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semi1.tex
\documentclass{article} \usepackage{amsfonts} \usepackage{amsmath} \usepackage{amsthm} \newtheorem{proposition}{Proposition} \begin{document} \section{Commutative models} Let $T_t$, $t\ge0$ be a centered semigroup. First we assume that the operators $T_t$ are invertible, i.e., have zero kernel and their image is the whole $H$. Write the polar decomposition, $T_t = U_tC_t$, then $C_t$ have (possibly unbounded) inverse, and $U_t$ are unitaries. Write $A_t = C_t$, $A_{-t} = U_t C_t^{-1} U_t^*$, $t\ge0$. Then $A_t$, $t\in \mathbb R$ is a commuting family of positive self-adjoint operators. \begin{proposition} The following relations hold for all $t\in \mathbb R$, $s\ge0$ \begin{align*} A_t U_s & = U_s A_{t+s} A_s^{-1}, \\ A_tU_s^* & = U_s^* A_{t-s} A_{-s}^{-1}. \end{align*} \end{proposition} \begin{proof} We have the relations \[ U_s^*C_tU_sC_s = C_sU_s^*C_tU_s,\quad C_tU_sC_sU_s^* = U_sC_sU_s^*C_t, \] and taking into account that $(U_tC_tU_t^*)^{-1} = U_tC_t^{-1}U_t^*$, we get the needed relations. \end{proof} \end{document} %%% Local Variables: %%% mode: latex %%% TeX-master: t %%% End: