\documentclass{standalone} \usepackage{amsmath,amssymb,amsfonts,pgfpages,graphicx,subfigure,xcolor,bm,multirow,microtype,wasysym,multimedia,hyperref,tabularx,amscd,pgfgantt,mhchem,physics} \usetikzlibrary{shapes.gates.logic.US,trees,positioning,arrows} \usepackage{tgchorus} \usepackage[T1]{fontenc} \begin{document} \begin{tikzpicture} \begin{scope}[very thick, node distance=5cm,on grid,>=stealth', theo1/.style={rectangle,draw,fill=red!20}, theo2/.style={rectangle,draw,fill=orange!20}, theo3/.style={rectangle,draw,fill=green!40}, exp1/.style={rectangle,draw,fill=cyan!40}, exp2/.style={rectangle,draw,fill=violet!40}] \node [theo1, text width=7cm, align=center] (KS) {\textbf{\LARGE Kohn-Sham DFT} $$ \qty[ -\frac{\nabla^2}{2} + v_\text{ext} + V^{\text{Hxc}} ] \phi_p^{\text{KS}} = \varepsilon^{\text{KS}}_p \phi_p^{\text{KS}} $$ }; \node [theo2, text width=7cm, align=center] (GW) [below=of KS, yshift=2cm] {\textbf{\LARGE $GW$ approximation} $$ \varepsilon_p^{GW} = \varepsilon_p^{\text{KS}} + \mel{\phi_p^{\text{KS}}}{\Sigma^{GW}(\varepsilon_p^{GW}) - V^{\text{xc}}}{\phi_p^{\text{KS}}} $$ }; \node [theo3, text width=7cm, align=center] (BSE) [below=of GW, yshift=2cm] {\textbf{\LARGE Bethe-Salpeter equation} $$ \begin{pmatrix} \bm{A} & \bm{B} \\ -\bm{B}^* & -\bm{A}^{*} \end{pmatrix} \begin{pmatrix} \bm{X}_m \\ \bm{Y}_m \end{pmatrix} = \Omega_{m} \begin{pmatrix} \bm{X}_m \\ \bm{Y}_m \end{pmatrix} $$ }; \node [exp1, align=center] (photo) [right=of GW, xshift=3cm] {\LARGE (Inverse) \\ \LARGE photoemission \\ \LARGE spectroscopy}; \node [exp2, align=center] (abs) [right=of BSE, xshift=3cm] {\LARGE Optical \\ \LARGE spectroscopy}; \path (KS) edge [->,color=black] node [right,black] {\LARGE Fundamental gap} (GW) (GW) edge [->,color=black] node [right,black] {\LARGE Excitonic effect} (BSE) (photo) edge [<->,color=black] node [above,black] {Ionization potentials} node [below,black] {Electron affinities} (GW) (abs) edge [<->,color=black] node [above,black] {Optical excitations} (BSE) ; \end{scope} \end{tikzpicture} \end{document}