The-Art-of-Linear-Algebra.tex

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\begin{document}
\title{The Art of Linear Algebra\\
\vspace{5pt}
\large{
-- Graphic Notes on ``Linear Algebra for Everyone" --
}
}

\author{Kenji Hiranabe
\thanks{twitter: @hiranabe, k-hiranabe@esm.co.jp, \url{https://anagileway.com}} \\
with the kindest help of Gilbert Strang
\thanks{Massachusetts Institute of Technology, \url{http://www-math.mit.edu/\~gs/}}
}

\date{September 1, 2021/updated \today}

\maketitle

\vspace{-5pt}

\begin{abstract}
I try to intuitively visualize some important concepts introduced
in ``Linear Algebra for Everyone",\footnote{``Linear Algebra for Everyone":
\url{http://math.mit.edu/everyone/} with Japanese translation from Kindai Kagaku.}
which include Column-Row ($\bm{CR}$), Gaussian Elimination ($\bm{LU}$),
Gram-Schmidt Orthogonalization ($\bm{QR}$), Eigenvalues and Diagonalization ($\bm{Q \Lambda Q\transp}$),
and Singular Value Decomposition ($\bm{U \Sigma V\transp}$).
This paper aims at promoting the understanding of vector/matrix calculations
and algorithms from the perspective of matrix factorization.
All the artworks including the article itself are maintained under the GitHub repository \url{https://github.com/kenjihiranabe/The-Art-of-Linear-Algebra/}.
\end{abstract}

\section*{Foreword}
I am happy to see Kenji Hiranabe's pictures of matrix operations in linear algebra !
The pictures are an excellent way to show the algebra.  We can think of matrix
multiplications by row $\bm{\cdot}$ column dot products, but that is not all --  it is ``linear combinations"
and ``rank 1 matrices" that complete the algebra and the art.
I am very grateful to see the books in Japanese translation
and the ideas in Kenji's pictures.
\begin{flushright}
-- Gilbert Strang \\ Professor of Mathematics at MIT
\end{flushright}

\tableofcontents

\section{Viewing a Matrix -- 4 Ways}

A matrix ($m \times n$) can be viewed as $1$ matrix, $mn$ numbers, $n$ columns and $m$ rows.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{ViewingMatrix-4Ways.eps}\\
    \caption{Viewing a Matrix in 4 Ways}
\end{figure}


\begin{equation*}
  A= \begin{bmatrix}
    a_{11} & a_{12}\\
    a_{21} & a_{22}\\
    a_{31} & a_{32}
  \end{bmatrix}
  =
  \begin{bmatrix}
    | & |\\
    \bm{a_1} & \bm{a_2}\\
    | & |
  \end{bmatrix}
  =
  \begin{bmatrix}
    - \bm{a_1^*} -\\
    - \bm{a_2^*} -\\
    - \bm{a_3^*} -
  \end{bmatrix}
\end{equation*} \\

Here, the column vectors are in bold as $\bm{a_1}$.
Row vectors include $\bm{*}$ as in $\bm{a_1^*}$.
Transposed vectors and matrices are indicated by $\mathrm{T}$ as
in $\bm{a}\transp$ and $A\transp$.

\section{Vector times Vector -- 2 Ways}

Hereafter I point to specific sections of ``Linear Algebra for Everyone"
and present graphics which illustrate the concepts with short names
in gray circles.

\begin{itemize}
  \item Sec. 1.1 (p.2) Linear combination and dot products
  \item Sec. 1.3 (p.25) Matrix of Rank One
  \item Sec. 1.4 (p.29) Row way and column way
\end{itemize}

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{VectorTimesVector.eps}
  \caption{Vector times Vector - (v1), (v2)}
\end{figure}

(v1) is an elementary operation of two vectors, but (v2) multiplies the column to the row
and produces a rank 1 matrix. Knowing this outer product (v2) is the key to the following sections.

