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Density Functional Theory Based on the Electron Distribution on the Energy Coordinate
Chemical Physics · Submitted 25 Jan 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim By taking advantage of this property we developed a prototype of the static correlation functional employing no empirical parameters, which realized a reasonable dissociation curve for H2 molecule.
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The abstract, sentence by sentence
We introduced a new electron density n({\epsilon}) by projecting the spatial electron density n(r) onto the energy coordinate {\epsilon} defined with the external potential \upsion (r) of interest. Then, a density functional theory (DFT) was formulated, where n({\epsilon}) serves as a fundamental variable for the electronic energy. It was demonstrated that the Kohn-Sham equation can also be adapted to the DFT that employs the density n({\epsilon}) as an argument to the exchange energy functional. An important attribute of the energy density is that it involves the spatially non-local population of the spin-adapted density n(r) at the bond dissociation. By taking advantage of this property we developed a prototype of the static correlation functional employing no empirical parameters, which realized a reasonable dissociation curve for H2 molecule.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We introduced a new electron density n({\epsilon}) by projecting the spatial electron density n(r) onto the energy coordinate {\epsilon} defined with the external potential \upsion (r) of interest. | contribution 0.87 | 0.94 | 0.08 | asserted 1.00 |
| s1 | Then, a density functional theory (DFT) was formulated, where n({\epsilon}) serves as a fundamental variable for the electronic energy. | contribution 0.78 | 0.90 | 0.18 | asserted 1.00 |
| s2 | It was demonstrated that the Kohn-Sham equation can also be adapted to the DFT that employs the density n({\epsilon}) as an argument to the exchange energy functional. | result 0.45 | 0.84 | 0.15 | asserted 1.00 |
| s3 | An important attribute of the energy density is that it involves the spatially non-local population of the spin-adapted density n(r) at the bond dissociation. | interpretation 0.49 | 0.77 | 0.12 | asserted 1.00 |
| s4 | By taking advantage of this property we developed a prototype of the static correlation functional employing no empirical parameters, which realized a reasonable dissociation curve for H2 molecule. | result 0.67 | 0.96 | 0.45 | asserted 0.99 |
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Original abstract
We introduced a new electron density n({\epsilon}) by projecting the spatial electron density n(r) onto the energy coordinate {\epsilon} defined with the external potential \upsion (r) of interest. Then, a density functional theory (DFT) was formulated, where n({\epsilon}) serves as a fundamental variable for the electronic energy. It was demonstrated that the Kohn-Sham equation can also be adapted to the DFT that employs the density n({\epsilon}) as an argument to the exchange energy functional. An important attribute of the energy density is that it involves the spatially non-local population of the spin-adapted density n(r) at the bond dissociation. By taking advantage of this property we developed a prototype of the static correlation functional employing no empirical parameters, which realized a reasonable dissociation curve for H2 molecule.
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