37.4 The Borel Functional Calculus
Definition 37.4.1 (Spectral Measure).label Let $X$ be a compact Hausdorff space, $H$ be a complex Hilbert space, and $E: \cb_{X} \to B(H)$, then $E$ is a spectral measure relative to $H$ if:
- (1)
For each $B \in \cb_{X}$, $E(B)$ is an orthogonal projection.
- (2)
$E(\emptyset) = 0$, $E(X) = I_{B(H)}$.
- (3)
For each $B, C \in \cb_{X}$, $E(B \cap C) = E(B)E(C)$.
- (4)
For each $x, y \in H$, the mapping
\[E_{x, y}: \cb_{X} \to \complex \quad B \mapsto \dpn{E(B)x, y}{H}\]is a complex Radon measure on $X$.
Definition 37.4.2 (Integration Against a Spectral Measure).label Let $X$ be a compact Hausdorff space, $H$ be a complex Hilbert space, and $E: \cb_{X} \to B(H)$ be a spectral measure. Define
where for each $x, y \in H$, $\angles{I_E(\phi) \cdot x, y}_{H}= \dpn{E_{x, y}, \phi}{C(X; \complex)^*}$, then:
- (1)
$I_{E}$ is continuous from the weak*-topology on $C(X; \complex)^{**}$ to the weak operator topology on $B(H)$.
- (2)
$I_{E}$ is a unital *-homomorphism.
For any $\phi \in C(X; \complex)^{**}$, $I_{E}(\phi) = \int_{X} \phi dE$ is the integral of $\phi$ with respect to $E$.
Proof. Firstly, let $x, y \in H$, $\seqf{B_j}\subset \cb_{X}$ be disjoint Borel sets, and $B = \bigsqcup_{j = 1}^{n} B_{j}$, then for each $1 \le i < j \le n$, $E(B_{i})(H) \perp E(B_{j})(H)$, so by the Cauchy-Schwarz inequality and the Pythagorean Theorem,
As the above holds for all finite sequences of disjoint Borel sets, $\norm{E_{x, y}}_{C(X; \complex)^*}\le \norm{x}_{H} \norm{y}_{H}$. Thus for any $\phi \in C(X; \complex)^{**}$,
Since the above holds for all $x, y \in H$, $I_{E}(\phi) \in B(H)$ with $\norm{I_E(\phi)}_{B(H)}\le \norm{\phi}_{C(X; \complex)^{**}}$.
(1): For each $x, y \in H$, $E_{x, y}\in C(X; \complex)^{*}$. Since $\angles{\int \phi dE \cdot x, y}_{H}= \dpn{E_{x, y}, \phi}{C(X; \complex)^*}$ for every $\phi \in C(X; \complex)^{**}$, $I_{E}$ is continuous from the weak* topology on $C(X; \complex)^{**}$ to the weak operator topology on $B(H)$.
(2): By Lemma 26.6.4, the simple functions $\Sigma(X; \complex)$ are uniformly dense in the bounded Borel functions $B^{\infty}(X; \complex)$. Since
- (i)
$I_{E}$ restricted to $\Sigma(X; \complex)$ is a *-homomorphism.
- (ii)
Multiplication and conjugation are continuous in the uniform norm on $B^{\infty}(X; \complex)$
- (iii)
Composition and transposition are continuous in the operator norm on $B(H)$
the map $I_{E}$ restricted to $B^{\infty}(X; \complex)$ is a *-homomorphism by continuity. By Goldstine’s Theorem, $C(X; \complex) \subset B^{\infty}(X; \complex)$ is weak*-dense in $C(X; \complex)^{**}$. So as
- (i)
$I_{E}$ restricted to $B^{\infty}(X; \complex)$ is a *-homomorphism.
- (ii)
The involution $\phi \mapsto \ol \phi$ is weak*-continuous on $C(X; \complex)^{**}$.
- (iii)
The transpose $T \mapsto T^{*}$ is weak-operator continuous on $B(H)$.
- (iv)
The product $(\phi, \psi) \mapsto \phi \psi$ is separately weak*-continuous on $C(X; \complex)^{**}$.
- (v)
The composition $(S, T) \mapsto ST$ is separately weak-operator continuous on $B(H)$.
the map $I_{E}$ is a *-homomorphism by (1). Finally, since $E(X) = I_{B(H)}$, $I_{E}$ is a unital *-homomorphism.$\square$
Theorem 37.4.3 (Spectral Theorem (I)).label Let $H$ be a complex Hilbert space and $A \subset B(H)$ be a commutative $C^{*}$-subalgebra with $I \in A$, then:
- (1)
There exists a unique spectral measure $E: \cb_{\Omega(A)}\to B(H)$ such that
\[T = \int_{\Omega(A)}\Gamma_{A} T dE \quad \forall T \in A\] - (2)
Let $B \subset B(H)$ be the strong-operator closure of $A$ in $B(H)$, then
\[B = \bracs{\int_{\Omega(A)} \phi dE \bigg | \phi \in C(\Omega(A); \complex)^{**}}\]
The mapping $C(\Omega(A); \complex)^{**}\to B$ defined by $\phi \mapsto \int \phi dE$ is the extended inverse Gelfand transform of $A$.
