diff --git a/src/op/c-star/gelfand.tex b/src/op/c-star/gelfand.tex new file mode 100644 index 0000000..1e786d7 --- /dev/null +++ b/src/op/c-star/gelfand.tex @@ -0,0 +1,77 @@ +\section{The Gelfand-Naimark Theorem} +\label{section:gelfand-naimark} + +\begin{theorem}[Gelfand-Naimark] +\label{theorem:gelfand-naimark} + Let $A$ be a commutative unital $C^*$-algebra, then the Gelfand transform + \[ + \Gamma_A: A \to C(\Omega(A); \complex) \quad \Gamma_A(x)(\phi) = \phi(x) + \] + + is a unital $C^*$-isomorphism. +\end{theorem} +\begin{proof}[Proof, {{\cite[Theorem II.9.4]{Zhu}}}. ] + By construction $\Gamma_A$ is a unital algebra homomorphism. + + To see that $\Gamma_A$ preserves involutions, let $y \in A$ be self-adjoint. By \autoref{proposition:gelfand-transform-gymnastics} and \autoref{proposition:self-adjoint-spectrum}, $\Gamma_A(y)(\Omega(A)) = \sigma_A(y) \subset \real$, so $\Gamma_A(y) \in C(\Omega(A); \real)$. For any $x \in A$, write $x = \text{Re}(x) + i\text{Im}(x)$, where $\text{Re}(x)$ and $\text{Im}(x)$ are both self-adjoint, then + \begin{align*} + \Gamma_A(x^*) &= \Gamma_A(\text{Re}(x) - i\text{Im}(x)) \\ + &= \Gamma_A(\text{Re}(x)) - i\Gamma_A(\text{Im}(x)) \\ + &= \overline{\Gamma_A(\text{Re}(x)) + i\Gamma_A(\text{Im}(x))} = \overline{\Gamma_A(x)} + \end{align*} + + so $\Gamma_A(x^*) = \Gamma_A(x)^*$. + + Now, for each $x \in A$, \autoref{corollary:c-star-unique-norm} and \autoref{proposition:gelfand-transform-gymnastics} imply that + \begin{align*} + \norm{x}_A^2 &= \sup\bracs{|\lambda|\ | \lambda \in \sigma_A(x^*x)} \\ + &= \sup\bracs{|\Gamma_A(x^*x)(\phi)|\ | \phi \in \Omega(A)} \\ + &= \sup\bracs{|\Gamma_A(x)(\phi)|^2\ | \phi \in \Omega(A)} \\ + \norm{x}_A &= \norm{\Gamma_A(x)}_u + \end{align*} + + Thus $\Gamma_A$ is an isometry, and $\Gamma_A(A)$ is a closed subalgebra of $C(\Omega(A))$. + + Since $\Gamma_A(1_A) = 1$, $\Gamma_A(A)$ contains constants. As $\Gamma_A(A)$ separates points and is closed under complex conjugation, $\Gamma_A(A) = C(\Omega(A))$ by the \hyperref[Stone-Weierstrass Theorem]{theorem:complex-stone-weierstrass}. +\end{proof} + +\begin{corollary} +\label{corollary:gelfand-naimark-converse} + Let $A$ be a unital $C^*$-algebra, then the following are equivalent: + \begin{enumerate} + \item $A$ is commutative. + \item $\Gamma_A$ is a *-isomorphism. + \item $\Gamma_A$ is injective. + \end{enumerate} +\end{corollary} + +\begin{corollary} +\label{corollary:spectrum-characterisation-iff} + Let $A$ be a commutative unital $C^*$-algebra and $x \in A$ be normal, then: + \begin{enumerate} + \item $x$ is self-adjoint if and only if $\sigma_A(x) \subset \real$. + \item $x$ is unitary if and only if $\sigma_A(x) \subset \partial B_\complex(0, 1)$. + \item $x$ is positive if and only if $\sigma_A(x) \subset [0, \infty)$. + \item $x$ is a projection if and only if $\sigma_A(x) \subset \bracs{0,1}$. + \end{enumerate} +\end{corollary} +% NEEDS WORK + +\begin{corollary} +\label{corollary:stonean-commutative-algebra} + Let $A$ be a unital $C^*$-algebra, then $A_{sa}$ is order complete if and only if $\Omega(A)$ is extremely disconnected. +\end{corollary} +\begin{proof} + By \autoref{theorem:gelfand-naimark}, $A$ and $C(\Omega(A); \complex)$ are isomorphic as $C^*$-algebras. In particular, $A_{sa}$ and $C(\Omega(A); \real)$ are isomorphic as ordered vector spaces, so $A_{sa}$ is order complete if and only if $C(\Omega(A); \real)$ is order complete. Thus the \hyperref[Stone-Nakano Theorem]{theorem:stone-nakano-extremely-disconnected} implies that $A_{sa}$ is order complete if and only if $\Omega(A)$ is extremely disconnected. +\end{proof} + +\begin{corollary} +\label{corollary:linfinity-extremely-disconnected} + Let $(X, \cm, \mu)$ be a localisable measure space, then $\Omega(L^\infty(X))$ is extremely disconnected. +\end{corollary} +\begin{proof} + By \autoref{corollary:l-infty-dedekind-complete}, $L^\infty(X; \real)$ is order complete. By \autoref{corollary:stonean-commutative-algebra}, $\Omega(L^\infty(X))$ is extremely disconnected. +\end{proof} + + + diff --git a/src/op/c-star/homomorphism.tex b/src/op/c-star/homomorphism.tex new file mode 100644 index 0000000..33a717d --- /dev/null +++ b/src/op/c-star/homomorphism.tex @@ -0,0 +1,39 @@ +\section{*-Homomorphisms} +\label{section:c-star-homomorphism} + +\begin{definition}[*-Homomorphism] +\label{definition:c-star-homomorphism} + Let $A, B$ be involutive algebras over $\complex$ and $\phi: A \to B$, then $\phi$ is a \textbf{*-homomorphism} if: + \begin{enumerate}[label=(SH\arabic*)] + \item For each $x, y \in A$ and $\lambda \in \complex$, $\phi(\lambda x + y) = \lambda \phi(x) + \phi(y)$. + \item For each $x, y \in A$, $\phi(xy) = \phi(x)\phi(y)$. + \item For each $x \in A$, $\phi(x^*) = \phi(x)^*$. + \end{enumerate} + + If $A$ and $B$ are unital, then $\phi$ is \textbf{unital} if: + \begin{enumerate} + \item[(U)] $\phi(1_A) = \one_B$. + \end{enumerate} +\end{definition} + + +\begin{proposition} +\label{proposition:star-homomorphism-contractive} + Let $A, B$ be unital $C^*$-algebras and $\phi: A \to B$ be a unital *-homomorphism, then for each $x \in A$, + \begin{enumerate} + \item $\sigma_B(\phi(x)) \subset \sigma_A(x)$. + \item $\norm{\phi(x)}_B \le \norm{x}_A$. + \end{enumerate} +\end{proposition} +\begin{proof} + (1): Since $\phi$ is unital, $\phi(G(A)) \subset G(B)$, so $\sigma_B(\phi(x)) \subset \sigma_A(x)$. + + (2): By (1) and \autoref{corollary:c-star-unique-norm}, + \begin{align*} + \norm{\phi(x)}_B^2 &= \sup\bracsn{|\lambda|\ | \lambda \in \sigma_B(\phi(x^*x))} \\ + &\ge \sup\bracsn{|\lambda|\ | \lambda \in \sigma_A(x^*x)} = \norm{x}_A^2 + \end{align*} + +\end{proof} + + diff --git a/src/op/c-star/index.tex b/src/op/c-star/index.tex index 9586e09..6e4ceb8 100644 --- a/src/op/c-star/index.tex +++ b/src/op/c-star/index.tex @@ -5,3 +5,5 @@ \input{./unitary.tex} \input{./sa.tex} \input{./order.tex} +\input{./homomorphism.tex} +\input{./gelfand.tex} \ No newline at end of file