changing notation for n_2
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@ -662,13 +662,13 @@ an impact on the CI coefficients similar to the Jastrow factor.
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%%% TABLE II %%%
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\begin{table}
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\caption{\ce{H2O}, double-zeta basis set. Integrated on-top pair density $\expval{ n_2(\br,\br) }$
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\caption{\ce{H2O}, double-zeta basis set. Integrated on-top pair density $\expval{ P }$
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for $\Psi^J$ and $\Psi^\mu$ with different values of $\mu$.
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\titou{Please remove table and merge data in the Fig. 5.}}
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\label{tab:table_on_top}
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\begin{ruledtabular}
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\begin{tabular}{cc}
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$\mu$ & $\expval{ n_2(\br,\br) }$ \\
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$\mu$ & $\expval{ P }$ \\
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\hline
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0.00 & 1.443 \\
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0.25 & 1.438 \\
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@ -711,9 +711,9 @@ an impact on the CI coefficients similar to the Jastrow factor.
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In order to refine the comparison between $\Psi^\mu$ and $\Psi^J$, we
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report several quantities related to the one- and two-body densities of
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$\Psi^J$ and $\Psi^\mu$ with different values of $\mu$. First, we
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report in Table~\ref{table_on_top} the integrated on-top pair density
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report in Table~\ref{tab:table_on_top} the integrated on-top pair density
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\begin{equation}
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\expval{ n_2(\br,\br) } = \int d\br \,\,n_2(\br,\br)
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\expval{ P } = \int d\br \,\,n_2(\br,\br)
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\end{equation}
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where $n_2(\br_1,\br_2)$ is the two-body density [normalized to $\Nelec(\Nelec-1)$]
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obtained for both $\Psi^\mu$ and $\Psi^J$.
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