43.4 Normal Maps

Lemma 43.4.1 (Jordan Decomposition).label Let $H$ be a complex Hilbert space, $M \subset B(H)$ be a von Neumann algebra, and $\omega: M \to \complex$ be a weak-operator continuous linear functional, then there exist positive weak-operator continuous functionals $\bracsn{\omega_k}_{0}^{3}$ such that $\omega = \sum_{k = 0}^{3} i^{k} \omega_{k}$.

Proof. Assume without loss of generality that there exist $\xi, \eta \in H$ such that $\dpn{x, \omega}{M}= \dpn{x\xi, \eta}{H}$ for all $x \in M$. In which case, by polarisation,

\[\dpn{x, \omega}{M}= \dpn{x\xi, \eta}{H}= \frac{1}{4}\sum_{k = 0}^{3} i^{k} \dpn{x(\xi + i^k\eta), \xi + i^k\eta}{H}\]

for all $x \in M$.$\square$

Lemma 43.4.2 (Radon-Nikodym).label Let $H$ be a complex Hilbert space, $M \subset B(H)$ be a von Neumann algebra, $\omega: M \to \complex$ be a positive linear functional, and $\xi \in H$ such that $\omega(x) \le \dpn{x\xi, \xi}{H}$ for all $x \in M_{+}$, then there exists $x' \in M'_{+}$ such that $\omega(x) = \dpn{x(x'\xi), x'\xi}{H}$ for all $x \in M$.

Proof. By the Cauchy-Schwarz inequality, for each $x, y \in M$,

\[|\omega(y^{*}x)|^{2} \le \omega(x^{*}x)\omega(y^{*}y) \le \norm{x\xi}_{H}^{2} \norm{y\xi}_{H}^{2}\]

so the mapping $(x, y) \mapsto \omega(y^{*}x)$ is a bounded sesquilinear form on $M\xi$. By the Riesz Representation Theorem, there exists $z \in B(\ol{M\xi})$ such that $\omega(y^{*}x) = \dpn{zx\xi, y\xi}{H}$ for all $x, y \in M$. In particular, $0 \le \omega(x^{*}x) = \dpn{zx\xi, x\xi}{H}$ for all $x \in M$, so $z \ge 0$. Moreover, for any $x, y, t \in M$,

\[\dpn{ztx\xi, y\xi}{H}= \omega(y^{*}tx) = \omega((t^{*}y)^{*}x) = \dpn{zx\xi, t^*y\xi}{H}= \dpn{tzx\xi, y\xi}{H}\]

so $z \in M'_{+}$. Finally, let $p: H \to \ol{M\xi}$ be the orthogonal projection onto $\ol{M\xi}$, and $x' = (zp)^{1/2}\in M'$, then for each $x \in M$,

\[\omega(x) = \dpn{zx\xi, \xi}{H}= \dpn{zpx\xi, \xi}{H}= \dpn{x(zp)^{1/2}\xi, (zp)^{1/2}\xi}{H}\]

$\square$

Lemma 43.4.3.label Let $H$ be a complex Hilbert space, $M \subset B(H)$ be a von Neumann algebra, and $\varphi: M \to \complex$ be a positive linear functional. If for any mutually orthogonal projections $\mathcal{P}\subset M$, $\varphi\paren{\sum_{p \in \mathcal{P}}p}= \sum_{p \in \mathcal{P}}\varphi(p)$, then there exist a non-zero projection $p \in M$ and $\xi \in pH$ such that $\varphi(x) = \dpn{x\xi, \xi}{H}$ for all $x \in pMp$.

Proof, [Lemma 2.5.6., AP]. Let $\eta \in H$ with $\varphi(1_{M}) < \dpn{\eta, \eta}{H}$. Let $\mathcal{P}\subset M$ be a maximal family of mutually orthogonal projections with $\varphi(p) \ge \dpn{p\eta, \eta}{H}$ for all $p \in \mathcal{P}$. By assumption,

\begin{align*}\varphi\paren{\sum_{p \in \mathcal{P}}p}&\ge \angles{\sum_{p \in \mathcal{P}}p\eta, \eta}_{H} \\ \varphi\paren{1_M - \sum_{p \in \mathcal{P}}p}&= \varphi(1_{M}) - \varphi\paren{\sum_{p \in \mathcal{P}}p}\\&< \dpn{\eta, \eta}{H}- \angles{\sum_{p \in \mathcal{P}}p\eta, \eta}_{H} \ge 0\end{align*}

Let $p := 1_{M} - \sum_{q \in \mathcal{P}}q > 0$, then by maximality of $\mathcal{P}$, $\varphi(q) < \dpn{q\eta, \eta}{H}$ for all subprojections $q \le p$.

