306 lines
8.3 KiB
TeX
306 lines
8.3 KiB
TeX
\documentclass[9pt,aspectratio=169]{beamer}
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\usepackage[utf8]{inputenc}
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\usepackage[T1]{fontenc}
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\usepackage{hyperref}
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\usepackage{amsmath,amssymb,amsfonts,graphicx,xcolor,bm,microtype,wasysym,hyperref,tabularx,amscd,mhchem,physics}
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\definecolor{darkgreen}{RGB}{0, 180, 0}
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\definecolor{fooblue}{RGB}{0,153,255}
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\definecolor{fooyellow}{RGB}{234,180,0}
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\definecolor{lavender}{rgb}{0.71, 0.49, 0.86}
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\definecolor{inchworm}{rgb}{0.7, 0.93, 0.36}
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\newcommand{\violet}[1]{\textcolor{lavender}{#1}}
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\newcommand{\orange}[1]{\textcolor{orange}{#1}}
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\newcommand{\purple}[1]{\textcolor{purple}{#1}}
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\newcommand{\blue}[1]{\textcolor{blue}{#1}}
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\newcommand{\green}[1]{\textcolor{darkgreen}{#1}}
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\newcommand{\yellow}[1]{\textcolor{fooyellow}{#1}}
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\newcommand{\red}[1]{\textcolor{red}{#1}}
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\newcommand{\highlight}[1]{\textcolor{fooblue}{#1}}
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\newcommand{\pub}[1]{\textcolor{purple}{#1}}
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\newcommand{\bC}{\boldsymbol{C}}
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\newcommand{\bF}{\boldsymbol{F}}
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\newcommand{\bH}{\boldsymbol{H}}
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\newcommand{\bHd}{\boldsymbol{H}_\text{d}}
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\newcommand{\bHod}{\boldsymbol{H}_\text{od}}
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\newcommand{\bO}{\boldsymbol{0}}
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\newcommand{\bI}{\boldsymbol{1}}
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\newcommand{\bV}{\boldsymbol{V}}
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\newcommand{\bEta}{\boldsymbol{\eta}}
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\newcommand{\bSig}{\boldsymbol{\Sigma}}
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\newcommand{\bpsi}{\boldsymbol{\psi}}
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\newcommand{\bPsi}{\boldsymbol{\Psi}}
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\institute{Laboratoire de Chimie et Physique Quantiques, IRSAMC, UPS/CNRS, Toulouse \\
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\url{https://lcpq.github.io/pterosor}}
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\usetheme{pterosor}
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\author{Antoine Marie \& Pierre-Fran\c{c}ois Loos}
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\date{14th November 2022}
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\title{Similarity Renormalization Group (SRG) Formalism Applied to Green's Function Methods}
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\begin{document}
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\maketitle
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%-----------------------------------------------------
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\begin{frame}{First-Quantized Form of SRG}
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\begin{block}{General upfolded many-body perturbation theory (MBPT) problem}
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\begin{align}
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\qty[ \bF + \bSig(\omega) ] \bpsi = \omega \bpsi
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& \qq{$\Leftrightarrow$}
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\bH \bPsi = \omega \bPsi
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\\
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\bSig(\omega) = \bV \qty(\omega \bI - \bC)^{-1} \bV^{\dag}
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& \qq{$\Leftrightarrow$}
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\bH =
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\begin{pmatrix}
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\bF & \bV
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\\
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\bV^{\dagger} & \bC
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\end{pmatrix}
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\end{align}
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\end{block}
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%
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\begin{block}{Perturbative partitioning}
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\begin{equation}
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\bH \equiv \bH(s=0) =
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\underbrace{
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\begin{pmatrix}
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\bF & \bO
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\\
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\bO & \bC
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\end{pmatrix}
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}_{\bHd^{(0)}(s=0)}
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+ \lambda
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\underbrace{
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\begin{pmatrix}
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\bO & \bV
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\\
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\bV^{\dagger} & \bO
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\end{pmatrix}
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}_{\bHod^{(1)}(s=0)}
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\qq{with}
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\bHd^{(1)}(s=0) = \bHod^{(0)}(s=0) = \bO
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\end{equation}
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\end{block}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{Perturbative Expansions}
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%
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\begin{block}{Perturbative partitioning in the SRG framework}
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\begin{equation}
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\bH(s) =
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\underbrace{