\section{Matrix times Vector -- 2 Ways}

A matrix times a vector creates a vector of three dot products (Mv1)
as well as a linear combination (Mv2) of the column vectors of $A$.

\begin{itemize}
  \item Sec. 1.1 (p.3) Linear combinations
  \item Sec. 1.3 (p.21) Matrices and Column Spaces
\end{itemize}

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{MatrixTimesVector.eps}
  \caption{Matrix times Vector - (Mv1), (Mv2)}
\end{figure}

At first, you learn (Mv1). But when you get used to viewing it as (Mv2),
you can understand $A\bm{x}$ as a linear combination of the columns of $A$.
Those products fill the column space of $A$  denoted as $\mathbf{C}(A)$.
The solution space of $A\bm{x}=\bm{0}$ is the nullspace of $A$ denoted as $\mathbf{N}(A)$.
To understand the nullspace, let the right-hand side of (Mv1) be $\bm{0}$
and see all the dot products are zero.

Also, (vM1) and (vM2) show the same pattern for a row vector times a matrix.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{VectorTimesMatrix.eps}
  \caption{Vector times Matrix - (vM1), (vM2)}
\end{figure}


The products fill the row space of $A$ denoted as $\mathbf{C}(A\transp)$.
The solution space of $yA=0$ is the left-nullspace of $A$, denoted as $\mathbf{N}(A\transp)$.


The four subspaces consist of $\mathbf{N}(A)$ + $\mathbf{C}(A\transp)$
(which are perpendicular to each other) in $\mathbb{R}^n$ and
$\mathbf{N}(A\transp)$ + $\mathbf{C}(A)$ in $\mathbb{R}^m$
(which are perpendicular to each other).


\begin{itemize}
  \item Sec. 3.5 (p.124) Dimensions of the Four Subspaces
\end{itemize}

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{4-Subspaces.eps}
  \caption{The Four Subspaces}
\end{figure}

See $A=CR$ (Sec 6.1) for the rank $r$.


\section{Matrix times Matrix -- 4 Ways}

``Matrix times Vector" naturally extends to ``Matrix times Matrix".

\begin{itemize}
  \item Sec. 1.4 (p.35) Four Ways to Multiply $\bm{AB=C}$
  \item Also see the back cover of the book
\end{itemize}


\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{MatrixTimesMatrix.eps}
  \caption{Matrix times Matrix - (MM1), (MM2), (MM3), (MM4)}
\end{figure}

\section{Practical Patterns}

Here, I show some practical patterns which allow you to capture
the upcoming factorizations in a more intuitive way.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{Pattern12.eps}
  \caption{Pattern 1, 2 - (P1), (P1)}
\end{figure}

Pattern 1 is a combination of (MM2) and (Mv2).
Pattern 2 is an extension of (MM3). Note that Pattern 1 is a column operation (multiplying a matrix from right),
whereas Pattern 2 is a row operation (multiplying a matrix from left).

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{Pattern11-22.eps}
  \caption{Pattern 1$^\prime$, 2$^\prime$ - (P1$^\prime$), (P2$^\prime$)}
\end{figure}

(P1$^\prime$) multiplies the diagonal numbers to the columns of the matrix,
whereas (P2$^\prime$) multiplies the diagonal numbers to the row of the matrix.
Both are variants of (P1) and (P2).

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.6]{Pattern3.eps}
  \caption{Pattern 3 - (P3)}
\end{figure}

This pattern emerges when you solve differential equations and recurrence equations:

\begin{itemize}
  \item Sec. 6 (p.201) Eigenvalues and Eigenvectors
  \item Sec. 6.4 (p.243) Systems of Differential Equations
\end{itemize}

\begin{align*}
  \frac{d \bm{u}(t) }{dt} &= A \bm{u}(t), \quad \bm{u}(0)=\bm{u}_0\\
  \bm{u}_{n+1} &= A \bm{u}_n, \quad \bm{u_0} = \bm{u}_0
\end{align*}

In both cases, the solutions are expressed with
eigenvalues ($\lambda_1, \lambda_2, \lambda_3$),
eigenvectors $X=\begin{bmatrix} \bm{x}_1 & \bm{x}_2 & \bm{x}_3 \end{bmatrix}$ of $A$, and
the coefficients $c=\begin{bmatrix} c_1 & c_2 & c_3 \end{bmatrix}\transp$
which are the coordinates of the initial condition $\bm{u}(0)=\bm{u}_0$ in terms of
the eigenvectors $X$.