Proof, [Theorem 20.2, Zhu93]. (1): By the Gelfand-Naimark Theorem, $\Gamma_{A}: A \to C(\Omega(A); \complex)$ is a unital *-isomorphism. For each $x, y \in H$, $\Gamma_{A}^{-1}$ induces a mapping
which, by the Riesz Representation Theorem, takes the form of a complex Radon measure on $\Omega(A)$. Thus by the uniqueness part of the Riesz Representation Theorem, such a spectral measure must be unique if it exists.
Since $\norm{E_{x, y}}_{C(\Omega(A); \complex)^*}\le \norm{x}_{H}\norm{y}_{H}$ for all $x, y \in H$, $\bracsn{E_{x, y}|x, y \in H}$ induces a bounded linear map
with $I_{E}(f) = \Gamma_{A}^{-1}(f)$ for all $f \in C(\Omega(A); \complex)$.
For any $C \in \cb_{\Omega(A)}$, $\one_{C}$ is a projection in $B^{\infty}(\Omega(A); \complex)$. So to see that
defines a spectral measure, it is sufficient to show that $I_{E}|_{B^\infty(\Omega(A); \complex)}$ is a *-homomorphism.
Let $x, y \in H$, then as $\Gamma_{A}$ is a *-isomorphism, for any $f, g \in C(\Omega(A); \complex)$,
As the above holds for all $g \in C(\Omega(A); \complex)$, $fE_{x, y}= E_{x, I_E(f)^*y}$. Now, fix $\phi \in B^{\infty}(\Omega(A); \complex)$, then for every $f \in C(\Omega(A); \complex)$,
so $\phi E_{x, y}= E_{I_E(\phi)x, y}$ for all $\phi \in B^{\infty}(\Omega(A); \complex)$. Thus for any $\phi, \psi \in B^{\infty}(\Omega(A); \complex)$,
and $I_{E}|_{B^\infty(\Omega(A); \complex)}$ is a homomorphism[1].
Finally, let $f \in C(\Omega(A); \real)$, then since $\Gamma_{A}$ is a *-isomorphism, $I_{E}(f) = \Gamma_{A}^{-1}(f)$ is self-adjoint. As such, for any $x \in H$, $\dpn{f, E_{x, x}}{C(\Omega(A); \complex)}= \dpn{I_E(f)x, x}{H}\in \real$, so $E_{x, x}$ is real-valued. Thus for any $\phi \in B^{\infty}(\Omega(A); \real)$ and $x \in H$, $\dpn{I_E(\phi)x, x}{H}= \dpn{E_{x, x}, \phi}{C(\Omega(A); \complex)^*}\in \real$ as well. Therefore $I_{E}(\phi)$ is self-adjoint, and $I_{E}|_{B^\infty(\Omega(A); \complex)}$ is a *-homomorphism.
(2): By Goldstine’s Theorem, $C(\Omega(A); \complex)$ is weak*-dense in $C(\Omega(A); \complex)^{**}$. Since the mapping $\phi \mapsto \int_{\Omega(A)}\phi dE$ is continuous from the weak* topology on $C(\Omega(A); \complex)^{**}$ to the weak operator topology on $B(H)$,
On the other hand, by the Banach-Alaoglu Theorem, $\ol{B_{C(\Omega(A); \complex)^{**}}(0, 1)}$ is weak*-compact, so
is weak-operator compact. As $\Gamma_{A}: A \to C(\Omega(A); \complex)$ is an isometric isomorphism, $S \supset \ol{B_A(0, 1)}$. By the Kaplansky Density Theorem, $S \supset B_{B}(0, 1)$, and
$\square$
Definition 37.4.4 (Borel 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 there exists a unique unital *-homomorphism
such that:
- (1)
$\one(T) = I$, $\text{Id}(T) = T$, $\ol{\text{Id}}(T) = T^{*}$.
- (2)
The mapping $\phi \mapsto \phi(T)$ is continuous from the weak* topology on $C(\sigma_{B(H)}(T); \complex)^{**}$ to the weak operator topology on $A$.
Moreover, there exists a unique spectral measure $E: \cb_{\sigma_{B(H)}(T)}\to A$ such that $\phi(T) = \int_{\sigma_{B(H)}(T)}\phi dE$ for all $\phi \in C(\sigma_{B(H)}(T); \complex)^{**}$.
Proof. By the Spectral Theorem applied to $B(H)[T]$, there exists a unique spectral measure $E$ on $\sigma_{B(H)}(T)$ such that the mapping
extends the inverse Gelfand transform $\Gamma_{B(H)[T]}^{-1}: C(\sigma_{B(H)}(T); \complex) \to B(H)[T]$.
For each $\phi \in C(\sigma_{B(H)}(T); \complex)^{**}$, let $\phi(T) = \int_{\sigma_{B(H)}(T)}\phi dE$, then the mapping $\phi \mapsto \phi(T)$ is continuous from the weak* topology on $C(\sigma_{B(H)}(T); \complex)^{**}$ to the weak operator topology on $A$ by Definition 37.4.2.
Finally, by uniqueness of the continuous functional calculus, Goldstine’s Theorem, and (2), the mapping $\phi \mapsto \phi(T)$ is unique.$\square$
- With the same amount of writing and considerably more mental gymnastics, it can be shown that $I_{E}$ is a *-homomorphism on the full space $C(\Omega(A); \complex)^{**}$. However, it is not needed to show that $E$ is a spectral measure, and the homomorphism property falls out at the end anyways.keyboard_return
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