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\begin{pmatrix}
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\bF(s) & \bO
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\\
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\bO & \bC(s)
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\end{pmatrix}
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}_{\bHd{}(s)}
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+ \lambda
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\underbrace{
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\begin{pmatrix}
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\bO & \bV(s)
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\\
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\bV^{\dagger}(s) & \bO
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\end{pmatrix}
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}_{\bHod(s)}
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\end{equation}
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\end{block}
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%
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\begin{block}{Components of the Hamiltonian}
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\begin{equation}
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\bH(s) = \bH^{(0)}(s) + \lambda \bH^{(1)}(s) + \lambda^2 \bH^{(2)}(s) + \cdots
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\end{equation}
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\begin{equation}
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\bC(s) = \bC^{(0)}(s) + \lambda \bC^{(1)}(s) + \lambda^2 \bC^{(2)}(s) + \cdots
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\end{equation}
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\begin{equation}
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\bV(s) = \bV^{(0)}(s) + \lambda \bV^{(1)}(s) + \lambda^2 \bV^{(2)}(s) + \cdots
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\end{equation}
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\end{block}
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\begin{block}{Wegner generator}
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\begin{equation}
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\bEta(s) = \bEta^{(0)}(s) + \lambda \bEta^{(1)}(s) + \lambda^2 \bEta^{(2)}(s) + \cdots
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\end{equation}
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\end{block}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{Zeroth-Order Terms}
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\begin{block}{Wegner generator}
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\begin{equation}
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\bEta^{(0)}(s)
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= \comm{\bHd^{(0)}(s)}{\bHod^{(0)}(s)}
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= \bO
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\end{equation}
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\end{block}
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%
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\begin{block}{Zeroth-order Hamiltonian}
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\begin{equation}
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\dv{\bH^{(0)}(s)}{s}
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= \comm{\bEta^{(0)}(s)}{\bH^{(0)}(s)}
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= \bO
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\qq{$\Rightarrow$}
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\bH^{(0)}(s) = \bH^{(0)}{(s=0)}
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\end{equation}
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\end{block}
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\alert{NB: we omit the $s$ dependency from hereon}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{First-Order Terms}
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\begin{block}{Wegner generator}
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\begin{equation}
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\bEta^{(1)} = \comm{\bHd^{(0)}}{\bHod^{(1)}}
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=
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\begin{pmatrix}
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\bO & \bF^{(0)} \bV^{(1)} - \bV^{(1)} \bC^{(0)}
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\\
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\bC^{(0)} \bV^{(1),\dagger} - \bV^{(1),\dagger} \bF^{(0)} & \bO
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\end{pmatrix}
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\end{equation}
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\end{block}
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%
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\begin{block}{First-order Hamiltonian}
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\begin{equation}
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\dv{\bH^{(1)}}{s} = \comm{\bEta^{(1)}}{\bHd^{(0)}}
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=
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\begin{pmatrix}
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\dv{\bF^{(1)}}{s} & \dv{\bV^{(1)}}{s}
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\\
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\dv{\bV^{(1),\dagger}}{s} & \dv{\bC^{(1)}}{s}
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\end{pmatrix}
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\end{equation}
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with
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\begin{gather}
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\dv{\bF^{(1)}}{s}
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= \dv{\bC^{(1)}}{s}
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= \bO
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\\
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\dv{\bV^{(1)}}{s}
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= 2 \bF^{(0)} \bV^{(1)} \bC^{(0)}
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- \qty[\bF^{(0)}]^2 \bV^{(1)}
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- \bV^{(1)} \qty[\bC^{(0)}]^2
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\end{gather}
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\end{block}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{Second-Order Terms}
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\begin{block}{Wegner generator}
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\begin{equation}
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\bEta^{(2)}
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= \comm{\bHd^{(0)}}{\bHod^{(2)}}
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+ \underbrace{\comm{\bHd^{(1)}}{\bHod^{(1)}}}_{=\bO}
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=
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\begin{pmatrix}
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\bO & \bF^{(0)} \bV^{(2)} - \bV^{(2)} \bC^{(0)}