\begin{equation*}
  \bm{u}_0 = c_1 \bm{x}_1 + c_2 \bm{x}_2 + c_3 \bm{x}_3
\end{equation*}
\begin{equation*}
  \bm{c} =
  \begin{bmatrix}
    c_1\\
    c_2\\
    c_3
  \end{bmatrix} = X^{-1} \bm{u}_0
\end{equation*}

and the general solution of the two equations are:

\begin{align*}
  \bm{u}(t) &= e^{At} \bm{u}_0 = X e^{\Lambda t} X^{-1} \bm{u_0} &= X e^{\Lambda t} \bm{c} &= c_1 e^{\lambda_1 t} \bm{x}_1 + c_2 e^{\lambda_2 t} \bm{x}_2 + c_3 e^{\lambda_3 t} \bm{x}_3\\
  \bm{u}_n &= A^n \bm{u}_0 = X \Lambda^n X^{-1} \bm{u_0} &= X \Lambda^n \bm{c} &= c_1 \lambda_1^n \bm{x}_1 + c_2 \lambda_2^n \bm{x}_2 + c_3 \lambda_3^n \bm{x}_3
\end{align*}

See Figure 9: Pattern 3 (P3) above again to get $XDc$.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{Pattern4.eps}
  \caption{Pattern 4 - (P4)}
\end{figure}

This pattern (P4) works in both eigenvalue decomposition and singular value decomposition.
Both decompositions are expressed as a product of three matrices with a diagonal matrix in the middle,
and also a sum of rank 1 matrices with the eigenvalue/singular value coefficients.

More details are discussed in the next section.

\clearpage

\section{The Five Factorizations of a Matrix}

\begin{itemize}
  \item Preface p.vii, The Plan for the Book.
\end{itemize}
$A=CR, A=LU, A=QR, A=Q \Lambda Q\transp, A=U \Sigma V\transp$ are
illustrated one by one.

\begin{table}[h]
  \begin{tabular}{lll}
    \Large{\boldmath $A=CR$} & \includegraphics{A_CR.eps} &
    \begin{tabular}{l}
      Independent columns in $C$\\
      Row echelon form in $R$\\
      Leads to column rank = row rank
    \end{tabular}\\

    \Large{\boldmath $A=LU$} & \includegraphics{A_LU.eps} &
    \begin{tabular}{l}
      $LU$ decomposition from\\
      Gaussian elimination\\
      (Lower triangular)(Upper triangular)
    \end{tabular}\\

    \Large{\boldmath $A=QR$} & \includegraphics{A_QR.eps} &
    \begin{tabular}{l}
      $QR$ decomposition as\\
      Gram-Schmidt orthogonalization\\
      Orthogonal $Q$ and triangular $R$
    \end{tabular}\\

    \Large{\boldmath $S=Q\Lambda Q\transp$} & \includegraphics{A_QLQT.eps} &
    \begin{tabular}{l}
      Eigenvalue decomposition\\
      of a symmetric matrix $S$\\
      Eigenvectors in $Q$, eigenvalues in $\Lambda$
    \end{tabular}\\

    \Large{\boldmath $A=U\Sigma V\transp$} & \includegraphics{A_USVT.eps} &
    \begin{tabular}{l}
      Singular value decomposition\\
      of all matrices $A$\\
      Singular values in $\Sigma$
    \end{tabular}
  \end{tabular}
  \caption{The Five Factorization}

\end{table}

\subsection{$\boldsymbol{A=CR}$}

\begin{itemize}
  \item Sec.1.4 Matrix Multiplication and $\bm{A=CR}$ (p.29)
\end{itemize}

The row rank and the column rank of a general rectangular matrix $A$ are equal.
This factorization is the most intuitive way to understand this theorem.
$C$ consists of independent columns of $A$, and $R$ is the row reduced echelon form of $A$.
$A=CR$ reduces to $r$ independent columns in $C$ times $r$ independent rows in $R$.

\begin{equation*}
  \begin{split}
    A &= CR\\
  \begin{bmatrix}
    1 & 2 & 3 \\
    2 & 3 & 5
  \end{bmatrix}
  & =
  \begin{bmatrix}
    1 & 2 \\
    2 & 3
  \end{bmatrix}
  \begin{bmatrix}
    1 & 0 & 1 \\
    0 & 1 & 1
  \end{bmatrix}
\end{split}
\end{equation*}

Procedure: Look at the columns of $A$ from left to right. Keep independent ones,
discard dependent ones which can be created by the former columns.
The column 1 and the column 2 survive, and the column 3 is discarded
because it is expressed as a sum of the former two columns.
To rebuild $A$ by the independent columns 1 and 2, you find a row echelon form $R$
appearing on the right.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{CR1.eps}
  \caption{Column Rank in $CR$}
\end{figure}

Now the column rank is two because there are only two independent columns in $C$
and all the columns of $A$ are linear combinations of the two columns of $C$.

