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@ -365,8 +365,10 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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\label{fig:vsEPT2}}
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\end{figure*}
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\begin{squeezetable}
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\begin{table*}
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\caption{Total energy $E$ (in \SI{}{\hartree}) and correlation energy $\Delta E$ (in \SI{}{\milli\hartree}) for the frozen-core ground state of five-membered rings in the cc-pVDZ basis set.
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For the CIPSI estimates of the correlation energy, the fitting error associated with the 4-point linear fit is reported in parenthesis.
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\label{tab:Tab5-VDZ}}
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\begin{ruledtabular}
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\begin{tabular}{lcccccccccc}
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@ -392,14 +394,16 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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CCSD(T) & $-193.5439$ & $-735.6$ & $-229.4073$ & $-764.0$ & $-225.6099$ & $-774.5$ & $-209.5836$ & $-754.9$ & $-552.0458$ & $-724.8$
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\\
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\hline
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CIPSI & & $-739.3$ & & $-768.1$ & & $-778.3$ & & $-758.4$ & & $-729.1$\\
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CIPSI & & $-739.3(1)$ & & $-768.1(2)$ & & $-778.3(1)$ & & $-758.4(2)$ & & $-729.1(3)$\\
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\end{tabular}
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\end{ruledtabular}
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\end{table*}
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\end{squeezetable}
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\begin{squeezetable}
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\begin{table*}
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\caption{Total energy $E$ (in \SI{}{\hartree}) and correlation energy $\Delta E$ (in \SI{}{\milli\hartree}) for the frozen-core ground state of six-membered rings in the cc-pVDZ basis set.
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For the CIPSI estimates of the correlation energy, the fitting error associated with the 4-point linear fit is reported in parenthesis.
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\label{tab:Tab6-VDZ}}
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\begin{ruledtabular}
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\begin{tabular}{lcccccccccccccc}
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@ -425,18 +429,127 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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\hline
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CCSD(T) & $-231.5798$ & $-857.5$ & $-263.6024$ & $-899.4$ & $-263.5740$ & $-904.1$ & $-247.5929$ & $-877.7$ & $-263.6099$ & $-896.2$ & $-295.5680$ & $-952.2$ & $-279.6305$ & $-913.1$ \\
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\hline
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CIPSI & & $-863.0$ & & $-904.6$ & & $-908.8$ & & $-883.4$ & & $-900.4$ & & $-957.3$ & & $-918.5$\\
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CIPSI & & $-863.0(4)$ & & $-904.6(6)$ & & $-908.8(2)$ & & $-883.4(0)$ & & $-900.4(4)$ & & $-957.3(2)$ & & $-918.5(5)$\\
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\end{tabular}
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\end{ruledtabular}
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\end{table*}
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\end{squeezetable}
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\begin{squeezetable}
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\begin{table}
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\caption{
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\label{tab:fit}}
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\begin{ruledtabular}
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\begin{tabular}{lccc}
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Molecule & Number & \mc{2}{c}{Fitting parameter} \\
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\cline{3-4}
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& of points & $\Delta \Evar$ & Standard error \\
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\hline
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Cyclopentadiene & 3 & $-739.295$ & $0.199$ \\
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& 4 & $-739.309$ & $0.088$ \\
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& 5 & $-739.230$ & $0.074$ \\
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& 6 & $-739.304$ & $0.072$ \\
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& 7 & $-739.292$ & $0.055$ \\
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& 8 & $-739.119$ & $0.131$ \\
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\hline
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Furan & 3 & $-767.790$ & $0.064$ \\
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& 4 & $-768.104$ & $0.196$ \\
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& 5 & $-768.194$ & $0.135$ \\
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& 6 & $-768.060$ & $0.131$ \\
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& 7 & $-768.086$ & $0.101$ \\
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& 8 & $-767.904$ & $0.154$ \\
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\hline
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Imidazole & 3 & $-778.295$ & $0.356$ \\
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& 4 & $-778.270$ & $0.150$ \\
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& 5 & $-778.178$ & $0.105$ \\
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& 6 & $-778.174$ & $0.072$ \\
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& 7 & $-778.051$ & $0.099$ \\
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& 8 & $-777.992$ & $0.089$ \\
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\hline
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Pyrrole & 3 & $-758.650$ & $0.321$ \\
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& 4 & $-758.389$ & $0.174$ \\
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& 5 & $-758.460$ & $0.110$ \\
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& 6 & $-758.352$ & $0.100$ \\
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& 7 & $-758.347$ & $0.075$ \\
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& 8 & $-758.357$ & $0.059$ \\
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\hline
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Thiophene & 3 & $-728.744$ & $0.691$ \\
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& 4 & $-729.052$ & $0.331$ \\
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& 5 & $-728.948$ & $0.203$ \\
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& 6 & $-728.987$ & $0.140$ \\
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& 7 & $-729.067$ & $0.117$ \\
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& 8 & $-728.876$ & $0.162$ \\
