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Pierre-Francois Loos 2022-03-06 22:54:21 +01:00
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@ -23,20 +23,9 @@
\newcommand{\tabc}[1]{\multicolumn{1}{c}{#1}}
\newcommand{\QP}{\textsc{quantum package}}
\newcommand{\hI}{\Hat{1}}
\newcommand{\hT}{\Hat{T}}
\newcommand{\hH}{\Hat{H}}
\newcommand{\bH}{\Bar{H}}
\newcommand{\ERI}[2]{v_{#1}^{#2}}
\newcommand{\EHF}{E_\text{HF}}
\newcommand{\EDOCI}{E_\text{DOCI}}
\newcommand{\EFCI}{E_\text{FCI}}
\newcommand{\ECC}{E_\text{CC}}
\newcommand{\EVCC}{E_\text{VCC}}
\newcommand{\EpCCD}{E_\text{pCCD}}
\newcommand{\si}{\sigma}
\renewcommand{\thesection}{S\arabic{section}}
\renewcommand{\thetable}{S\arabic{table}}
@ -89,45 +78,55 @@
%x
%\newpage
%Start.
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\section{oo-CI}
%\label{sec:oo-CI}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[h!]
\includegraphics[width=\linewidth]{plot_stat_opt}
\caption{Non-parallelity errors as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hCI (green),
\includegraphics[width=0.8\linewidth]{plot_stat_opt}
\caption{Non-parallelity errors as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with orbitals optimized at each CI level.
}
\label{fig:plot_stat_opt}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{plot_distance_opt}
\caption{Distance errors as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hCI (green),
\includegraphics[width=0.8\linewidth]{plot_distance_opt}
\caption{Distance errors as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with orbitals optimized at each CI level.
}
\label{fig:plot_distance_opt}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{xe_opt}
\caption{Equilibrium geometries as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hCI (green),
\includegraphics[width=0.8\linewidth]{xe_opt}
\caption{Equilibrium geometries as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with orbitals optimized at each CI level.
}
\label{fig:xe_opt}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{freq_opt}
\caption{Vibrational frequencies (or force constants) as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hCI (green),
\includegraphics[width=0.8\linewidth]{freq_opt}
\caption{Vibrational frequencies (or force constants) as function of the number of determinants, for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with orbitals optimized at each CI level.
}
\label{fig:freq_opt}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\section{oo-CIS
%\label{sec:oo-CIS}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[h!]
\includegraphics[width=0.8\linewidth]{plot_pes}
\caption{Potential energy curves for dissociation of six molecular systems (see main text for details), according to RHF (gray), oo-CIS (red), and FCI (black) calculations.
}
\label{fig:plot_pes}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\section{\ce{HF}, different basis sets}
%\label{sec:HF_basis}
@ -136,7 +135,7 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{plot_pes_HF}
\caption{Potential energy curves (top) and energy differences with respect to FCI (bottom), for dissociation of \ce{HF},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hybrid hCI (green),
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals,
and for the cc-pVDZ (left), cc-pVTZ (center), and cc-pVQZ (right) basis sets.
