data generated using the Connor-Stevens model with ${\bar{g}}_{A} = 0 mS {cm}^{- 2}$ ⁠. (Top) Current clamp experiment with a decreasing ramp of the current $I_{app}$ ⁠. (Bottom) Data used to evaluate the cost function, where points for which $V > V_{max}$ are removed. $V_{s}$ is obtained by filtering $V$ with a first-order linear low-pass filter and reset to $V_{s, r}$ after every spike, and $I_{ion}$ is evaluated using these $V$ and $V_{s}$ ⁠.

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