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\\
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\bC^{(0)} \bV^{(2),\dagger} - \bV^{(2),\dagger} \bF^{(0)} & \bO
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\end{pmatrix}
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\end{equation}
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\end{block}
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%
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\begin{block}{Second-order Hamiltonian}
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\begin{equation}
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\dv{\bH^{(2)}}{s} = \comm{\bEta^{(2)}}{\bHd^{(0)}} + \comm{\bEta^{(1)}}{\bHd^{(1)}}
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=
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\begin{pmatrix}
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\dv{\bF^{(2)}}{s} & \dv{\bV^{(2)}}{s}
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\\
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\dv{\bV^{(2),\dagger}}{s} & \dv{\bC^{(2)}}{s}
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\end{pmatrix}
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\end{equation}
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with
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\begin{gather}
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\dv{\bF^{(2)}}{s}
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= \bF^{(0)} \bV^{(1)} \bV^{(1),\dag}
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+ \bV^{(1)} \bV^{(1),\dag} \bF^{(0)}
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- 2 \bV^{(1)} \bC^{(0)} \bV^{(1),\dag}
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\\
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\dv{\bC^{(2)}}{s}
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= \bC^{(0)} \bV^{(1)} \bV^{(1),\dag}
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+ \bV^{(1)} \bV^{(1),\dag} \bC^{(0)}
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- 2 \bV^{(1)} \bF^{(0)} \bV^{(1),\dag}
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\\
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\dv{\bV^{(2)}}{s}
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= 2 \bF^{(0)} \bV^{(2)} \bC^{(0)}
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- \qty[\bF^{(0)}]^2 \bV^{(2)}
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- \bV^{(2)} \qty[\bC^{(0)}]^2
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\end{gather}
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\end{block}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{Integration of the First-Order Terms}
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\begin{equation}
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\dv{\bF^{(1)}}{s} = \bO
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\land
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\bF^{(1)}(0) = \bO
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\Rightarrow
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\bF^{(1)}(s) = \bO
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\end{equation}
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\begin{equation}
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\dv{\bC^{(1)}}{s}
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\land
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\bC^{(1)}(0) = \bO
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\Rightarrow
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\bC^{(1)}(s) = \bO
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\end{equation}
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\begin{equation}
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\dv{\bV^{(1)}}{s}
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= 2 \bF^{(0)} \bV^{(1)} \bC^{(0)}
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- \qty[\bF^{(0)}]^2 \bV^{(1)}
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- \bV^{(1)} \qty[\bC^{(0)}]^2
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\land
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\Rightarrow
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\bV^{(1)}(s) = ?
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\end{equation}
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\end{frame}
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%-----------------------------------------------------
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%-----------------------------------------------------
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\begin{frame}{Integration of the Second-Order Terms}
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\begin{equation}
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\dv{\bF^{(2)}}{s}
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= \bF^{(0)} \bV^{(1)} \bV^{(1),\dag}
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+ \bV^{(1)} \bV^{(1),\dag} \bF^{(0)}
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- 2 \bV^{(1)} \bC^{(0)} \bV^{(1),\dag}
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\land
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\bF^{(2)}(0) = ?
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\Rightarrow
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\bF^{(2)}(s) = ?
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\end{equation}
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\begin{equation}
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\dv{\bC^{(2)}}{s}
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= \bC^{(0)} \bV^{(1)} \bV^{(1),\dag}
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+ \bV^{(1)} \bV^{(1),\dag} \bC^{(0)}
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- 2 \bV^{(1)} \bF^{(0)} \bV^{(1),\dag}
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\land
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\bC^{(2)}(0) = ?
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\Rightarrow
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\bC^{(2)}(s) = ?
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\end{equation}
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\begin{equation}
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\dv{\bV^{(2)}}{s}
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= 2 \bF^{(0)} \bV^{(2)} \bC^{(0)}
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- \qty[\bF^{(0)}]^2 \bV^{(2)}
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- \bV^{(2)} \qty[\bC^{(0)}]^2
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\land
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\Rightarrow
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\bV^{(2)}(s) = ?
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\end{equation}
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\end{frame}
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%-----------------------------------------------------
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\end{document}
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