}
@ -145,9 +144,9 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{freq_HF}
\caption{Nonparallelity error (left), vibrational frequencies (center), and equilibrium geometries (right) for \ce{HF},
\caption{Non-parallelity error (left), vibrational frequencies (center), and equilibrium geometries (right) of \ce{HF},
as function of the number of determinants,
for the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and our proposed hybrid hCI (green),
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals,
and for the cc-pVDZ (left), cc-pVTZ (center), and cc-pVQZ (right) basis sets.}
\label{fig:freq_HF}
@ -161,48 +160,60 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_pes}
\caption{Potential energy curves for \ce{HF},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_pes_error}
\caption{Energy difference to the FCI results for \ce{HF},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:HF_pes} and FCI results for \ce{HF},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_npe}
\caption{Nonparallelity error for \ce{HF},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{HF}, corresponding to the potential energy curves of Fig.~\ref{fig:HF_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_distance}
\caption{Nonparallelity error for \ce{HF},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Distance error for \ce{HF}, corresponding to the potential energy curves of Fig.~\ref{fig:HF_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_distance}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_freq}
\caption{Vibrational frequency of \ce{HF},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_freq}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{HF_xe}
\caption{Equilibrium bond length of \ce{HF},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:HF_xe}
\end{figure}
@ -213,33 +224,61 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_pes}
\caption{Potential energy curves for \ce{F2},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Potential energy curves for \ce{F2},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_pes_error}
\caption{Energy difference to the FCI results for \ce{F2},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:F2_pes} and FCI results for \ce{F2},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_npe}
\caption{Nonparallelity error for \ce{F2},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{F2}, corresponding to the potential energy curves of Fig.~\ref{fig:F2_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_distance}
\caption{Distance error for \ce{F2}, corresponding to the potential energy curves of Fig.~\ref{fig:F2_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_distance}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_freq}
\caption{Vibrational frequency of \ce{F2},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_freq}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{F2_xe}
\caption{Equilibrium bond length of \ce{F2},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Equilibrium bond length of \ce{F2},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:F2_xe}
\end{figure}
@ -250,33 +289,61 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_pes}
\caption{Potential energy curves for ethylene, as function of the C$=$C distance,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Potential energy curves for \ce{ethylene},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_pes_error}
\caption{Energy difference to the FCI results for ethylene, as function of the C$=$C distance,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:ethylene_pes} and FCI results for \ce{ethylene},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_npe}
\caption{Nonparallelity error for ethylene,
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{ethylene}, corresponding to the potential energy curves of Fig.~\ref{fig:ethylene_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_distance}
\caption{Distance error for \ce{ethylene}, corresponding to the potential energy curves of Fig.~\ref{fig:ethylene_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_distance}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_freq}
\caption{Vibrational frequency of \ce{ethylene},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_freq}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{ethylene_xe}
\caption{C$=$C equilibrium bond length of ethylene,
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Equilibrium bond length of \ce{ethylene},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:ethylene_xe}
\end{figure}
@ -287,36 +354,63 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_pes}
\caption{Potential energy curves for \ce{N2},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Potential energy curves for \ce{N2},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_pes_error}
\caption{Energy difference to the FCI results for \ce{N2},
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:N2_pes} and FCI results for \ce{N2},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_npe}
\caption{Nonparallelity error for \ce{N2},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{N2}, corresponding to the potential energy curves of Fig.~\ref{fig:N2_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_xe}
\caption{Equilibrium bond length of \ce{N2},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\label{fig:N2_xe}
\includegraphics[width=\linewidth]{N2_distance}
\caption{Distance error for \ce{N2}, corresponding to the potential energy curves of Fig.~\ref{fig:N2_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_distance}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_freq}
