\documentclass[aip,jcp,reprint,onecolumn,noshowkeys,superscriptaddress]{revtex4-1} \usepackage{graphicx,dcolumn,bm,xcolor,microtype,multirow,amscd,amsmath,amssymb,amsfonts,physics,longtable,wrapfig,txfonts} \usepackage[version=4]{mhchem} \usepackage[utf8]{inputenc} \usepackage[T1]{fontenc} \usepackage{txfonts} \usepackage{siunitx} \usepackage{soul} \DeclareSIUnit[number-unit-product = {\,}] \cal{cal} \DeclareSIUnit\kcal{\kilo\cal} \newcommand{\kcalmol}{\si{\kcal\per\mole}} \usepackage[ colorlinks=true, citecolor=blue, breaklinks=true ]{hyperref} \urlstyle{same} \newcommand{\ie}{\textit{i.e.}} \newcommand{\eg}{\textit{e.g.}} \newcommand{\alert}[1]{\textcolor{red}{#1}} \usepackage[normalem]{ulem} \newcommand{\titou}[1]{\textcolor{red}{#1}} \newcommand{\trashPFL}[1]{\textcolor{red}{\sout{#1}}} \newcommand{\trashXB}[1]{\textcolor{darkgreen}{\sout{#1}}} \newcommand{\PFL}[1]{\titou{(\underline{\bf PFL}: #1)}} \newcommand{\mc}{\multicolumn} \newcommand{\fnm}{\footnotemark} \newcommand{\fnt}{\footnotetext} \newcommand{\tabc}[1]{\multicolumn{1}{c}{#1}} \newcommand{\SupInf}{\textcolor{blue}{supporting information}} \newcommand{\QP}{\textsc{quantum package}} \newcommand{\T}[1]{#1^{\intercal}} %% bold in Table \newcommand{\bb}[1]{\textbf{#1}} \newcommand{\rb}[1]{\textbf{\textcolor{red}{#1}}} \newcommand{\gb}[1]{\textbf{\textcolor{darkgreen}{#1}}} %geometries \newcommand{\Dtwo}{$D_{2h}$} \newcommand{\Dfour}{$D_{4h}$} \sisetup{range-phrase=--} \sisetup{range-units=single} %states %D2h states \newcommand{\oneAg}{$1{}^1A_g$} \newcommand{\tBoneg}{$1{}^3B_{1g}$} \newcommand{\sBoneg}{$1{}^1B_{1g}$} \newcommand{\twoAg}{$2{}^1A_g$} %D4h states %\newcommand{\oneBoneg}{$1{}^1B_{1g}$} same label as the D2h state \newcommand{\Atwog}{$1{}^3A_{2g}$} \newcommand{\Aoneg}{$1{}^1A_{1g}$} \newcommand{\Btwog}{$1{}^1B_{2g}$} % addresses \newcommand{\LCPQ}{Laboratoire de Chimie et Physique Quantiques (UMR 5626), Universit\'e de Toulouse, CNRS, UPS, France} \newcommand{\CEISAM}{4Nantes Universit\'e, CNRS, CEISAM UMR-6230, Nantes F-44000, France.} \begin{document} \title{Supporting Information for ``Reference Energies for Cyclobutadiene: Autoisomerization and Excited States''} \author{Enzo \surname{Monino}} \email{emonino@irsamc.ups-tlse.fr} \affiliation{\LCPQ} \author{Martial \surname{Boggio-Pasqua}} \affiliation{\LCPQ} \author{Anthony \surname{Scemama}} \affiliation{\LCPQ} \author{Denis \surname{Jacquemin}} \affiliation{\CEISAM} \author{Pierre-Fran\c{c}ois \surname{Loos}} \email{loos@irsamc.ups-tlse.fr} \affiliation{\LCPQ} %\maketitle %%%%%%%%%%%%%%%%%%%%%%%% \section{Geometries} %%%%%%%%%%%%%%%%%%%%%%%% Below, we provide the Cartesian coordinates (in \si{\angstrom}) of the geometries that are employed in this work. \begin{itemize} \item {\Dtwo} rectangular equilibrium geometry of the {\oneAg} ground state computed at the CASPT2(12,12)/aug-cc-pVTZ level: \begin{verbatim} C 0.0000000000 -0.6769380253 -0.7827569236 C 0.0000000000 -0.6769380253 0.7827569236 C 0.0000000000 0.6769380253 0.7827569236 C 0.0000000000 0.6769380253 -0.7827569236 H 0.0000000000 -1.4379809006 -1.5441628360 H 0.0000000000 -1.4379809006 1.5441628360 H 0.0000000000 1.4379809006 1.5441628360 H 0.0000000000 1.4379809006 -1.5441628360 \end{verbatim} %%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%% \item {\Dfour} square planar equilibrium geometry of the {\sBoneg} ground state computed at the CASPT2(12,12)/aug-cc-pVTZ level: \begin{verbatim} C 1.0248323754 0.0000000000 0.0000000000 C 0.0000000000 -1.0248323754 0.0000000000 C -1.0248323754 0.0000000000 0.0000000000 C 0.0000000000 1.0248323754 0.0000000000 H 2.1005277359 0.0000000000 0.0000000000 H 0.0000000000 -2.1005277359 0.0000000000 H -2.1005277359 0.0000000000 0.0000000000 H 0.0000000000 2.1005277359 0.0000000000 \end{verbatim} %%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%% \item {\Dtwo} rectangular equilibrium geometry of the {\oneAg} ground state computed at the CC3/aug-cc-pVTZ level: \begin{verbatim} C -0.78248546 -0.67208001 0.00000000 C 0.78248546 -0.67208001 0.00000000 C -0.78248546 0.67208001 0.00000000 C 0.78248546 0.67208001 0.00000000 H -1.54227765 -1.43404123 -0.00000000 H 1.54227765 -1.43404123 0.00000000 H -1.54227765 1.43404123 0.00000000 H 1.54227765 1.43404123 -0.00000000 \end{verbatim} %%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%% \item {\Dfour} square planar equilibrium geometry of the {\Atwog} state computed at the (RO)-CCSD(T)/aug-cc-pVTZ level: \begin{verbatim} C 0.000000 1.017702 0.000000 C 1.017702 -0.000000 0.000000 C -1.017702 0.000000 0.000000 C -0.000000 -1.017702 0.000000 H 0.000000 2.092429 0.000000 H 2.092429 -0.000000 0.000000 H -0.000000 -2.092429 0.000000 H -2.092429 0.000000 0.000000 \end{verbatim} %%%%%%%%%%%%%%%%%%%%%%%% \end{itemize} %\begin{squeezetable} \begin{table*} \caption{Energy differences between the states computed with various methods and the reference TBE values. Note that AB stands for the automerization barrier and is reported in \si{\kcalmol}. The numbers reported in parenthesis are the percentage of single excitations involved in the transition ($\%T_1$) calculated at the CC3/aug-cc-pVTZ level. The values between square brackets have been obtained by extrapolation via the procedure described in the corresponding footnote.