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Let $T$ be a self-adjoint strict contraction ($||Tx||<||x||$ for all $x\in H\setminus\{0\}$ where $H$ is a Hilbert space). One observe that the expression $T\sqrt{I-T^2}^{-1}$ is well-defined on the range of $\sqrt{(I-T^2)}^{-1}$. Can someone help me to prove that $T\sqrt{I-T^2}^{-1}$ is self-adjoint on this domain?

Thanks a lot

freishahiri
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The operator $I-T^{2}$ is positive because $$ ((I-T^{2})x,x) = \|x\|^{2}-\|Tx\|^{2} \ge 0 $$ with equality iff $x=0$. So there is a unique $\sqrt{I-T^{2}} \ge 0$ that is non-negative and commutes with every bounded operator that commutes with $T$. This square root is injective because $$ \|\sqrt{I-T^{2}}x\|^{2}=((I-T^{2})x,x)=\|x\|^{2}-\|Tx\|^{2}. $$ The range of $\sqrt{I-T^{2}}$ is dense in $H$ because $$ \mathcal{R}(\sqrt{I-T^{2}})^{\perp}=\mathcal{N}(\sqrt{I-T^{2}})=\{0\}. $$ Let $S=\sqrt{I-T^{2}}^{-1}$ on $\mathcal{D}(S)=\mathcal{R}(\sqrt{I-T^{2}})$. Then $S$ is a densely-defined selfadjoint linear operator, which follows from general results relating inverses and adjoints: $$ S^{\star}=(\sqrt{I-T^{2}}^{-1})^{\star}=(\sqrt{I-T^{2}}^{\star})^{-1}=S. $$ Because $T$ commutes with $\sqrt{I-T^{2}}$, then $$ T\sqrt{I-T^{2}}=\sqrt{I-T^{2}}T \\ Tx = \sqrt{I-T^{2}}TSx, \;\;\; x\in\mathcal{D}(S) $$ It follows that $T : \mathcal{D}(S)\rightarrow \mathcal{D}(S)$ and $$ STx = TSx, \;\;\; x\in\mathcal{D}(S). $$ It is conceivable that $STx$ is defined for more $x$ than is $TSx$, but it turns out this is not the case. Indeed, suppose $Tx \in \mathcal{D}(S)$; equivalently, there exists $y$ such that $$ Tx = \sqrt{I-T^{2}}y, $$ which can be rewritten as $$ T^{2}x = T\sqrt{I-T^{2}}y=\sqrt{I-T^{2}}Ty,\\ (I-T^{2})x = x-\sqrt{I-T^{2}}Ty, \\ \sqrt{I-T^{2}}\left\{\sqrt{I-T^{2}}x+Ty\right\}=x \\ \implies x \in \mathcal{D}(S). $$ So $x \in \mathcal{D}(S)$ iff $Tx \in \mathcal{D}(S)$ and, for any such $x$, $$ TSx = STx,\;\;\; x\in\mathcal{D}(S). $$ The operator $TS$ is symmetric on $\mathcal{D}(S)$ because $x,y\in\mathcal{D}(S)$ implies $$ (TSx,y) = (STx,y) = (Tx,Sy)=(x,TSy). $$ Therefore, $TS \preceq (TS)^{\star}$, meaning that the graph of $TS$ is a subspace of the graph of $(TS)^{\star}$. Conversely, suppose $y \in \mathcal{D}((TS)^{\star})$. Then $$ ((TS)x,y) = (x,(TS)^{\star}y),\;\;\; x\in\mathcal{D}(S),\\ (Sx,Ty) = (x,(TS)^{\star}y),\;\;\; x\in\mathcal{D}(S), \\ \implies Ty \in \mathcal{D}(S^{\star})=D(S) \mbox{ and } STy = (TS)^{\star}y. $$ By what has been shown, $Ty \in \mathcal{D}(S)$ iff $y \in \mathcal{D}(S)$ and, in that case, $TSy = STy = (TS)^{\star}y$. Therefore $$ (TS)^{\star} \preceq TS. $$ So $(TS)^{\star}=(TS)$ follows from $TS \preceq (TS)^{\star} \preceq TS$.

Disintegrating By Parts
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