Exploring Neurological Dynamical Systems: Part 2
In my previous post on dynamic mode decomposition, I discussed the foundations of DMD as a means for linearizing a dynamical system123. In this post, I want to look at a way in which we can use rank-updates to incorporate new information into the spectral decomposition of our linear operator, $A$, in the event that we are generating online measurements from our dynamical system4 – see the citation below if you want a more-detailed overview of this topic along with open source code for testing this method.
Recall that we are given an initial data matrix
$$\begin{align}
X = \begin{bmatrix}
x_{n_{1},m_{1}} & x_{n_{1},m_{2}} & x_{n_{1},m_{3}} & … \\
x_{n_{2},m_{1}} & x_{n_{1},m_{2}} & x_{n_{2},m_{3}} & … \\
x_{n_{3},m_{1}} & x_{n_{1},m_{2}} & x_{n_{3},m_{3}} & … \\
… & … & … & … \\
\end{bmatrix}
\in R^{n \times m}
\end{align}$$
which we can split into two matrices, shifted one unit in time apart:
$$\begin{align}
X^{\ast} &=
\begin{bmatrix}
\vert & \vert & \dots & \vert \\
\vec{x}_1 & \vec{x}_2 & \dots & \vec{x}_{m-1} \\
\vert & \vert & \dots & \vert \\
\end{bmatrix} \in R^{n \times (m-1)} \\
Y &= \begin{bmatrix}
\vert & \vert & \dots & \vert \\
\vec{x}_2 & \vec{x}_3 & \dots & \vec{x}_{m} \\
\vert & \vert & \dots & \vert \\
\end{bmatrix} \in R^{n \times (m-1)}
\end{align}$$
and we are interested in solving for the linear operator $A$, such that
$$\begin{align} Y = AX^{\ast} \end{align}$$
For simplicity, since we are no longer using the full matrix, I’ll just refer to $X^{\ast}$ as $X$. In the previous post, we made the constraint that $n > m$, and that rank($X$) $\leq m < n$. Here, however, we’ll reverse this assumption, and such that $m > n$, and that rank($X$) $\leq m < n$, such that $XX^{T}$ is invertible, so by multiplying both sides by $X^{T}$ we have
$$\begin{align}
AXX^{T} &= YX^{T} \\
A &= YX^{T}(XX^{T})^{-1} \\
A &= QP_{x}
\end{align}$$
where $Q = YX^{T}$ and $P_{x} = (XX^{T})^{-1}$. Now, let’s say you observe some new data $x_{m+1}, y_{m+1}$, and you want to incorporate this new data into your $A$ matrix. As in the previous post on rank-one updates, we saw that directly computing the inverse could potentially be costly, so we want to refrain from doing that if possible. Instead, we’ll use the Shermann-Morrison-Woodbury theorem again to incorporate our new $x_{m+1}$ sample into our inverse matrix, just as before:
$$\begin{align} (X_{m+1}X^{T}_{m+1})^{-1} = P_{x} + \frac{P_{x}x_{m+1}x_{m+1}^{T}P_{x}}{1 + x_{m+1}^{T}P_{x}x_{m+1}} \end{align}$$
Likewise, since we’re appending new data to our $Y$ and $X$ matrices, we also have
$$\begin{align}
Y_{m+1} = \begin{bmatrix}
Y & y_{m+1} \end{bmatrix} \\
X_{m+1} = \begin{bmatrix} \\
X & x_{m+1} \end{bmatrix} \\
\end{align}$$
such that
$$\begin{align}
Y_{m+1} X_{m+1}^{T} &= YX^{T} + y_{m+1}x_{m+1}^{T} \\
&= Q + y_{m+1}x_{m+1}^{T}
\end{align}$$
which is simply the sum of our original matrix $Q$, plus a rank-one matrix. The authors go on to describe some pretty cool “local” DMD schemes, by incorporating weights, as well as binary thresholds, that are time-dependent into the computation of the linear operator, $A$.
P.J. Schmid. Dynamic mode decomposition of numerical and experimental data. Journal of Fluid Mechanics 656.1. 2010. ↩︎
Tu et al. On Dynamic Mode Decomposition: Theory And Applications ↩︎
Kunert-Graf et al. Extracting Reproducible Time-Resolved Resting State Networks Using Dynamic Mode Decomposition. Front. Comput. Neurosci. 2019. ↩︎
Zhang et al. Online dynamic mode decomposition for time-varying systems. 2017. ↩︎