} %\hl{On which geoms ? You give 2 pairs on previous page, but we are not sure which one are used here}} \label{tab:TBE} \begin{ruledtabular} \begin{tabular}{lrrrrrrr} %\begin{tabular}{*{1}{*{8}{l}}} & &\mc{3}{c}{{\Dtwo} excitation energies (eV)} & \mc{3}{c}{{\Dfour} excitation energies (eV)} \\ \cline{3-5} \cline{6-8} Method & AB & {\tBoneg}(99\%) & {\sBoneg}(95\%)& {\twoAg}(1\%) & {\Atwog} & {\Aoneg} & {\Btwog} \\ \hline SF-TD-B3LYP & $10.41$ & $0.241$ & $-0.926$ & $-0.050$ & $-0.164$ & $-1.028$ & $-1.316$ \\ SF-TD-PBE0 & $8.95$ & $0.220$ & $-0.829$ & $0.043$ & $-0.163$ & $-0.903$ &$-1.172$ \\ SF-TD-BH\&HLYP & $3.79$ & $0.078$ & $-0.393$ & $0.454$ & $-0.099$ & $-0.251$ & $-0.418$ \\ SF-TD-M06-2X & $1.42$ & $0.000$ & $-0.354$ & $0.319$ & $-0.066$ & $-0.097$ & $-0.247$ \\ SF-TD-CAM-B3LYP & $9.90$ & $0.280$ & $-0.807$ &$0.100$ & $-0.134$ & $-0.920$ & $-1.185$\\ SF-TD-$\omega $B97X-V & $10.01$ & $0.335$ & $-0.774$ & $0.175$ & $-0.118$ & $-0.928$ & $-1.187$ \\ SF-TD-LC-$\omega $PBE08 & $10.81$ & $0.435$ & $-0.710$ & $0.310$ & $-0.086$ & $-0.939$ & $-1.191$ \\ SF-TD-M11 & $2.29$ & $0.097$ & $-0.474$ & $0.262$ & $-0.063$ & $-0.312$ & $-0.490$ \\[0.1cm] SF-ADC(2)-s & $-0.30$ & $0.069$ & $-0.026$ & $0.093$ & $0.112$ & $0.112$ & $-0.005$ \\ SF-ADC(2)-x & $1.44$ & $0.077$ & $-0.094$ & $-0.335$ & $0.068$ & $-0.409$ & $-0.118$ \\ SF-ADC(2.5) & $0.18$ & $0.013$ & $0.006$ &$0.140$ & $0.024$ & $0.094$ & $0.000$ \\ SF-ADC(3) & $0.65$ & $-0.043$ & $0.037$ & $0.186$ & $-0.065$ & $0.075$ & $0.004$ \\[0.1cm] CASSCF(4,4) & $-1.55$ & $0.208$ & $1.421$ & $0.403$& $0.290$ & $0.734$ & $1.575$ \\ CASPT2(4,4) & $-1.16$ & $-0.050$ & $-0.202$ & $0.034$ & $-0.016$ & $0.006$ & $-0.214$ \\ %XMS-CASPT2(4,4) & & & & $-0.035$ & & & \\ SC-NEVPT2(4,4) & $0.30$ & $-0.083$ & $-0.703$ & $0.070$ & $-0.120$ & $-0.072$ & $-0.794$ \\ PC-NEVPT2(4,4) & $0.31$ & $-0.080$ & $-0.757$ & $0.045$ & $-0.118$ & $-0.097$ & $-0.846$ \\ %MRCI(4,4) & & $0.106$ & $0.553$ & $0.121$ & $0.127$ & $0.324$ & $0.381$ \\[0.1cm] CASSCF(12,12) & $2.66$ & $0.224$ & $0.719$ & $0.179$ & $0.226$ & $0.443$ & $0.785$ \\ CASPT2(12,12) & $-0.42$& $0.018$ & $0.058$ & $0.005$ & $0.039$ & $0.038$ & $0.077$ \\ %XMS-CASPT2(12,12) & & & & $-0.090$ & & & \\ SC-NEVPT2(12,12) & $-0.64$ & $0.039$ & $0.063$ & $0.048$ & $0.021$ & $0.046$ & $0.043$ \\ PC-NEVPT2(12,12) & $-0.65$ & $0.000$ & $-0.062$ & $0.018$ & $-0.013$ & $-0.024$ & $-0.093$ \\[0.1cm] CCSD & $0.95$ & $-0.145$ & $0.067$ & & $-0.059$ & $0.100$ & \\ CC3 & $-1.05$ & $-0.060$ & $-0.006$ & $0.739$ & & $0.162$ & $0.871$ \\ CCSDT & $-0.25$ & $-0.051$ & $0.014$ & $0.391$ & $0.005$ & $0.131$ & $0.688$ \\ CC4 & $-0.11$ & & $0.003$ & $0.105$ & & $0.011$ & $-0.013$ \\ CCSDTQ & $0.00$ & & $0.000$ & $0.000$ & $0.000$ & $0.000$ & $0.000$ \\[0.1cm] %CIPSI & & $-0.001\pm 0.030$ & $0.017\pm 0.035$ & $-0.120\pm 0.090$ & $0.025\pm 0.029$ & $0.130\pm 0.050$ & \\ \bf{TBE} & $[\bf{8.93}]$\fnm[1] & $[\bf{1.462}]$\fnm[2] & $[\bf{3.125}]$\fnm[3] & $[\bf{4.038}]$\fnm[3] & $[\bf{0.144}]$\fnm[4] & $[\bf{1.500}]$\fnm[3] & $[\bf{1.849}]$\fnm[3] \\[0.1cm] Literature & $8.53$\fnm[5] & $1.573$\fnm[5] & $3.208$\fnm[5] & $4.247$\fnm[5] & $0.266$\fnm[5] & $1.664$\fnm[5] & $1.910$\fnm[5] \\ & $10.35$\fnm[6] & $1.576$\fnm[6] & $3.141$\fnm[6] & $3.796$\fnm[6] & $0.217$\fnm[6] & $1.123$\fnm[6] & $1.799$\fnm[6]\\ & $9.58$\fnm[7]& $1.456$\fnm[7] & $3.285$\fnm[7] & $4.334$\fnm[7] & $0.083$\fnm[7] & $1.621$\fnm[7] & $1.930$\fnm[7] \\ & $7.48$\fnm[8]& $1.654$\fnm[8] & $3.416$\fnm[8] & $4.360$\fnm[8] & $0.369$\fnm[8] & $1.824$\fnm[8] & $2.143$\fnm[8] \\ \end{tabular} \end{ruledtabular} \fnt[1]{Value obtained using CCSDTQ/aug-cc-pVDZ corrected by the difference between CC4/aug-cc-pVTZ and CC4/aug-cc-pVDZ.} \fnt[2]{Value obtained using NEVPT2(12,12).} \fnt[3]{Value obtained using CCSDTQ/aug-cc-pVDZ corrected by the difference between CC4/aug-cc-pVTZ and CC4/aug-cc-pVDZ.} \fnt[4]{Value obtained using CCSDTQ/aug-cc-pVDZ corrected by the difference between CCSDT/aug-cc-pVTZ and CCSDT/aug-cc-pVDZ.} \fnt[5]{Value obtained from Ref.~\onlinecite{Lefrancois_2015} at the SF-ADC(2)-s/cc-pVTZ level with the geometry obtained at the CCSD(T)/cc-pVTZ level.} \fnt[6]{Value obtained from Ref.~\onlinecite{Lefrancois_2015} at the SF-ADC(2)-x/cc-pVTZ level with the geometry obtained at the CCSD(T)/cc-pVTZ level.} \fnt[7]{Value obtained from Ref.~\onlinecite{Lefrancois_2015} at the SF-ADC(3)/cc-pVTZ level with the geometry obtained at the CCSD(T)/cc-pVTZ level.} \fnt[8]{Value obtained from Ref.~\onlinecite{Manohar_2008} at the EOM-SF-CCSD/cc-pVTZ level with the geometry obtained at the CCSD(T)/cc-pVTZ level.