Finished all chapters and definitions. I need to add subsections and see if there's any theorems or definitions in the appendicies that are worth adding to this as well.

chapter-6/the-adjoint-of-a-linear-operator.tex

@@ -1 +1,108 @@
 \section{The Adjoint of a Linear Operator}
+
+\begin{definition}\label{Definition 6.16}
+	\hfill\\
+	For a linear operator $T$ on an inner product space $V$, we define a related linear operator on $V$ called the \textbf{adjoint} of $T$, whose matrix representation with respect to any orthonormal basis $\beta$ for $V$ is $[T]_\beta^*$.
+\end{definition}
+
+\begin{theorem}
+	\hfill\\
+	Let $V$ be a finite-dimensional inner product space over $\F$, and let $\mathsf{g}: V \to \F$ be a linear transformation. Then there exists a unique vector $y \in V$ such that $\mathsf{g}(x) = \lr{x,y}$ for all $x \in V$.
+\end{theorem}
+
+\begin{theorem}
+	\hfill\\
+	Let $V$ be a finite-dimensional inner product space, and let $T$ be a linear operator on $V$. Then there exists a unique function $T^*: V \to V$ such that $\lr{T(x), y} = \lr{x, T^*(y)}$ for all $x,y \in V$. Furthermore, $T^*$ is linear.
+\end{theorem}
+
+\begin{remark}
+	\hfill\\
+	\textbf{Important Note:} For the remainder of this chapter we adopt the convention that a reference to the adjoint of a linear operator on an infinite-dimensional inner product space assumes its existence.
+\end{remark}
+
+\begin{theorem}
+	\hfill\\
+	Let $V$ be a finite-dimensional inner product space, and let $\beta$ be an orthonormal basis for $V$. If $T$ is a linear operator on $V$, then
+
+	\[[T^*]_\beta = [T]_\beta^*.\]
+\end{theorem}
+
+\begin{corollary}
+	\hfill\\
+	Let $A$ be an $n \times n$ matrix. Then $L_{A^*} = (L_A)^*$.
+\end{corollary}
+
+\begin{theorem}
+	\hfill\\
+	Let $V$ be an inner product space, and let $T$ and $U$ be linear operators on $V$. Then
+
+	\begin{enumerate}
+		\item $(T+U)^* = T^* + U^*$;
+		\item $(cT)^* = \overline{c}T^*$ for any $c \in \F$;
+		\item $(TU)^* = U^*T^*$;
+		\item $T^{**} = T$;
+		\item $I^* = I$.
+	\end{enumerate}
+\end{theorem}
+
+\begin{corollary}
+	\hfill\\
+	Let $A$ and $B$ be $n \times n$ matrices. Then
+
+	\begin{enumerate}
+		\item $(A + B)^* = A^* + B^*$;
+		\item $(cA)^* = \overline{c}A^*$ for all $c \in \F$;
+		\item $(AB)^* = B^*A^*$;
+		\item $A^{**} = A$;
+		\item $I^* = I$.
+	\end{enumerate}
+\end{corollary}
+
+\begin{lemma}
+	\hfill\\
+	Let $A \in M_{m \times n}(\F), x \in F^n$, and $y \in F^m$. Then
+
+	\[\lr{Ax,y}_m = \lr{x,A^*y}_n.\]
+\end{lemma}
+
+\begin{lemma}
+	\hfill\\
+	Let $A \in M_{m \times n}(\F)$. Then $\rank{A^*A} = \rank{A}$.
+\end{lemma}
+
+\begin{corollary}
+	\hfill\\
+	If $A$ is an $m \times n$ matrix such that $\rank{A} = n$, then $A^*A$ is invertible.
+\end{corollary}
+
+\begin{theorem}
+	\hfill\\
+	Let $A \in M_{m \times n}(\F)$ and $y \in F^m$. Then there exists $x_0 \in F^n$ such that $(A^*A)x_0 = A^*y$ and $||Ax_0 = y|| \leq ||Ax - y||$ for all $x \in F^n$. Furthermore, if $\rank{A} = n$, then $x_0 = (A^*A)^{-1}A^*y$.
+\end{theorem}
+
+\begin{definition}
+	\hfill\\
+	A solution $s$ to a system of linear equations $Ax = b$ is called a \textbf{minimal solution} if $||s|| \leq ||u||$ for all other solutions $u$.
+\end{definition}
+
+\begin{theorem}
+	\hfill\\
+	Let $A \in M_{m \times n}(\F)$ and $b \in F^m$. Suppose that $Ax = b$ is consistent. Then the following statements are true.
+
+	\begin{enumerate}
+		\item There exists exactly one minimal solution $s$ of $Ax = b$, and $x \in \range{L_{A^*}}$.
+		\item The vector $s$ is the only solution to $Ax = b$ that lies in $\range{L_{A^*}}$; that is, if $u$ satisfies $(AA^*)u = b$, then $s = A^*u$.
+	\end{enumerate}
+\end{theorem}
+
+\begin{definition}
+	\hfill\\
+	Let $T: V \to W$ be a linear transformation, where $V$ and $W$ are finite-dimensional inner product spaces with inner products $\lr{\cdot, \cdot}_1$ and $\lr{\cdot, \cdot}_2$, respectively. A function $T^*: W \to V$ is called an \textbf{adjoint} of $T$ if $\lr{T(x),y}_2 = \lr{x,T^*{y}}_1$ for all $x \in V$ and $y \in W$.\\
+
+	This is an extension of the definition of the \textit{adjoint} of a linear operator (\autoref{Definition 6.16})
+\end{definition}
+
+\begin{definition}
+	\hfill\\
+	In physics, \textit{Hooke's law} states that (within certain limits) there is a linear relationship between the length $x$ of a spring and the force $y$ applied to (or exerted by) the spring. That is, $y = cx + d$, where $c$ is called the \textbf{spring constant}.
+\end{definition}