A modified Morris-Lecar model with gM and gAHP (Yang et al., 2022)
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<html> <body> <h2>Initial conductance density values:</h2> GD_gsubNa=3p3_gL=fitted.mat - initial conductance values for Figure 4<br> GD_gsubNa=3p5_gsubK=p7_gM=1p75_gAHP=p5_gL=2_stdev=0.1_300mdls.mat - initial conductance values for Figure 5-10<br> <h2>Istim (fast fluctuating signal):</h2> fast_signal_mu_40_std=10p5_length=1p5sec.mat - the Istim (fast fluctuating signal) used for measuring firing rate <h2>Target ranges:</h2> output_target_values.mat - target ranges for outputs— firing rate, energy efficiency, input resistance, etc. <h2>Simulations:</h2> gridsearch.m<br> feedback_control.m <br> feedback_control_dg.m <br> P_control.m - Runs proportional feedback control without noise<br> P_control_dg.m - Modified from P_control.m to add noise (dg) <br> ML_HH_adapt.m - Calculates V based on the input (gi’s) and returns spike timing<br> ML_HH_adapt_ver2.m - Modified from ML_HH_adapt.m to calculate FR and energy consumption rate<br> Rheo_ML_HH_JY.m - Modified from ML_HH_adapt.m to calculate rheobase<br> Vrest_Rinput_ML_HH.m - Modified from ML_HH_adapt.m to calculate Vrest and input resistance<br> calc_EE.m - Modified from ML_HH_adapt.m to calculate energy efficiency<br> calc_fmin.m - Modified from ML_HH_adapt.m to calculate minimum frequency<br> find_inter.m - Returns the intersection of two surfaces<br> round_JY.m - Round to two decimal places<br> <h2>Figures:</h2> figure3E_H.m - Reproduces Figure3E-H, but can be modified to reproduce contour plots and iso-output1 contour vs. output2 plots in Figure 3A-D<br> figure4.m - Reproduces Figure 4<br> figure5.m - Reproduces Figure 5D, which is essentially equal to a combination of Figure 5A-C<br> figure6-10.m - Reproduces Figure 6, but can be modified to reproduce 3D plots of iso-output surfaces, conductance trajectories and correlation matrices in Figures 7-10 </body> </html>
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A modified Morris-Lecar model with gM and gAHP (Yang et al., 2022)
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