\caption{Vibrational frequency of \ce{N2},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_freq}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{N2_xe}
\caption{Equilibrium bond length of \ce{N2},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:N2_xe}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\section{\ce{H4}}
@ -325,36 +419,63 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_pes}
\caption{Potential energy curves for linear \ce{H4}, as function of the symmetric stretching coordinate,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Potential energy curves for \ce{H4},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_pes_error}
\caption{Energy difference to the FCI results for linear \ce{H4}, as function of the symmetric stretching coordinate,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:H4_pes} and FCI results for \ce{H4},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_npe}
\caption{Nonparallelity error for linear \ce{H4},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{H4}, corresponding to the potential energy curves of Fig.~\ref{fig:H4_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_xe}
\caption{Equilibrium bond length of linear \ce{H4},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\label{fig:H4_xe}
\includegraphics[width=\linewidth]{H4_distance}
\caption{Distance error for \ce{H4}, corresponding to the potential energy curves of Fig.~\ref{fig:H4_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_distance}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_force}
\caption{Force constants for symmetric dissociation of \ce{H4},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_force}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H4_xe}
\caption{Equilibrium bond length of \ce{H4},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H4_xe}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\section{\ce{H8}}
@ -363,37 +484,63 @@
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_pes}
\caption{Potential energy curves for linear \ce{H8}, as function of the symmetric stretching coordinate,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Potential energy curves for \ce{H8},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_pes}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_pes_error}
\caption{Energy difference to the FCI results for linear \ce{H8}, as function of the symmetric stretching coordinate,
computed with different CI methods and the cc-pVDZ basis set,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right).}
\caption{Energy differences between the potential energy curves of Fig.~\ref{fig:H8_pes} and FCI results for \ce{H8},
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
(dashed lines for half-integer $h$),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_pes_error}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_npe}
\caption{Nonparallelity error for linear \ce{H8},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\caption{Non-parallelity error for \ce{H8}, corresponding to the potential energy curves of Fig.~\ref{fig:H8_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_npe}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_xe}
\caption{Equilibrium bond length of linear \ce{H8},
as function of the computational scaling of excitation-based CI (red) and CIo (green) methods,
with Hartree-Fock orbitals (left) and orbitals optimized for a given CI method (right), for the cc-pVDZ basis set.}
\label{fig:H8_xe}
\includegraphics[width=\linewidth]{H8_distance}
\caption{Distance error for \ce{H8}, corresponding to the potential energy curves of Fig.~\ref{fig:H8_pes},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_distance}
\end{figure}
%End.
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_force}
\caption{Force constants for symmetric dissociation of \ce{H8},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_force}
\end{figure}
\begin{figure}[h!]
\includegraphics[width=\linewidth]{H8_xe}
\caption{Equilibrium bond length of \ce{H8},
as function of the number of determinants,
according to the three classes of CI methods: seniority-based CI (blue), excitation-based CI (red), and hierarchy-based CI (green),
with Hartree-Fock orbitals (left) and orbitals optimized at a given level of CI (right),
and with the cc-pVDZ basis set.}
\label{fig:H8_xe}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\bibliography{seniority}

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@ -51,8 +51,8 @@ set label 11 'HF' at screen 0.34,0.94 tc ls 2 font 'Helvet
set label 12 'F_2' at screen 0.79,0.94 tc ls 2 font 'Helvetica,26'
set label 13 'ethylene' at screen 0.34,0.63 tc ls 2 font 'Helvetica,26'
set label 14 'N_2' at screen 0.79,0.63 tc ls 2 font 'Helvetica,26'
set label 15 'H_4' at screen 0.34,0.315 tc ls 2 font 'Helvetica,26'
set label 16 'H_8' at screen 0.79,0.315 tc ls 2 font 'Helvetica,26'
set label 15 'H_4' at screen 0.34,0.310 tc ls 2 font 'Helvetica,26'
set label 16 'H_8' at screen 0.79,0.310 tc ls 2 font 'Helvetica,26'
set format y "%.1f"

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@ -51,8 +51,8 @@ set label 11 'HF' at screen 0.34,0.94 tc ls 2 font 'Helvet
set label 12 'F_2' at screen 0.79,0.94 tc ls 2 font 'Helvetica,26'
set label 13 'ethylene' at screen 0.34,0.63 tc ls 2 font 'Helvetica,26'
set label 14 'N_2' at screen 0.79,0.63 tc ls 2 font 'Helvetica,26'
set label 15 'H_4' at screen 0.34,0.315 tc ls 2 font 'Helvetica,26'
set label 16 'H_8' at screen 0.79,0.315 tc ls 2 font 'Helvetica,26'
set label 15 'H_4' at screen 0.34,0.310 tc ls 2 font 'Helvetica,26'
set label 16 'H_8' at screen 0.79,0.310 tc ls 2 font 'Helvetica,26'
set format y "%.1f"