Let $x \in (pMp)_{+}$ with $0 \le x \le 1$. By Theorem 43.7.2, there exist projections $\seq{q_n}\subset pMp$ such that $x = \sum_{n = 1}^{\infty} \frac{q_{n}}{2^{n}}$. In which case[1],

\[\dpn{x\eta, \eta}{H}= \sum_{n = 1}^{\infty} 2^{-n}\dpn{q_n\eta, \eta}{H}\ge \sum_{n = 1}^{\infty} \frac{\varphi(q_{n})}{2^{n}}= \varphi(x)\]

Therefore $\dpn{x\eta, \eta}{H}\ge \varphi(x)$ for all $x \in (pMp)_{+}$. By the Radon-Nikodym theorem for positive functionals, there exists $\xi \in pH$ with $\varphi(x) = \dpn{x\xi, \xi}{H}$ for all $x \in pMp$.$\square$

Definition 43.4.4 (Normal Linear Functional).label Let $H$ be a complex Hilbert space, $M \subset B(H)$ be a von Neumann algebra, and $\omega: M \to \complex$ be a positive linear functional, then the following are equivalent:

  1. (1)

    For any bounded, upward-directed family $A \subset M$, $\omega(\sup(A)) = \sup(\omega(A))$.

  2. (2)

    For any mutually orthogonal projections $\mathcal{P}\subset M$, $\omega\paren{\sum_{p \in \mathcal{P}}p}= \sum_{p \in \mathcal{P}}\omega(p)$.

  3. (3)

    $\omega$ is the norm limit of a sequence of weak-operator continuous positive linear functionals.

  4. (4)

    $\omega$ is weak-operator continuous on bounded subsets of $M$.

  5. (5)

    $\omega$ is strong-operator continuous on bounded subsets of $M$.

Proof, [Theorem 2.5.5, AP]. (2) $\Rightarrow$ (3): Let $\mathcal{P}\subset M$ be a maximal family of mutually orthogonal projections such that for each $p \in \mathcal{P}$, there exists $\xi_{p} \in pH$ such that $\omega(x) = \dpn{x\xi_p, \xi_p}{H}$ for all $x \in pMp$. Let $q = \sum_{p \in \mathcal{P}}p$, then by maximality of $\mathcal{P}$ and Lemma 43.4.3 applied to $(1 - q)M(1 - q)$, $\sum_{p \in \mathcal{P}}p = 1_{M}$.

For each $x \in M$ and $p \in \mathcal{P}$, by the Cauchy-Schwarz inequality,

\[|\omega(xp)|^{2} \le \omega(1) \cdot \omega(px^{*}xp) = \omega(1) \cdot \norm{x\xi_p}_{H}^{2}\]

so the mapping $y \xi_{p} \mapsto \omega(yp)$ extends into a bounded linear functional on $\ol{M\xi_p}$. By the Riesz Representation Theorem, there exists $\eta_{p} \in \ol{M\xi_p}$ such that $\omega(xp) = \dpn{x\xi_p, \eta_p}{H}$ for all $x \in M$.

Let $\mathcal{F}\subset 2^{\mathcal{P}}$ be the collection of all finite subsets of $\mathcal{P}$, directed by inclusion. For each $F \in \mathcal{F}$, let $q_{F} = \sum_{p \in F}p$ and $\omega_{F} \in M^{*}$ be defined by $\omega_{F}(x) = \omega(q_{F}xq_{F})$, then for each $x \in M$,

\[\omega_{F}(x) = \sum_{p \in F}\omega(q_{F}xp) = \sum_{p \in F}\dpn{q_Fx\xi_p, \eta_p}{H}\]

so $\omega_{F}$ is weak-operator continuous. Finally, for any $x \in M$,

\begin{align*}|\omega(x) - \omega_{F}(x)|&\le |\omega(x) - \omega(xq_{F})| + |\omega(xq_{F}) - \omega(q_{F}xq_{F})| \\&= |\omega(x(1_{M} - q_{F}))| + |\omega((1 - q_{F})xq_{F})| \\&\le 2\norm{x}_{M}\omega(1)^{1/2}\cdot \omega(1 - q_{F})^{1/2}\end{align*}

