Manu: done with my revisions.
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@ -186,12 +186,11 @@ that the deviation from linearity of the ensemble energy would be zero.}
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\alert{The legend of Fig.~2 was incorrect (the curves were mislabeled), but this has now been corrected.
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\alert{The legend of Fig.~2 was incorrect (the curves were mislabeled), but this has now been corrected.
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In the corrected Fig.~2 (which is now Fig.~4 in the revised
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In the corrected Fig.~2 (which is now Fig.~4 in the revised
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manuscript), the crossover point occurs for two different states that
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manuscript), the crossover point occurs for two different states in
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belong to two different ensembles. In other words, this point is not
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two different ensembles. In other words, this point is not
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interesting anymore. The discussion of this Figure has become much more fluid:
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interesting anymore. The discussion of this Figure has become much more fluid:
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when the weight of a state increases, this state is stabilized
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when the weight of a state increases, this state is stabilized
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while the two others increase in energy (as it should). \manu{Well, the
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while the two others increase in energy (as it should).
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energy of the first excited state still decreases when $w_2$ increases}
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The discussion regarding this figure has been modified accordingly.}
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The discussion regarding this figure has been modified accordingly.}
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% \alert{It is clear from our derivations that the individual
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% \alert{It is clear from our derivations that the individual
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%correlation energies should vary with both the density {\it
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%correlation energies should vary with both the density {\it
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@ -221,10 +220,20 @@ manuscrit before commenting on the plots.}
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If not, why not? }
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If not, why not? }
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\alert{Yes, as readily seen from the data provided in the
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\alert{Yes, as readily seen from the data provided in the
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supplemental material, similar issues appear for excited states.
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supplemental material, similar issues appear for excited states.\manu{I
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would remove your sentence and be more optimistic (see what follows). Do
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you agree?}\\
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Interestingly, increasing the ensemble weights (which of course cannot
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Interestingly, increasing the ensemble weights (which of course cannot
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be done in conventional ground-state DFT) seems to reduce
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be done in conventional ground-state DFT calculations) leads to a
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errors}
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significant improvement of the ground-state energy while either
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improving or not deteriorating too much the excited-state energies, at
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least in the weak correlation regime. The main reason is the
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destabilization of the ground state that occurs when increasing the
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weights assigned to the excited states. This major difference between
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practical
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conventional DFT (where the correlation energy would be overestimated)
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and GOK-DFT calculations is a promising result that is
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now highlighted in the revised manuscript.}
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%\manu{We need to check the tables in the SI}
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%\manu{We need to check the tables in the SI}
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\item
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\item
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