37.4 The Spectral Theorem
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 $X$.
Lemma 37.4.2.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 relative to $H$, then:
- (1)
For each $x, y \in H$, $\norm{E_{x, y}}_{\text{var}}\le \norm{x}_{H} \norm{y}_{H}$.
- (2)
For each $x \in H$, $E_{x, x}$ is positive.
Let $\mathscr{E}\subset M_{R}(X; \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, then
- (3)
For any $\mu \in \mathscr{E}$ and $\nu \in M_{R}(X; \complex)$ with $\nu \ll \mu$, $\nu \in \mathscr{E}$ as well.
- (4)
Let
\[J: B^{\infty}(X; \complex) \to \mathscr{E}^{*} \quad \dpn{\mu, J(f)}{\mathscr{E}}= \int_{X} f d\mu\]then $\mathscr{E}^{*}$ admits a unique weak*-continuous involution and a unique separately weak*-continuous product, such that $\mathscr{E}^{*}$ is a commutative unital $C^{*}$-algebra, and $J$ is a unital *-homomorphism.
Proof. (1): 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, $\norm{E_{x, y}}_{\text{var}}\le \norm{x}_{H} \norm{y}_{H}$.
(2): For each $B \in \cb_{X}$, $E(B)$ is a projection, so $E_{x, x}(B) = \dpn{E(B)x, x}{H}\ge 0$.
(3): For each $x, y \in H$ and $B, C \in \cb_{X}$,
By linearity, $fdE_{x, y}\in \mathscr{E}$ for all $f \in \Sigma(X; \complex)$. For each $f \in \Sigma(X; \complex)$, the mapping $\mu \mapsto f d\mu$ is continuous in the total variation norm, so $fd\mu \in \mathscr{E}$ for all $\mu \in \mathscr{E}$ and $f \in \Sigma(X; \complex)$. By Proposition 16.1.10, $\Sigma(X; \complex)$ is dense in $L^{1}(\mu; \complex)$ for all $\mu \in \mathscr{E}$. Therefore $fd\mu \in \mathscr{E}$ for all $f \in L^{1}(\mu; \complex)$ and $\mu \in \mathscr{E}$.
Finally, let $\mu \in \mathscr{E}$ and $\nu \in M_{R}(X; \complex)$ with $\nu \ll \mu$, then by the Radon-Nikodym Theorem, there exists $f \in L^{1}(\mu; \complex)$ such that $d\nu = f d\mu \in \mathscr{E}$.
(4): By (3), for any $\mu \in \mathscr{E}$ and $f \in L^{1}(\mu; \complex)$, $fd\mu \in \mathscr{E}$ as well. By Proposition 38.8.1, there exists a unique weak*-continuous involution and separately weak*-continuous product on $\mathscr{E}^{*}$ making $\mathscr{E}^{*}$ a commutative unital $C^{*}$-algebra, and $J|_{C(X; \complex)}$ a unital *-homomorphism. Since
- (i)
$J$ is $\sigma(B^{\infty}(X; \complex), M_{R}(X; \complex))$-$\sigma(\mathscr{E}^{*}, \mathscr{E})$ continuous.
- (ii)
Conjugation on $B^{\infty}(X; \complex)$ is $\sigma(B^{\infty}(X; \complex), M_{R}(X; \complex))$-continuous.
- (iii)
Multiplication on $B^{\infty}(X; \complex)$ is separately $\sigma(B^{\infty}(X; \complex), M_{R}(X; \complex))$-continuous.
the mapping $J$ is a unital *-homomorphism.$\square$
Definition 37.4.3 (Integration Against Spectral Measure).label Let $X$ be a compact Hausdorff space, $H$ be a complex Hilbert space, $E: \cb_{X} \to B(H)$ be a spectral measure relative to $H$, $\mathscr{E}\subset M_{R}(X; \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, and
Then, $\mathscr{E}^{*}$ admits a unique weak*-continuous involution and a unique separately weak*-continuous product, such that $\mathscr{E}^{*}$ is a commutative unital $C^{*}$-algebra, and $J$ is a unital *-homomorphism.