By (2), $\lim_{F \in \mathcal{F}}\omega(1 - q_{F})^{1/2}= 0$. Therefore $\omega = u\text{-}\lim_{F \in \mathcal{F}}\omega_{F}$.$\square$

Lemma 43.4.5.label Let $M$ be a von Neumann algebra, $\varphi, \omega \in M^{*}$ be positive linear functionals. If $\omega$ is normal and $\varphi \le \omega$, then $\varphi$ is also normal.

Proof. By (2) of Definition 43.4.4.$\square$

Definition 43.4.6 (Normal Positive Map).label Let $M, N$ be von Neumann algebras and $\phi: M \to N$ be a positive linear map, then the following are equivalent:

  1. (1)

    For any bounded, upward-directed family $A \subset M$, $\phi(\sup(A)) = \sup(\phi(A))$.

  2. (2)

    For any normal, positive linear functional $\omega \in N^{*}$, $\omega \circ \phi$ is a normal, positive linear functional.

  3. (3)

    $\phi$ restricted to bounded subsets of $M$ is continuous with respect to the weak operator topologies.

If $\phi$ is in addition a *-homomorphism, then the above are also equivalent to

  1. (4)

    $\phi$ restricted to bounded subsets of $M$ is continuous with respect to the strong operator topologies.

If the above holds, then $\phi$ is normal.

Proof, [Proposition 2.5.8, AP]. (2) $\Rightarrow$ (3): Let $\omega \in N^{*}$ be a weak-operator continuous functional. By Lemma 43.4.1, there exist positive weak-operator continuous functionals $\bracsn{\omega_k}_{0}^{3}$ such that $\omega = \sum_{k = 0}^{3} i^{k} \omega_{k}$. By assumption, $\omega_{k} \circ \phi$ is weak-operator continuous on bounded subsets of $M$. In which case, $\omega \circ \phi = \sum_{k = 0}^{3} i^{k} \omega_{k} \circ \phi$ is weak-operator continuous on bounded subsets of $M$. Therefore $\phi$ is weak-operator continuous on bounded subsets of $M$.

(3) $\Rightarrow$ (1), (4) $\Rightarrow$ (1): By (1) of Theorem 43.3.1.

(3) $\Rightarrow$ (4)[2]: Suppose that $M$ acts on the Hilbert space $H$, and $N$ acts on the Hilbert space $K$. Let $\angles{x_\alpha}_{\alpha \in A}\subset M$ be a bounded net converging to $x \in M$ in the strong operator topology, then for each $\xi \in H$,

\[\lim_{\alpha \in A}\dpn{(x - x_\alpha)^*(x - x_\alpha)\xi, \xi}{H}= \lim_{\alpha \in A}\normn{(x - x_\alpha)\xi}_{H}^{2} = 0\]

By polarisation, $\wotlim_{\alpha \in A}(x - x_{\alpha})^{*}(x - x_{\alpha}) = 0$. As $\angles{x_\alpha}_{\alpha \in A}$ is bounded,

\[\wotlim_{\alpha \in A}\phi((x - x_{\alpha})^{*}(x - x_{\alpha})) = 0\]

as well. In particular, for any $\xi \in K$,

\[\lim_{\alpha \in A}\norm{\phi(x - x_\alpha)\xi}_{K}^{2} = \lim_{\alpha \in A}\dpn{\phi(x - x_\alpha)^*\phi(x - x_\alpha)\xi, \xi}{K}= 0\]

Therefore $\phi$ restricted to bounded subsets of $M$ is strong-operator continuous.$\square$

Proposition 43.4.7.label Let $M, N$ be von Neumann algebras, then every isomorphism $\phi: M \to N$ is normal. In particular, the weak and strong operator topologies on $M$, restricted to bounded subsets, are independent of its representation.

