Definition 43.8.10 (Absolute Value).label Let $H$ be a complex Hilbert space, $T: D(T) \to H$ be a closed, densely defined linear operator, and $|T| = (T^{*}T)^{1/2}: D(|T|) \to H$, then:
- (1)
$|T|$ is a densely defined, self-adjoint, and positive operator.
- (2)
Equip $D(T)$ with the inner product $\dpn{\xi, \eta}{D(T)}= \dpn{\xi, \eta}{H}+ \dpn{T\xi, T\eta}{H}$, then $D(T)$ is a Hilbert space with $D(T^{*}T)$ being dense in $D(T)$.
- (3)
Equip $D(|T|)$ with the inner product $\dpn{\xi, \eta}{D(|T|)}= \dpn{\xi, \eta}{H}+ \dpn{|T|\xi, |T|\eta}{H}$, then $D(|T|)$ is a Hilbert space with $D(T^{*}T)$ being dense in $D(|T|)$.
- (4)
$D(T) = D(|T|)$.
- (5)
For each $\xi \in D(T) = D(|T|)$, $\normn{T\xi}_{H} = \norm{|T|\xi}_{H}$. In particular, $\ker T = \ker |T|$.
The operator $|T|$ is the absolute value of $T$.
Proof. (1): By von Neumann’s theorem, $T^{*}T: D(T^{*}T) \to H$ is a densely defined, self-adjoint, and positive operator. Thus $|T| = (T^{*}T)^{1/2}$ is well-defined, self-adjoint, and positive via the spectral theorem.
(2): By definition, $D(T)$ is isomorphic to the graph of $T$, which is a Hilbert space given that $T$ is closed.
Let $\xi \in D(T)$ with $\xi \perp D(T^{*}T)$, then for each $\eta \in D(T^{*}T)$,
By (2) of Lemma 43.8.8, $(I+T^{*}T): D(T^{*}T) \to H$ is surjective, so $\xi = 0$, and $D(T^{*}T)$ is dense in $D(T)$.
(3): By (3) of Definition 43.8.6, $|T|$ is self-adjoint, and in particular closed. Since $D(T)$ is isomorphic to the graph of $|T|$, $D(|T|)$ is a Hilbert space. Similarly, for any $\xi \in D(|T|)$ with $\xi \perp D(T^{*}T)$ and $\eta \in D(T^{*}T)$, by the Borel functional calculus[1],
By (2) of Lemma 43.8.8, $\xi = 0$, and $D(T^{*}T)$ is dense in $D(|T|)$.
(4): For any $\xi \in D(T^{*}T)$, $\norm{\xi}_{D(T)}= \norm{\xi}_{D(|T|)}$. By (2) and (3), $D(T)$ and $D(|T|)$ are both the completions of $D(T^{*}T)$ under the same norm, so, $D(T) = D(|T|)$.
(5): For each $\xi \in D(T^{*}T)$,
By the density provided in (2) and (3), $\normn{T\xi}_{H}^{2} = \norm{|T|\xi}_{H}^{2}$ for all $\xi \in D(T)$.$\square$
- The fact that the spectral measure of a positive element is supported in $[0, \infty)$ is needed here.keyboard_return
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