For each $\phi \in \mathscr{E}^{*}$, let $I_{E}(\phi) \in B(H)$ be the operator defined by
then
- (1)
$I_{E}$ is a contraction from $\mathscr{E}^{*}$ to $B(H)$.
- (2)
$I_{E}$ is continuous from the weak*-topology on $\mathscr{E}^{*}$ to the weak operator topology on $B(H)$.
- (3)
$I_{E}$ is an injective unital *-homomorphism.
For any $\phi \in \mathscr{E}^{*}$, $I_{E}(\phi) = \int_{X} \phi dE$ is the integral of $\phi$ with respect to $E$.
Proof. (1): Let $\phi \in \mathscr{E}^{*}$ and $x, y \in H$, then by Lemma 37.4.2,
Since the above holds for all $x, y \in H$, $I_{E}(\phi) \in B(H)$ with $\norm{I_E(\phi)}_{B(H)}\le \norm{\phi}_{\mathscr{E}^{*}}$.
(2): For each $x, y \in H$, $E_{x, y}\in \mathscr{E}$. Since $\angles{\int \phi dE \cdot x, y}_{H}= \dpn{E_{x, y}, \phi}{\mathscr{E}}$ for every $\phi \in \mathscr{E}^{*}$, $I_{E}$ is continuous from the weak* topology on $\mathscr{E}^{*}$ to the weak operator topology on $B(H)$.
(3): 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 $J(\Sigma(X; \complex))$ is a *-homomorphism.
- (ii)
Multiplication and conjugation are continuous in the uniform norm on $B^{\infty}(X; \complex)$
- (iii)
Composition and adjunction are continuous in the operator norm on $B(H)$
the map $I_{E}$ restricted to $J(B^{\infty}(X; \complex))$ 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 $J(C(X; \complex))$ is weak*-dense in $\mathscr{E}^{*}$. As
- (i)
$I_{E}$ restricted to $J(B^{\infty}(X; \complex))$ is a *-homomorphism.
- (ii)
The involution $\phi \mapsto \ol \phi$ is weak*-continuous on $\mathscr{E}^{*}$.
- (iii)
The adjunction $T \mapsto T^{*}$ is weak-operator continuous on $B(H)$.
- (iv)
The product $(\phi, \psi) \mapsto \phi \psi$ is separately weak*-continuous on $\mathscr{E}^{*}$.
- (v)
The composition $(S, T) \mapsto ST$ is separately weak-operator continuous on $B(H)$.
the map $I_{E}$ is a *-homomorphism by the weak* to weak-operator continuity established in (2). Since $E(X) = I_{B(H)}$, $I_{E}$ is a unital *-homomorphism.
Finally, let $\phi \in \mathscr{E}^{*}$ with $I_{E}(\phi) = 0$, then $\dpn{I_E(\phi)x, y}{H}= \dpn{E_{x, y}, \phi}{\mathscr{E}}= 0$ for all $x, y \in H$. As $\mathscr{E}$ is the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, $\phi = 0$. Therefore $I_{E}$ is an injective unital *-homomorphism.$\square$
Theorem 37.4.4 (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[1]
\[T = \int_{\Omega(A)}\Gamma_{A} T dE \quad \forall T \in A\] - (2)
Let $B \subset B(H)$ be the strong-operator closure of $A$ in $B(H)$, and $\mathscr{E}\subset M_{R}(\Omega(A); \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, then
\[I_{E}: \mathscr{E}^{*} \to B \quad \phi \mapsto \int_{\Omega(A)}\phi dE\]is a *-isomorphism.
The measure $E$ is the spectral measure associated with $A$, and the homomorphism $I_{E}$ 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 *-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 $J_{E}(f) = \Gamma_{A}^{-1}(f)$ 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 $J_{E}$ 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 $g \in C(\Omega(A); \complex)$, $fE_{x, y}= E_{x, J_E(f)^*y}$. Now, fix $\phi \in B^{\infty}(\Omega(A); \complex)$, then for every $f \in C(\Omega(A); \complex)$,
so $\phi E_{x, y}= E_{J_E(\phi)x, y}$ for all $\phi \in B^{\infty}(\Omega(A); \complex)$. Thus for any $\phi, \psi \in B^{\infty}(\Omega(A); \complex)$,
and $J_{E}$ is a homomorphism.