} \end{table*} %\end{squeezetable} %%% %%% %%% %%% \begin{table} \caption{Automerization energy (in \si{\kcalmol}) of CBD computed at various levels of theory.} % \label{} \begin{ruledtabular} \begin{tabular}{lcr} % & \mc{4}{c}{Basis sets} \\ % \cline{2-5} Level of theory & Automerization barrier & Reference \\ & (\kcalmol) & \\ \hline CCSDTQ/aug-cc-pVTZ & $8.93$ & This work \\ ic-MRCISD+Q/cc-pVTZ & $8.93$ & Ref.~\onlinecite{Zhang_2019}\\ Mk-MRCCSD/cc-pVTZ & $10.09$ & Ref.~\onlinecite{Zhang_2019}\\ Mk-MRCCSD(T)/cc-pVTZ & $8.56$ & Ref.~\onlinecite{Zhang_2019}\\ SUCCSD/cc-pVTZ & $8.7$ & Ref.~\onlinecite{Li_2009}\\ MkCCSD/cc-pVTZ & $9.6$ & Ref.~\onlinecite{Li_2009}\\ RMRCCSD(T)/cc-pVTZ & $9.5$ & Ref.~\onlinecite{Li_2009}\\ MRCISD/cc-pVTZ & $8.4$ & Ref.~\onlinecite{Eckert-Maksic_2006}\\ MRCISD + Q/cc-pVTZ & $8.8$ & Ref.~\onlinecite{Eckert-Maksic_2006}\\ MRAQCC/cc-pVTZ & $8.9$ & Ref.~\onlinecite{Eckert-Maksic_2006}\\ CCSDt/cc-pVTZ & $9.5$ & Ref.~\onlinecite{Shen_2012}\\ CCSD(T)-h/cc-pVTZ & $6.8$ & Ref.~\onlinecite{Shen_2012}\\ CC(t;3)/cc-pVTZ & $10.0$ & Ref.~\onlinecite{Shen_2012}\\ \end{tabular} \end{ruledtabular} \end{table} %%% %%% %%% %%% %%%%%%%%%%%%%%%%%%%%%%%% \begin{table} \caption{$\expval*{S^2}$ values for the different excited states computed at the SF-TD-DFT/aug-cc-pVTZ level for the {\Dtwo} and {\Dfour} structures.} %\hl{same comment as for Table I} % \label{tab:Ssquare} \begin{ruledtabular} \begin{tabular}{lrrrrrr} &\mc{3}{c}{$\expval*{S^2}$ for {\Dtwo} geometry} & \mc{3}{c}{{$\expval*{S^2}$ for {\Dfour} geometry}} \\ \cline{2-4} \cline{5-7} Method & {\tBoneg} & {\sBoneg} & {\twoAg} & {\Atwog} & {\Aoneg} & {\Btwog} \\ \hline SF-TD-B3LYP & $1.989$ & $0.030$ & $0.017$ & $2.007$ & $0.014$ & $0.012$\\[0.1cm] SF-TD-PBE0 & $2.001$ & $0.021$ & $0.019$ & $2.009$ & $0.018$ & $0.012$ \\[0.1cm] SF-TD-BH\&HLYP & $2.017$ & $0.026$ & $0.041$ & $2.020$ & $0.021$ & $0.018$\\[0.1cm] SF-TD-M06-2X & $2.014$ & $0.017$ & $0.040$ & $2.014$ & $0.015$ & $0.012$\\[0.1cm] SF-TD-CAM-B3LYP & $1.990$ & $0.033$ & $0.024$ & $2.008$ & $0.013$ & $0.012$\\[0.1cm] SF-TD-$\omega$B97X-V & $1.986$ & $0.035$ & $0.024$ & $2.008$ & $0.012$ & $0.010$\\[0.1cm] SF-TD-LC-$\omega $PBE08 & $1.984$ & $0.044$ & $0.031$ & $2.012$ & $0.015$ & $0.012$\\[0.1cm] SF-TD-M11 & $2.011$ & $0.023$ & $0.045$ & $2.012$ & $0.016$ & $0.014$\\ \end{tabular} \end{ruledtabular} \end{table} %%% %%% %%% %%% \clearpage %%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \bibliography{CBD} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \end{document}