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@ -508,11 +508,12 @@ This molecular set has been exhausively studied in the last 20 years (see, for e
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As a method $\modX$ we employ either CCSD(T) or exFCI.
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Here, exFCI stands for extrapolated FCI energies computed with the CIPSI algorithm. \cite{HurMalRan-JCP-73, GinSceCaf-CJC-13, GinSceCaf-JCP-15}
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We refer the interested reader to Refs.~\onlinecite{HolUmrSha-JCP-17, SceGarCafLoo-JCTC-18, LooSceBloGarCafJac-JCTC-18, SceBenJacCafLoo-JCP-18, LooBogSceCafJAc-JCTC-19} for more details.
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In the case of the CCSD(T) calculations, we have $\modY = \HF$ as we use the Restricted open-shell Hartree-Fock (ROHF) one-electron density to compute the complementary energy, and for the CIPSI calculations we use the density of a converged variational wave function.
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In the case of the CCSD(T) calculations, we have $\modY = \HF$ as we use the restricted open-shell Hartree-Fock (ROHF) one-electron density to compute the complementary energy.
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\titou{For exFCI, we use the density of a converged variational wave function.}
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For the definition of the interaction, we use a single Slater determinant built in the ROHF basis for the CCSD(T) calculations, and built with the natural orbitals of the converged variational wave function for the exFCI calculations.
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The CCSD(T) calculations have been performed with Gaussian09 with standard threshold values. \cite{g09}
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RS-DFT and exFCI calculations are performed with {\QP}. \cite{QP2}
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For the quadrature grid, we employ the radial and angular points of the SG2 grid\cite{DasHer-JCC-17}.
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For the numerical quadrature, we employ the SG-2 grid. \cite{DasHer-JCC-17}
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Except for the carbon dimer where we have taken the experimental equilibrium bond length (\InAA{1.2425}), all geometries have been extracted from Ref.~\onlinecite{HauJanScu-JCP-09} and have been obtained at the B3LYP/6-31G(2df,p) level of theory.
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Frozen core calculations are defined as such: an \ce{He} core is frozen from \ce{Li} to \ce{Ne}, while a \ce{Ne} core is frozen from \ce{Na} to \ce{Ar}.
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In the context of the basis set correction, the set of valence spinorbitals $\Val$ involved in the definition of the effective interaction refers to the non-frozen spinorbitals.
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