Finally, let $f \in C(\Omega(A); \real)$, then since $\Gamma_{A}$ is a *-isomorphism, $J_{E}(f) = \Gamma_{A}^{-1}(f)$ is self-adjoint. As such, for any $x \in H$, $\dpn{f, E_{x, x}}{C(\Omega(A); \complex)}= \dpn{J_E(f)x, x}{H}\in \real$, so $E_{x, x}$ is real-valued. Thus for any $\phi \in B^{\infty}(\Omega(A); \real)$ and $x \in H$, $\dpn{J_E(\phi)x, x}{H}= \dpn{E_{x, x}, \phi}{C(\Omega(A); \complex)^*}\in \real$ as well. Therefore $J_{E}(\phi)$ is self-adjoint, and $J_{E}$ is a *-homomorphism.
(2): By Definition 37.4.3, $I_{E}$ is an injective unital *-homomorphism, so it is sufficient to show that $I_{E}(\mathscr{E}^{*}) = B$.
Let $J: C(\Omega(A); \complex) \to \mathscr{E}^{*}$ be defined by $\dpn{\mu, J(f)}{\mathscr{E}}= \int_{\Omega(A)}f d\mu$ for each $\mu \in \mathscr{E}$ and $f \in C(\Omega(A); \complex)$. By Goldstine’s Theorem, $C(\Omega(A); \complex)$ is weak*-dense in $C(\Omega(A); \complex)^{**}$, so $J(C(\Omega(A); \complex))$ is weak*-dense in $\mathscr{E}^{*}$. Since $I_{E}$ is continuous from the weak* topology on $\mathscr{E}^{*}$ to the weak operator topology on $B(H)$, $I_{E}(\mathscr{E}^{*}) \subset B$ by Proposition 5.5.3.
On the other hand, by the Banach-Alaoglu Theorem, $\ol{B_{\mathscr{E}^*}(0, 1)}$ is weak*-compact, so $I_{E}(\ol{B_{\mathscr{E}^*}(0, 1)})$ is weak-operator compact. As $\Gamma_{A}: A \to C(\Omega(A); \complex)$ is an isometric isomorphism, $I_{E}(\ol{B_{\mathscr{E}^*}(0, 1)}) \supset \ol{B_A(0, 1)}$. By the Kaplansky Density Theorem, $I_{E}(\ol{B_{\mathscr{E}^*}(0, 1)}) \supset \ol{B_B(0, 1)}$, and $I_{E}(\mathscr{E}^{*}) = B$.$\square$
Theorem 37.4.5 (Spectral Theorem II).label Let $H$ be a complex Hilbert space, $A \subset B(H)$ be a commutative $C^{*}$-subalgebra with $I \in A$, $B \subset B(H)$ be the von Neumann algebra generated by $A$, $E: \cb_{\Omega(A)}\to B(H)$ be the spectral measure associated with $A$, $\mathscr{E}\subset M_{R}(\Omega(A); \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$, and $\seqi{\xi}\subset H$ be a maximal family such that the subspaces $\bracsn{A\xi_i|i \in I}$ are mutually orthogonal, then:
- (1)
For each $i \in I$, there exists a finite positive Radon measure $\mu_{i}$ on $\Omega(A)$ such that for every Borel set $C \in \cb_{\Omega(A)}$, $\mu_{i}(C) = 0$ if and only if $E_{x, y}(C) = 0$ for all $x, y \in \ol{A\xi_i}$.
- (2)
For each $i \in I$, let $P_{i}: H \to \ol{A\xi_i}$ be the orthogonal projection onto $\ol{A\xi_i}$, then for any $x, y \in H$, $E_{x, y}= \sum_{i \in I}E_{P_ix, P_iy}$.
- (3)
The natural map $C(\Omega(A); \complex) \to [l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)]$ is injective. Equivalently, $\ol{\bigcup_{i \in I}\supp{\mu_i}}= \Omega(A)$.