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{CR2.eps}
  \caption{Row Rank in $CR$}
\end{figure}

And the row rank is also two because there are only two independent rows in $R$
and all the rows of $A$ are linear combinations of the two rows of $R$.

\subsection{$\boldsymbol{A=LU}$}

Solving $A\bm{x}=\bm{b}$  via Gaussian elimination can be represented as an $LU$ factorization.
Usually, you apply elementary row operation matrices ($E$) to $A$ to make upper triangular $U$.

\begin{align*}
  EA &= U\\
  A &= E^{-1}U\\
\text{let} \; L = E^{-1}, \quad  A &= LU
\end{align*}

Now solve $A\bm{x}=\bm{b}$ in 2 steps: (1) forward $L\bm{c}=\bm{b}$ and (2) back $U\bm{x}=\bm{c}$.


\begin{itemize}
  \item Sec.2.3 (p.57) Matrix Computations and $\bm{A=LU}$
\end{itemize}

Here, we directly calculate $L$ and $U$ from $A$.

\begin{equation*}
  A =
      \begin{bmatrix}
        |\\
        \bm{l}_1\\
        |
      \end{bmatrix}
      \begin{bmatrix}
        -  \bm{u}^*_1  -
      \end{bmatrix}
  +  \begin{bmatrix}
      0 & \begin{matrix} 0 & 0 \end{matrix}\\
      \begin{matrix} 0 \\ 0 \end{matrix} & A_2
    \end{bmatrix}
  =
  \begin{bmatrix}
    |\\
    \bm{l}_1\\
    |
  \end{bmatrix}
  \begin{bmatrix}
    - \bm{u}^*_1 -
  \end{bmatrix}
  +
  \begin{bmatrix}
    |\\
    \bm{l}_2\\
    |
  \end{bmatrix}
  \begin{bmatrix}
    - \bm{u}^*_2  -
  \end{bmatrix}
  +  \begin{bmatrix}
  0 & 0 & 0\\
  0 & 0 & 0 \\
  0 & 0 & A_3
  \end{bmatrix} = LU
\end{equation*}


\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{LU1.eps}
\caption{Recursive Rank 1 Matrix Peeling from $A$}
\end{figure}

To find $L$ and $U$, peel off the rank 1 matrix made of
the first row and the first column of $A$.
This leaves $A_2$. Do this recursively and decompose $A$ into the sum of rank 1 matrices.


\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{LU2.eps}
\caption{$LU$ rebuilds $A$}
\end{figure}

To rebuild $A$ from $L$ times $U$, use column-row multiplication.

\subsection{$\boldsymbol{A=QR}$}

$A=QR$ changes the columns of $A$ into perpendicular columns of $Q$, keeping $\bm{C}(A) = \bm{C}(Q)$.

\begin{itemize}
  \item Sec.4.4 Orthogonal matrices and Gram-Schmidt (p.165)
\end{itemize}

In Gram-Schmidt, the normalized $\bm{a}_1$ is $\bm{q}_1$.
Then $\bm{a}_2$ is adjusted to be perpendicular to $\bm{q}_1$ to create $\bm{q}_2$.
This procedure gives:

\begin{align*}
  \bm{q}_1 &= \bm{a}_1/||\bm{a}_1|| \\
  \bm{q}_2 &= \bm{a}_2 - (\bm{q}_1\transp \bm{a}_2)\bm{q}_1 , \quad \bm{q}_2 = \bm{q}_2/||\bm{q}_2|| \\
  \bm{q}_3 &= \bm{a}_3 - (\bm{q}_1\transp \bm{a}_3)\bm{q}_1 - (\bm{q}_2\transp \bm{a}_3)\bm{q}_2, \quad \bm{q}_3 = \bm{q}_3/||\bm{q}_3||
\end{align*}

