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Alexander Ororbia
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tweak to img folder for sindy
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docs/museum/sindy.md

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# Sparse Identification of Non-linear Dynamical Systems (SINDy)[1]
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# Sparse Identification of Non-linear Dynamical Systems (SINDy)
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In this section, we will study, create, simulate, and visualize a model known as the sparse identification of non-linear dynamical systems (SINDy) [1], implementing it in NGC-Learn and JAX. After going through this demonstration, you will:
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docs/tutorials/neurocog/hodgkin_huxley_cell.md

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$$
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\tau_v \frac{\partial \mathbf{v}_t}{\partial t} &= \mathbf{j}_t - g_Na * \mathbf{m}^3_t * \mathbf{h}_t * (\mathbf{v}_t - v_Na) - g_K * \mathbf{n}^4_t * (\mathbf{v}_t - v_K) - g_L * (\mathbf{v}_t - v_L) \\
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\frac{\partial \mathbf{n}_t}{\partial t} &= alpha_n(\mathbf{v}_t) * (1 - \mathbf{n}_t) - beta_n(\mathbf{v}_t) * \mathbf{n}_t \\
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\frac{\partial \mathbf{m}_t}{\partial t} &= alpha_m(\mathbf{v}_t) * (1 - \mathbf{m}_t) - beta_m(\mathbf{v}_t) * \mathbf{m}_t \\
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\frac{\partial \mathbf{h}_t}{\partial t} &= alpha_h(\mathbf{v}_t) * (1 - \mathbf{h}_t) - beta_h(\mathbf{v}_t) * \mathbf{h}_t
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\frac{\partial \mathbf{n}_t}{\partial t} &= \alpha_n(\mathbf{v}_t) * (1 - \mathbf{n}_t) - \beta_n(\mathbf{v}_t) * \mathbf{n}_t \\
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\frac{\partial \mathbf{m}_t}{\partial t} &= \alpha_m(\mathbf{v}_t) * (1 - \mathbf{m}_t) - \beta_m(\mathbf{v}_t) * \mathbf{m}_t \\
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\frac{\partial \mathbf{h}_t}{\partial t} &= \alpha_h(\mathbf{v}_t) * (1 - \mathbf{h}_t) - \beta_h(\mathbf{v}_t) * \mathbf{h}_t
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$$
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where we observe that the above four-dimensional set of dynamics is composed of nonlinear ODEs. Notice that, in each gate or channel probability ODE, there are two generator functions (each of which is a function of the membrane potential $\mathbf{v}_t$) that produces the necessary dynamic coefficients at time $t$; $\alpha_x(\mathbf{v}_t)$ and $\beta_x(\mathbf{v}_t)$ produce different biopphysical weighting values depending on which channel $x = \{n, m, h\}$ they are related to.

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