- (4)
The space $\mathscr{E}$ is a quotient of $[l^{1}(I); L^{1}(\mu_{i}; \complex)]$ under the mapping
\[\mathscr{M}: [l^{1}(I); L^{1}(\mu_{i}; \complex)] \to \mathscr{E}\quad f \mapsto \sum_{i \in I}f_{i}d\mu_{i}\]and $\mathscr{E}^{*}$ may be identified as a closed subspace of $[l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)]$ through $\mathscr{M}^{*}$.
- (5)
There exists a unitary equivalence $U: H \to [l^{2}(I); L^{2}(\mu_{i}; \complex)]$ between $\mathscr{E}^{*}$ acting on $[l^{2}(I); L^{2}(\mu_{i}; \complex)]$ and $B$ acting on $H$, such that for each $i \in I$, $U|_{\ol{A\xi_i}}$ is an isometry onto the $i$-th factor of $[l^{2}(I); L^{2}(\mu_{i}; \complex)]$.
Proof, [Theorem 1.47, Fol16]. (1): Fix $i \in I$ and let $\mu_{i} = E_{\xi_i, \xi_i}$, then for any $C \in \cb_{\Omega(A)}$ with $E_{x, y}(C) = 0$ for all $x, y \in \ol{A\xi_i}$, $\mu_{i}(C) = 0$. By (1) and (2) of Lemma 37.4.2, $\mu_{i}$ is a finite positive Radon measure.
By Spectral Theorem I, for each $S, T \in A$ and $C \in \cb_{\Omega(A)}$,
so $\Gamma_{A}S \cdot \ol{\Gamma_AT}dE_{\xi_i, \xi_i}= dE_{S\xi_i, T\xi_i}\ll \mu_{i}$. By (1) of Lemma 37.4.2 and completeness of $L^{1}(\mu_{i}; \complex)$, $\bracsn{E_{x, y}|x, y \in \ol{A\xi_i}}$ is absolutely continuous with respect to $\mu_{i}$. Therefore for any $C \in \cb_{\Omega(A)}$, $\mu_{i}(C) = 0$ if and only if $E_{x, y}(C) = 0$ for all $x, y \in \ol{A \xi_i}$.
(2): Let $i, j \in I$ with $i \ne j$, $x \in \ol{A\xi_i}$, $y \in \ol{A\xi_j}$, and $f \in C(\Omega(A); \complex)$, then since $\ol{A\xi_i}\perp \ol{A\xi_j}$,
As the above holds for all $f \in C(\Omega(A); \complex)$, $E_{x, y}= 0$.
Given that $\seqi{\xi}$ is maximal, $x = \sum_{i \in I}P_{i}x$ for all $x \in H$. Thus for any $x, y \in H$,
(3): Let $T \in A$ with $\Gamma_{A} T = 0$ $\mu_{i}$-almost everywhere for all $i \in I$. By (1), $E_{P_ix, P_iy}\ll \mu_{i}$ for all $i \in I$. Thus for any $x, y \in H$,
Therefore $C(\Omega(A); \complex)$ may be identified as a subspace of $[l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)]$.
(4): By (2), for each $x, y \in H$, $E_{x, y}= \sum_{i \in I}E_{P_ix, P_iy}$. By (1), $E_{P_ix, P_iy}\ll \mu_{i}$ for all $i \in I$, so $\mathscr{E}\subset \mathscr{M}([l^{1}(I); L^{1}(\mu_{i}; \complex)])$.
On the other hand, for each $i \in I$, since $\mu_{i}$ is a Radon measure, $C(\Omega(A); \complex)$ is dense in $L^{1}(\mu_{i}; \complex)$ by Proposition 25.1.7. As
and $\mathscr{E}\subset M_{R}(\Omega(A); \complex)$ is closed, $\mathscr{E}\supset \bracsn{f d\mu_i|f \in L^1(\mu_i; \complex)}$.