In the reverse direction, let $r_{ij} = \bm{q}_i\transp \bm{a}_j$ and you will get:

\begin{align*}
  \bm{a}_1 &= r_{11}\bm{q}_1\\
  \bm{a}_2 &= r_{12}\bm{q}_1 + r_{22} \bm{q}_2\\
  \bm{a}_3 &= r_{13}\bm{q}_1 + r_{23} \bm{q}_2 + r_{33} \bm{q}_3
\end{align*}

The original $A$ becomes $QR$: orthogonal $Q$ times upper triangular $R$.

\begin{gather*}
  A =
  \begin{bmatrix}
    | & | & |\\
    \bm{q}_1 & \bm{q}_2 & \bm{q}_3\\
    | & | & |
  \end{bmatrix}
  \begin{bmatrix}
    r_{11} & r_{12} & r_{13}\\
           & r_{22} & r_{23}\\
           &        & r_{33}
  \end{bmatrix} = QR\\
  \\
  Q Q\transp=Q\transp Q = I
\end{gather*}

\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{QR.eps}
  \caption{$A=QR$}
\end{figure}

Each column vector of $A$ can be rebuilt from $Q$ and $R$.

See Pattern 1 (P1) again for the graphic interpretation.


\subsection{$\boldsymbol{S=Q \Lambda Q\transp}$}

All symmetric matrices $S$ must have real eigenvalues and orthogonal eigenvectors.
The eigenvalues are the diagonal elements of $\Lambda$ and the eigenvectors are in $Q$.

\begin{itemize}
  \item Sec.6.3 (p.227) Symmetric Positive Definite Matrices
\end{itemize}

\begin{align*}
  S = Q \Lambda Q\transp
&= \begin{bmatrix}
    | & | & |\\
    \bm{q}_1 & \bm{q}_2 & \bm{q}_3\\
    | & | & |
  \end{bmatrix}
  \begin{bmatrix}
    \lambda_1 \\
           & \lambda_2 & \\
           & & \lambda_3
  \end{bmatrix}
  \begin{bmatrix}
  - \bm{q}_1\transp -\\
  - \bm{q}_2\transp -\\
  - \bm{q}_3\transp -
  \end{bmatrix}\\
  \\
  &=
  \lambda_1 \begin{bmatrix}
    |\\
    \bm{q}_1\\
    |
  \end{bmatrix}
  \begin{bmatrix}
    - \bm{q}_1\transp -
  \end{bmatrix}
  +
  \lambda_2 \begin{bmatrix}
  |\\
  \bm{q}_2\\
  |
  \end{bmatrix}
  \begin{bmatrix}
  - \bm{q}_2\transp -
  \end{bmatrix}
  +
  \lambda_3 \begin{bmatrix}
    |\\
    \bm{q}_3 \\
    |
  \end{bmatrix}
  \begin{bmatrix}
    - \bm{q}_3\transp -
  \end{bmatrix} \\
&= \lambda_1 P_1 + \lambda_2 P_2 + \lambda_3 P_3
\end{align*}

\begin{equation*}
  P_1=\bm{q}_1 \bm{q}_1\transp, \quad P_2=\bm{q}_2 \bm{q}_2\transp, \quad P_3=\bm{q}_3 \bm{q}_3\transp
\end{equation*}


\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{EVD.eps}
  \caption{$S=Q \Lambda Q\transp$}
\end{figure}

A symmetric matrix $S$ is diagonalized into $\Lambda$  by an orthogonal matrix $Q$
and its transpose. And it is broken down into a combination of rank 1 projection matrices $P=qq\transp$.
This is the spectral theorem.

Note that Pattern 4 (P4) is working for the decomposition.

\begin{gather*}
  S=S\transp = \lambda_1 P_1 + \lambda_2 P_2 + \lambda_3 P_3\\
  QQ\transp = P_1 + P_2 + P_3 = I \\
  P_1 P_2 = P_2 P_3 = P_3 P_1 = O\\
  P_1^2 =P_1=P_1\transp, \quad P_2^2=P_2=P_2\transp, \quad P_3^2=P_3=P_3\transp
\end{gather*}

\subsection{$\boldsymbol{A=U \Sigma V\transp}$}


\begin{itemize}
  \item Sec.7.1 (p.259) Singular Values and Singular Vectors
\end{itemize}