Proof. As $\phi$ is an isomorphism, it is an order isomorphism. By (1) of Definition 43.4.6, $\phi$ is normal. By (3) and (4) of Definition 43.4.6, its restriction to bounded subsets of $M$ is both weak-operator and strong-operator continuous.$\square$

Proposition 43.4.8.label Let $M, N$ be von Neumann algebras, $\omega \in M^{*}$ and $\psi \in N^{*}$ be normal positive linear functionals with $\psi$ being faithful, and $\phi: M \to N$ be a positive linear map with $\psi \circ \phi \le \omega$, then $\phi$ is normal.

Proof, [Proposition 2.5.11, AP]. Let $\varphi = \psi \circ \phi \le \omega$, then $\varphi$ is normal by Lemma 43.4.5. For any bounded, upward-directed family $A \subset M$,

\[\psi(\sup(\phi(A))) =\sup(\psi(\phi(A))) = \sup(\varphi(A)) = \varphi(\sup(A)) = \psi(\phi(\sup(A)))\]

As $\psi$ is faithful, $\sup(\phi(A)) = \phi(\sup(A))$. Therefore $\phi$ is normal by (1) of Definition 43.4.6.$\square$

Proposition 43.4.9.label Let $M$ be a von Neumann algebra, $H$ be a complex Hilbert space, and $\pi: M \to B(H)$ be a normal unital *-homomorphism, then $\pi(M)$ is a von Neumann algebra.

Proof. Let $N = \pi(M)''$ be the von Neumann algebra generated by $\pi(M)$. By the Kaplansky Density Theorem, $\ol{B_N(0, 1)}^{B(H)}= \ol{B_{\pi(M)}(0, 1)}^{\text{\small WOT}}$. By Proposition 5.16.3 and Proposition 43.1.3, $\ol{B_M(0, 1)}^{M}$ is weak-operator compact, so $\pi(\ol{B_M(0, 1)}^{M})$ is weak-operator compact and contains $\pi(B_{M}(0, 1))$. Thus

\[\ol{B_{\pi(M)}(0, 1)}^{B(H)}\supset \pi(\ol{B_M(0, 1)}^{M}) \supset \ol{B_{\pi(M)}(0, 1)}^{\text{\small WOT}}\supset \ol{B_N(0, 1)}^{B(H)}\]

and $\ol{B_{\pi(M)}(0, 1)}^{B(H)}= \ol{B_{N}(0, 1)}^{B(H)}$, so $\pi(M) = \ol{\pi(M)}^{B(H)}= N$ by Theorem 39.13.3.$\square$

Lemma 43.4.10.label Let $M$ be a von Neumann algebra, $\varphi \in S(M)$ be a state, and $(H, \pi, \xi)$ be the GNS triple associated with $\varphi$, then $\pi$ is normal if and only if $\varphi$ is normal. In which case, $\pi(M) \subset B(H)$ is a von Neumann algebra.

Proof. (1): Suppose that $\varphi$ is normal. Since $\pi(M)\xi$ is dense in $H$, the Arzelà-Ascoli Theorem implies that the weak operator topology on $\ol{B_{\pi(M)}(0, 1)}$ coincides with the topology of pointwise convergence on $\bracsn{\eta \otimes \theta|\eta, \theta \in \pi(M)\xi}$. For each $x, y, z \in M$,

\[\dpn{\pi(x)\pi(y)\xi, \pi(z)\xi}{H}= \dpn{\pi(z^*)\pi(x)\pi(y)\xi, \xi}{H}= \varphi(z^{*}xy)\]

By separate continuity of composition in the weak operator topology, the functional $x \mapsto \dpn{\pi(x)\pi(y)\xi, \pi(z)\xi}{H}$ is weak-operator continuous. As such, $\pi|_{\ol{B_M(0, 1)}}: \ol{B_M(0, 1)}\to \ol{B_{\pi(M)}(0, 1)}$ is weak-operator continuous.

(2): By Proposition 43.4.9.$\square$

Definition 43.4.11 (Separable).label Let $M$ be a von Neumann algebra, then $M$ is separable if there exists a separable Hilbert space $H$ and a faithful normal representation $\pi: M \to B(H)$.

  1. Here, only continuity of $\varphi$ is used.keyboard_return
  2. Central here is the observation that $x_{\alpha} \to 0$ in the strong operator topology i.f.f. $x_{\alpha}^{*}x_{\alpha} \to 0$ in the weak operator topology. keyboard_return

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