Finally, given that the above holds for all $i \in I$, $\mathscr{E}= \mathscr{M}([l^{1}(I); L^{1}(\mu_{i}; \complex)])$. By Theorem 16.5.6 and Theorem 16.3.4, $[l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)] = [l^{1}(I); L^{1}(\mu_{i}; \complex)]^{*}$, so $\mathscr{E}^{*}$ may be identified with its image under $\mathscr{M}^{*}$.
(5): Fix $i \in I$, then for any $S, T \in A$ with $S\xi_{i} = T\xi_{i}$,
so $\Gamma_{A} S = \Gamma_{A} T$ $\mu_{i}$-almost everywhere. Thus the mapping
is well-defined. Moreover, for any $S, T \in A$,
so $U_{i}$ extends into an isometry between $\ol{A\xi_i}$ and $L^{2}(\mu_{i}; \complex)$. Thus the mapping
is an isometry between $H$ and $[l^{2}(I); L^{2}(\mu_{i}; \complex)]$ such that $U(Tx) = \Gamma_{A}T \cdot Ux$ for all $x \in H$ and $T \in A$.
Finally, given that
- (i)
By Goldstine’s Theorem, $C(\Omega(A); \complex)$ is weak*-dense in $\mathscr{E}^{*}$.
- (ii)
The weak* topology on $[l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)]$ is equal to the weak operator topology of $[l^{\infty}(I); L^{\infty}(\mu_{i}; \complex)]$ acting on $[l^{2}(I); L^{2}(\mu_{i}; \complex)]$.
- (iii)
$A$ is weak-operator dense in $B$.
- (iv)
By Spectral Theorem I, the isomorphism $\phi \mapsto \int \phi dE$ is continuous from the weak* topology on $\mathscr{E}^{*}$ to the weak operator topology on $B$.
the mapping $U$ is a unitary equivalence between $\mathscr{E}^{*}$ acting on $[l^{2}(I); L^{2}(\mu_{i}; \complex)]$ and $B$ acting on $H$.$\square$
Remark 37.4.1.label Let $H$ be a complex Hilbert space, $A \subset B(H)$ be a commutative $C^{*}$-subalgebra with $I \in A$, $B$ be the von Neumann algebra generated by $A$, $E: \cb_{\Omega(A)}\to B(H)$ be the spectral measure associated with $A$, and $\mathscr{E}\subset M_{R}(\Omega(A); \complex)$ be the closed subspace generated by $\bracsn{E_{x, y}|x, y \in H}$.
By Spectral Theorem II, there exists a decomposable measure space $\Omega$, corresponding to a number of copies of $\Omega(A)$, such that $\mathscr{E}$ is a quotient of its $L^{1}$ space, $\mathscr{E}^{*}$ is a subspace of its $L^{\infty}$ space, and $H$ is isomorphic to its $L^{2}$ space. The preceding isomorphisms are all linked by a unitary equivalence between $B$ acting on $H$, and $\mathscr{E}^{*}$ acting on the $l^{2}$ direct sum.
The complexity of $\Omega$, that is, the number of copies of $\Omega(A)$ that it contains, depends on two factors:
- (1)
The complexity of the von Neumann algebra $B$: If $B$ is sufficiently complex, then $\mathscr{E}$ cannot be expressed as the $L^{1}$ space of a single measure on $\Omega(A)$. Instead, multiple copies of $\Omega(A)$ are needed to handle mutually singular measures with overlapping supports. For more details on this phenomenon, see Theorem 24.7.2.
- (2)
The size of the Hilbert space $H$ relative to $B$: If $H$ is extremely large, then a large number of vectors are required for $B$ to cover it. As such, many copies of $\Omega(A)$ are required to handle the complexity of $H$.
More concretely, (1) manifests as the size of the space $\mathscr{E}$, and (2) manifests as the size of the kernel of the mapping $L^{1}(\Omega) \to \mathscr{E}$.
By limiting these two sources of complexity, it is possible to remove the need of multiple copies of $\Omega(A)$. In particular,
- (1)
If $B$ admits a cyclic vector, then only one copy of $\Omega(A)$ is required for the construction in the Spectral Theorem [Theorem 23.1, Zhu93].
- (2)
- Omitting the natural map $C(\Omega(A); \complex) \to \mathscr{E}^{*}$. keyboard_return
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