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\hline
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Benzene & 3 & $-862.325$ & $0.279$ \\
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& 4 & $-863.024$ & $0.424$ \\
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& 5 & $-862.890$ & $0.266$ \\
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& 6 & $-862.360$ & $0.383$ \\
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& 7 & $-862.083$ & $0.339$ \\
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& 8 & $-861.711$ & $0.370$ \\
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\hline
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Pyrazine & 3 & $-904.867$ & $1.420$ \\
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& 4 & $-904.588$ & $0.650$ \\
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& 5 & $-904.550$ & $0.385$ \\
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& 6 & $-903.982$ & $0.439$ \\
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& 7 & $-903.746$ & $0.359$ \\
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& 8 & $-903.549$ & $0.311$ \\
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\hline
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Pyridazine & 3 & $-909.292$ & $0.024$ \\
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& 4 & $-908.808$ & $0.230$ \\
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& 5 & $-908.820$ & $0.133$ \\
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& 6 & $-908.342$ & $0.303$ \\
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& 7 & $-908.368$ & $0.224$ \\
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& 8 & $-908.229$ & $0.198$ \\
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\hline
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Pyridine & 3 & $-883.363$ & $0.047$ \\
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& 4 & $-883.413$ & $0.029$ \\
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& 5 & $-882.700$ & $0.405$ \\
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& 6 & $-882.361$ & $0.341$ \\
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& 7 & $-882.023$ & $0.330$ \\
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& 8 & $-881.732$ & $0.322$ \\
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\hline
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Pyrimidine & 3 & $-900.817$ & $0.726$ \\
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& 4 & $-900.383$ & $0.356$ \\
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& 5 & $-900.496$ & $0.214$ \\
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& 6 & $-900.698$ & $0.190$ \\
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& 7 & $-900.464$ & $0.206$ \\
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& 8 & $-900.226$ & $0.227$ \\
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\hline
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Tetrazine & 3 & $-957.559$ & $0.246$ \\
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& 4 & $-957.299$ & $0.160$ \\
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& 5 & $-957.869$ & $0.349$ \\
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& 6 & $-957.744$ & $0.247$ \\
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& 7 & $-957.709$ & $0.183$ \\
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& 8 & $-957.558$ & $0.176$ \\
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\hline
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Triazine & 3 & $-919.596$ & $0.105$ \\
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& 4 & $-918.457$ & $0.538$ \\
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& 5 & $-918.355$ & $0.312$ \\
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& 6 & $-918.206$ & $0.226$ \\
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& 7 & $-917.876$ & $0.267$ \\
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& 8 & $-917.533$ & $0.308$ \\
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\end{tabular}
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\end{ruledtabular}
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\end{table}
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\end{squeezetable}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection{CIPSI estimates}
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\label{sec:cipsi_res}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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We first study the convergence of the variational energy as a function of the number of determinants.
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For the natural and optimized orbital sets we report, in Fig.~\ref{fig:vsNdet}, the evolution of the variational correlation energy $\Delta \Evar$ with respect to the number of determinants for the set of twelve cyclic molecules represented in Fig.~\ref{fig:mol}.
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As one can see, the use of optimized orbitals greatly facilitate the convergence towards the FCI limit.
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This is further evidenced in Fig.~\ref{fig:vsEPT2} where we show the behavior of $\Delta \Evar$ as a function of $\EPT$ as well as its 4-point linear fit using the four largest variational wave functions.
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In both cases, the CCSDTQ correlation energy is also represented for comparison purposes.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Benchmark of CC and MP methods}
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\label{sec:cc_mp_res}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Conclusion}
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%%%%%%%%%%%%%%%%%%%%%%%%%
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@ -24,4 +24,3 @@
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20971520 -231.5252061140 -0.0406298392 0.0000791195 -0.0403887454 0.0000786500
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41943040 -231.5337886859 -0.0346957844 0.0000668061 -0.0345247390 0.0000664767
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83886080 -231.5413391318 -0.0256659821 0.0001461668 -0.0294457584 0.0001455696
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167772160
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@ -24,4 +24,3 @@
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20971520 -193.5126035896 -0.0246344737 0.0000479428 -0.0245465962 0.0000477718
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41943040 -193.5183426226 -0.0206049053 0.0000402624 -0.0205451654 0.0000401457
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83886080 -193.5232476384 -0.0170993616 0.0000813000 -0.0170594255 0.0000811101
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167772160
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@ -24,4 +24,3 @@
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20971520 -229.3797442530 -0.0224998381 0.0000423186 -0.0224333245 0.0000421935
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41943040 -229.3852109522 -0.0185751065 0.0000362444 -0.0185311719 0.0000361586
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83886080 -229.3897820101 -0.0152739899 0.0000641000 -0.0152452221 0.0000639793
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167772160
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