$-(\mathrm{J\_fi}+\mathrm{J\_so}+\mathrm{J\_si}+\mathrm{J\_stim})$ $\mathrm{V\_0}+u(\mathrm{V\_fi}-\mathrm{V\_0})$ $\begin{cases}-1 & \text{if $(\mathrm{time\_}\ge 100)\land (\mathrm{time\_}\le 101)$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $u< \mathrm{u\_m}$}\\ 1 & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $u< \mathrm{u\_p}$}\\ 1 & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $u< \mathrm{u\_q}$}\\ 1 & \text{otherwise}\end{cases}$ $\begin{cases}0.006 & \text{if $\mathrm{epi}=1$}\\ 0.024 & \text{if $\mathrm{endo}=1$}\\ 0.1 & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $u< \mathrm{u\_r}$}\\ 1 & \text{otherwise}\end{cases}$ $\begin{cases}0.006 & \text{if $\mathrm{epi}=1$}\\ 0.006 & \text{if $\mathrm{endo}=1$}\\ 0.005 & \text{otherwise}\end{cases}$ $\frac{(1-m)(\mathrm{v\_inf}-v)}{\mathrm{tau\_v\_minus}}-\frac{mv}{\mathrm{tau\_v\_plus}}$ $\begin{cases}1 & \text{if $u< \mathrm{u\_q}$}\\ 0 & \text{otherwise}\end{cases}$ $q\mathrm{tau\_v2\_minus}-1\mathrm{tau\_v1\_minus}$ $\begin{cases}60 & \text{if $\mathrm{epi}=1$}\\ 75 & \text{if $\mathrm{endo}=1$}\\ 80 & \text{otherwise}\end{cases}$ $\begin{cases}1150 & \text{if $\mathrm{epi}=1$}\\ 10 & \text{if $\mathrm{endo}=1$}\\ 1.45 & \text{otherwise}\end{cases}$ $\frac{-mv(u-\mathrm{u\_m})(\mathrm{u\_u}-u)}{\mathrm{tau\_fi}}$ $\begin{cases}0.11 & \text{if $\mathrm{epi}=1$}\\ 0.104 & \text{if $\mathrm{endo}=1$}\\ 0.078 & \text{otherwise}\end{cases}$ $\begin{cases}1.55 & \text{if $\mathrm{epi}=1$}\\ 1.56 & \text{if $\mathrm{endo}=1$}\\ 1.61 & \text{otherwise}\end{cases}$ $\frac{u(1-p)}{\mathrm{tau\_o}}+\frac{p}{\mathrm{tau\_so}}$ $1\mathrm{tau\_o1}+r\mathrm{tau\_o2}$ $\begin{cases}400 & \text{if $\mathrm{epi}=1$}\\ 470 & \text{if $\mathrm{endo}=1$}\\ 410 & \text{otherwise}\end{cases}$ $\begin{cases}6 & \text{if $\mathrm{epi}=1$}\\ 6 & \text{if $\mathrm{endo}=1$}\\ 7 & \text{otherwise}\end{cases}$ $\mathrm{tau\_so1}+\frac{(\mathrm{tau\_so2}-\mathrm{tau\_so1})(1+\tanh (\mathrm{k\_so}(u-\mathrm{u\_so})))}{2}$ $\begin{cases}30.02 & \text{if $\mathrm{epi}=1$}\\ 40 & \text{if $\mathrm{endo}=1$}\\ 91 & \text{otherwise}\end{cases}$ $\begin{cases}0.996 & \text{if $\mathrm{epi}=1$}\\ 1.2 & \text{if $\mathrm{endo}=1$}\\ 0.8 & \text{otherwise}\end{cases}$ $\begin{cases}2.046 & \text{if $\mathrm{epi}=1$}\\ 2 & \text{if $\mathrm{endo}=1$}\\ 2.1 & \text{otherwise}\end{cases}$ $\begin{cases}0.65 & \text{if $\mathrm{epi}=1$}\\ 0.65 & \text{if $\mathrm{endo}=1$}\\ 0.6 & \text{otherwise}\end{cases}$ $\frac{(1-r)(\mathrm{w\_inf}-w)}{\mathrm{tau\_w\_minus}}-\frac{rw}{\mathrm{tau\_w\_plus}}$ $1(1-\frac{u\times 1}{\mathrm{tau\_winf}})+r\mathrm{wstar\_inf}$ $\begin{cases}0.07 & \text{if $\mathrm{epi}=1$}\\ 0.0273 & \text{if $\mathrm{endo}=1$}\\ 0.01 & \text{otherwise}\end{cases}$ $\begin{cases}0.94 & \text{if $\mathrm{epi}=1$}\\ 0.78 & \text{if $\mathrm{endo}=1$}\\ 0.5 & \text{otherwise}\end{cases}$ $\mathrm{tau\_w1\_minus}+\frac{(\mathrm{tau\_w2\_minus}-\mathrm{tau\_w1\_minus})(1+\tanh (\mathrm{k\_w\_minus}(u-\mathrm{u\_w\_minus})))}{2}$ $\begin{cases}60 & \text{if $\mathrm{epi}=1$}\\ 6 & \text{if $\mathrm{endo}=1$}\\ 70 & \text{otherwise}\end{cases}$ $\begin{cases}15 & \text{if $\mathrm{epi}=1$}\\ 140 & \text{if $\mathrm{endo}=1$}\\ 8 & \text{otherwise}\end{cases}$ $\begin{cases}65 & \text{if $\mathrm{epi}=1$}\\ 200 & \text{if $\mathrm{endo}=1$}\\ 200 & \text{otherwise}\end{cases}$ $\begin{cases}0.03 & \text{if $\mathrm{epi}=1$}\\ 0.016 & \text{if $\mathrm{endo}=1$}\\ 0.016 & \text{otherwise}\end{cases}$ $\begin{cases}200 & \text{if $\mathrm{epi}=1$}\\ 280 & \text{if $\mathrm{endo}=1$}\\ 280 & \text{otherwise}\end{cases}$ $\frac{\frac{1+\tanh (\mathrm{k\_s}(u-\mathrm{u\_s}))}{2}-s}{\mathrm{tau\_s}}$ $1\mathrm{tau\_s1}+p\mathrm{tau\_s2}$ $\begin{cases}16 & \text{if $\mathrm{epi}=1$}\\ 2 & \text{if $\mathrm{endo}=1$}\\ 4 & \text{otherwise}\end{cases}$ $\frac{-pws}{\mathrm{tau\_si}}$ $\begin{cases}1.8875 & \text{if $\mathrm{epi}=1$}\\ 2.9013 & \text{if $\mathrm{endo}=1$}\\ 3.3849 & \text{otherwise}\end{cases}$