Spin invariance
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@ -607,31 +607,77 @@ Ref.~\onlinecite{Scemama_2015}).
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\end{table}
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In this section, we make a numerical verification that the produced
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wave functions are size-consistent. We have computed the energy of the
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dissocited fluorine dimer, where the two atoms are at a distance of 50~\AA.
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We expect that the energy of this system is equal to twice the energy
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of the fluorine atom.
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The data in table~\ref{tab:size-cons} shows that the proposed scheme
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provides size-consistent FN-DMC energies for all values of $\mu$.
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wave functions are size-consistent for a given range-separation
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parameter.
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We have computed the energy of the dissocited fluorine dimer, where
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the two atoms are at a distance of 50~\AA. We expect that the energy
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of this system is equal to twice the energy of the fluorine atom.
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The data in table~\ref{tab:size-cons} shows that it is indeed the
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case, so we can conclude that the proposed scheme provides
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size-consistent FN-DMC energies for all values of $\mu$.
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\subsection{Spin-invariance}
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Closed-shell molecules usually dissociate into open-shell
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Closed-shell molecules often dissociate into open-shell
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fragments. To get reliable atomization energies, it is important to
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have a theory which is of comparable quality for open-shell and
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closed-shell systems.
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closed-shell systems. A good test is to check that all the components
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of a spin multiplet are degenerate.
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FCI wave functions are invariant with respect to the spin quantum
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number $m_s$, but the introduction of a
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Jastrow factor breaks this spin-invariance if the parameters
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Jastrow factor introduces spin contamination if the parameters
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for the same-spin electron pairs are different from those
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for the opposite-spin pairs.\cite{Tenno_2004}
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Again, using pseudo-potentials this error is transferred in the DMC
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calculation unless the determinant localization approximation is used.
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Again, when pseudo-potentials are used this tiny error is transferred
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in the FN-DMC energy unless the determinant localization approximation
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is used.
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Within DFT, the common density functionals make a difference for
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same-spin and opposite-spin interactions. As DFT is a
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single-determinant theory, the functionals are designed to work in
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with the highest value of $m_s$, and therefore different
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values of $m_s$ lead to different energies.
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So in the context of RS-DFT, the determinantal expansions will be
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impacted by this spurious effect, as opposed to FCI.
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\begin{table}
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\caption{FN-DMC Energies of the triplet carbon atom (BFD-VDZ) with
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different values of $m_s$.}
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\label{tab:spin}
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\begin{ruledtabular}
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\begin{tabular}{cccc}
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$\mu$ & $m_s=1$ & $m_s=0$ & Spin-invariance error \\
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\hline
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0.00 & $-5.416\,8(1)$ & $-5.414\,9(1)$ & $+0.001\,9(2)$ \\
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0.25 & $-5.417\,2(1)$ & $-5.416\,5(1)$ & $+0.000\,7(1)$ \\
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0.50 & $-5.422\,3(1)$ & $-5.421\,4(1)$ & $+0.000\,9(2)$ \\
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1.00 & $-5.429\,7(1)$ & $-5.429\,2(1)$ & $+0.000\,5(2)$ \\
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2.00 & $-5.432\,1(1)$ & $-5.431\,4(1)$ & $+0.000\,7(2)$ \\
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5.00 & $-5.431\,7(1)$ & $-5.431\,4(1)$ & $+0.000\,3(2)$ \\
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$\infty$ & $-5.431\,6(1)$ & $-5.431\,3(1)$ & $+0.000\,3(2)$ \\
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\end{tabular}
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\end{ruledtabular}
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\end{table}
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In this section, we investigate the impact of the spin contamination
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due to the short-range density functional on the FN-DMC energy. We have
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computed the energies of the carbon atom in its triplet state
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with BFD pseudo-potentials and the corresponding double-zeta basis
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set. The calculation was done with $m_s=1$ (3 $\uparrow$ electrons
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and 1 $\downarrow$ electrons) and with $m_s=0$ (2 $\uparrow$ and 2
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$\downarrow$ electrons).
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The results are presented in table~\ref{tab:spin}.
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Although using $m_s=0$ the energy is higher than with $m_s=1$, the
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bias is relatively small, more than one order of magnitude smaller
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than the energy gained by reducing the fixed-node error going from the single
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determinant to the FCI trial wave function. The highest bias, close to
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2~m\hartree, is obtained for $\mu=0$, but the bias decreases quickly
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below 1~m\hartree when $\mu$ increases. As expected, with $\mu=\infty$
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there is no bias (within the error bars), and the bias is not
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noticeable with $\mu=5$~bohr$^{-1}$.
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To check that the RSDFT-CIPSI are spin-invariant, we compute the
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FN-DMC energies of the ?? dimer with different values of the spin
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quantum number $m_s$.
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