Clean up Sec. IV and new fig 1
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@ -1080,27 +1080,23 @@ We use as basis functions the (orthonormal) orbitals of the one-electron system,
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\end{cases}
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\end{equation}
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with $ \mu = 1,\ldots,\nBas$ and $\nBas = 30$ for all calculations.
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\manu{The convergence threshold $\tau = \max{ \abs{ \bF{\bw} \bGam{\bw}
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The convergence threshold $\tau = \max{ \abs{ \bF{\bw} \bGam{\bw}
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\bS - \bS \bGam{\bw} \bF{\bw}}}$ [see Eq.~(\ref{eq:commut_F_AO})] is set
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to $10^{-5}$. For comparison, regular HF and KS-DFT calculations
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are performed with the same threshold.
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In order to compute the various density-functional
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integrals that cannot be performed in closed form,
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a 51-point Gauss-Legendre quadrature is employed.}
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a 51-point Gauss-Legendre quadrature is employed.
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In order to test the present eLDA functional we perform various sets of calculations.
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To get reference excitation energies for both the single and double excitations, we compute full configuration interaction (FCI) energies with the Knowles-Handy FCI program described in Ref.~\onlinecite{Knowles_1989}.
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For the single excitations, we also perform time-dependent LDA (TDLDA)
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calculations [\ie, TDDFT with the LDA functional defined in
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Eq.~\eqref{eq:LDA}], and the effect of the Tamm-Dancoff approximation
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(TDA) has been also investigated. \cite{Dreuw_2005}\manu{Manu: has been
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studied previously (if so why do you mention this?) or will be discussed
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in the present work?}
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Concerning the \manu{ensemble}
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%KS-eDFT and eHF
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calculations, two sets of weight are tested: the zero-weight
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\manu{(ground-state)} limit where $\bw = (0,0)$ and the
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equi\manu{-tri}-ensemble (or \manu{equal-weight} state-averaged) limit where $\bw = (1/3,1/3)$.
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calculations [\ie, TDDFT with the LDA functional defined in Eq.~\eqref{eq:LDA}].
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\titou{Its Tamm-Dancoff approximation (TDA) version is also considered.} \cite{Dreuw_2005}
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Concerning the ensemble calculations, two sets of weight are tested: the zero-weight
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(ground-state) limit where $\bw = (0,0)$ and the
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equi-tri-ensemble (or equal-weight state-averaged) limit where $\bw = (1/3,1/3)$.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Results and discussion}
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14551
Notebooks/eDFT_FUEG.nb
14551
Notebooks/eDFT_FUEG.nb
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