fix some problems in references
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@ -4508,6 +4508,7 @@
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@article{GolWerSto-PCCP-05,
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Author = {Erich Goll and Hans-Joachim Werner and Hermann Stoll},
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title = {A short-range gradient-corrected density functional in long-range coupled-cluster calculations for rare gas dimers},
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Journal = {Phys. Chem. Chem. Phys.},
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Pages = {3917},
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Volume = {7},
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@ -5871,6 +5872,7 @@
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@article{JanHenScu-JCP-09,
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Author = {B. G. Janesko and T. M. Henderson and G. E. Scuseria},
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title = {Long-range-corrected hybrids including random phase approximation correlation},
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Journal = {J. Chem. Phys.},
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Pages = {081105},
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Volume = {130},
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@ -12212,7 +12214,7 @@
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Author = {Holmes,Adam A. and Umrigar,C. J. and Sharma,Sandeep},
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Doi = {10.1063/1.4998614},
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Eprint = {https://doi.org/10.1063/1.4998614},
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Journal = {The Journal of Chemical Physics},
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Journal = {J. Chem. Phys.},
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Number = {16},
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Pages = {164111},
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Title = {Excited states using semistochastic heat-bath configuration interaction},
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@ -12269,7 +12271,7 @@
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Author = {Dasgupta, Saswata and Herbert, John M.},
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Doi = {10.1002/jcc.24761},
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Eprint = {https://onlinelibrary.wiley.com/doi/pdf/10.1002/jcc.24761},
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Journal = {Journal of Computational Chemistry},
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Journal = {J. Comput. Chem.},
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Number = {12},
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Pages = {869-882},
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Title = {Standard grids for high-precision integration of modern density functionals: SG-2 and SG-3},
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@ -12279,7 +12281,7 @@
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@article{Tenno-CPL-04,
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title = "Initiation of explicitly correlated Slater-type geminal theory",
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journal = "Chemical Physics Letters",
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journal = "Chem. Phys. Lett.",
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volume = "398",
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number = "1",
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pages = "56 - 61",
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@ -390,11 +390,11 @@ Depending on the functional choice, the complementary functional $\bE{}{\Bas}[\n
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As most WFT calculations are performed within the frozen-core (FC) approximation, it is important to define an effective interaction within a subset of MOs.
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We then naturally split the basis set as $\Bas = \Cor \bigcup \BasFC$ (where $\Cor$ and $\BasFC$ are the sets of core and active MOs, respectively) and define the FC version of the effective interaction as
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\begin{equation}
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\W{\Bas}{\FC}(\br{1},\br{2}) =
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\W{\Bas}{\FC}(\br{1},\br{2}) \! = \!
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\begin{cases}
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\f{\Bas}{\FC}(\br{1},\br{2})/\n{2,\Bas}{\FC}(\br{1},\br{2}), & \text{if $\n{2,\Bas}{\FC}(\br{1},\br{2})\ne 0$},
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\f{\Bas}{\FC}(\br{1},\br{2})/\n{2,\Bas}{\FC}(\br{1},\br{2}),\! & \!\!\! \text{if $\n{2,\Bas}{\FC}(\br{1},\br{2}) \!\ne \! 0$},
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\\
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\infty, & \text{otherwise,}
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\infty, \! & \!\!\! \text{otherwise,}
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\end{cases}
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\end{equation}
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with
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@ -512,7 +512,7 @@ To estimate the CBS limit of each method, following Ref.~\onlinecite{HalHelJorKl
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As the exFCI calculations are converged with a precision of about 0.1 {\kcal} on atomization energies, we can label those as near-FCI.
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Hence, they will be our references for \ce{C2}, \ce{N2}, \ce{O2} and \ce{F2}.
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The results for these diatomics are reported in Fig.~\ref{fig:diatomics}.
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The results for these diatomic molecules are reported in Fig.~\ref{fig:diatomics}.
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The corresponding numerical data can be found in the {\SI}.
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As one can see, the convergence of the exFCI atomization energies is, as expected, slow with respect to the basis set: chemical accuracy (error below 1 {\kcal}) is barely reached for \ce{C2}, \ce{O2} and \ce{F2} even with the cc-pV5Z basis set, and the atomization energies are consistently underestimated.
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A similar trend holds for CCSD(T).
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@ -545,7 +545,7 @@ Encouraged by these promising results, we are currently pursuing various avenues
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section*{Supporting information}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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See {\SI} for raw data associated with the atomization energies of the four diatomics and the G2 set.
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See {\SI} for raw data associated with the atomization energies of the four diatomic molecules and the G2 set.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\begin{acknowledgements}
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