Definition 37.4.6 ($L^{\infty}$ Functional Calculus).label Let $H$ be a complex Hilbert space, $T \in B(H)$ be normal, and $A \subset B(H)$ be the smallest von Neumann algebra acting on $H$ containing $T$ and $I$, then

  1. (1)

    There exists a unique spectral measure $E: \cb_{\sigma_{B(H)}(T)}\to A$ such that

    \[T = \int_{\sigma_{B(H)}(T)}\lambda E(d\lambda) \quad T^{*} = \int_{\sigma_{B(H)}(T)}\ol \lambda E(d\lambda)\]

  2. (2)

    Let $\mathscr{E}\subset M_{R}(\sigma_{B(H)}(T); \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, and $A \subset B(H)$ be the von Neumann algebra generated by $I$ and $T$, then

    \[I_{E}: \mathscr{E}^{*} \to A \quad \phi \mapsto \phi(T) := \int_{\sigma_{B(H)}(T)}\phi dE\]

    is a *-isomorphism.

  3. (3)

    $I_{E}: \mathscr{E}^{*} \to A$ is the unique weak* to weak-operator continuous unital *-homomorphism such that $I_{E}(\text{Id}) = T$.

The spectral measure $E$ is the resolution of the identity for $T$, and the mapping $f \mapsto f(T)$ on $\mathscr{E}^{*}$ is the $L^{\infty}$-functional calculus of $T$.

Proof. (1), (2): By Spectral Theorem I applied to $B(H)[T]$, there exists a unique spectral measure $E$ on $\sigma_{B(H)}(T)$ such that the mapping

\[I_{E}: \mathscr{E}^{*}\to A \quad \phi \mapsto \int_{\sigma_{B(H)}(T)}\phi dE\]

is a *-isomorphism that extends the inverse Gelfand transform $\Gamma_{B(H)[T]}^{-1}: C(\sigma_{B(H)}(T); \complex) \to B(H)[T]$.

For each $\phi \in \mathscr{E}^{*}$, let $\phi(T) = \int_{\sigma_{B(H)}(T)}\phi dE$, then the mapping $\phi \mapsto \phi(T)$ is continuous from the weak* topology on $\mathscr{E}^{*}$ to the weak operator topology on $A$ by Definition 37.4.3.

(3): By uniqueness of the continuous functional calculus, Goldstine’s Theorem, and (2), the mapping $\phi \mapsto \phi(T)$ is unique.$\square$

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