Every matrix (including rectangular one) has a singular value decomposition (SVD).
$A=U \Sigma V\transp$ has the singular vectors of $A$ in $U$ and $V$.
The following figure illustrates the 'reduced' SVD.


\begin{figure}[H]
  \centering
  \includegraphics[scale=0.8]{SVD.eps}
  \caption{$A=U \Sigma V\transp$}
\end{figure}

You can find $V$ as an orthonormal basis of $\mathbb{R}^n$ (eigenvectors of $A\transp A$)
and $U$ as an orthonormal basis of $\mathbb{R}^m$ (eigenvectors of $AA\transp$).
Together they diagonalize $A$ into $\Sigma$.
This can be also expressed as a combination of rank 1 matrices.

\begin{align*}
  A = U \Sigma V\transp =
  \begin{bmatrix}
    | & | & |\\
    \bm{u}_1 & \bm{u}_2 & \bm{u}_3\\
    | & | & |
  \end{bmatrix}
  \begin{bmatrix}
    \sigma_1 \\
           & \sigma_2 \\
           & &
  \end{bmatrix}
  \begin{bmatrix}
  - \bm{v}_1\transp -\\
  - \bm{v}_2\transp -
  \end{bmatrix}
  & =
  \sigma_1 \begin{bmatrix}
    |\\
    \bm{u}_1\\
    |
  \end{bmatrix}
  \begin{bmatrix}
    - \bm{v}_1\transp -
  \end{bmatrix}
  +
  \sigma_2 \begin{bmatrix}
  |\\
  \bm{u}_2\\
  |
  \end{bmatrix}
  \begin{bmatrix}
  - \bm{v}_2\transp -
  \end{bmatrix} \\
& = \sigma_1 \bm{u}_1 \bm{v}_1\transp + \sigma_2 \bm{u}_2 \bm{v}_2\transp
\end{align*}

Note that:

\begin{align*}
  U U\transp &= I_m \\
  V V\transp &= I_n
\end{align*}

See Pattern 4 (P4) for the graphic notation.

\section*{Conclusion and Acknowledgements}

I have presented a systematic visualization of matrix/vector multiplication and
its applications to the Five Matrix Factorizations. I hope you
enjoy them and find them useful
in understanding Linear Algebra.

Ashley Fernandes helped me with typesetting, which
makes this paper much more appealing and professional.

To conclude this paper, I'd like to thank Prof. Gilbert Strang for
publishing ``Linear Algebra for Everyone". It presents a new pathway to these beautiful landscapes in Linear Algebra.
Everyone can reach a fundamental understanding of its underlying ideas
in a practical manner that introduces us to contemporary and also
traditional data science and machine learning.

\section*{References and Related Works}
\begin{enumerate}
  \item
  Gilbert Strang(2020),\emph{Linear Algebra for Everyone}, Wellesley Cambridge Press.,\\
  \url{http://math.mit.edu/everyone}
  \item
  Gilbert Strang(2016), \emph{Introduction to Linear Algebra},Wellesley Cambridge Press, 6th ed.,\\
  \url{http://math.mit.edu/linearalgebra}
  \item Kenji Hiranabe(2021), \emph{Map of Eigenvalues}, Slidedeck,\\
  \url{https://github.com/kenjihiranabe/The-Art-of-Linear-Algebra/blob/main/MapofEigenvalues.pdf}
  \begin{figure}[H]
    \centering
    \includegraphics[keepaspectratio, width=\linewidth]{MapofEigenvalues.eps}
    \caption{Map of Eigenvalues}
  \end{figure}
  \item Kenji Hiranabe(2020), \emph{Matrix World}, Slidedeck,\\
  \url{https://github.com/kenjihiranabe/The-Art-of-Linear-Algebra/blob/main/MatrixWorld.pdf}\\
  \begin{figure}[H]
    \centering
    \includegraphics[keepaspectratio, width=\linewidth]{MatrixWorld.eps}
    \caption{Matrix World}
  \end{figure}
  \item Gilbert Strang, artwork by Kenji Hiranabe, \emph{The Four Subspaces and the solutions to $A\bm{x}=\bm{b}$}\\
  \begin{figure}[H]
    \centering
    \includegraphics[scale=0.6]{TheFourSubspaces.eps}
    \caption{The Four Subspaces and the solutions to $A\bm{x}=\bm{b}$}
  \end{figure}
\end{enumerate}

\end{document}