Effective One-Electron Potential in the Kohn—Sham Molecular Orbital Theory
Evert Jan Baerends, O. V. Gritsenko, Robert van Leeuwen
Abstract
Evert Jan Baerends, O. V. Gritsenko, Robert van Leeuwen
Abstract
Density functional theory has received great interest mostly because of the accurate bonding energies and related properties (geometries, force constants) it provides. However, the Kohn-Sham molecular orbital method, that is almost exclusively used, is more than a convenient tool to generate the required electron density. The effective one-electron potential in the Kohn-Sham equations is intimately related to the physics of electron correlation. We demonstrate that it is useful to break down the exchange-correlation part of the potential into a part that is directly related to the total energy (the hole potential or screening potential) and a socalled response part that is related to "response" of the exchange-correlation hole to density change. The latter part is poorly represented by the generalized gradient approximation, explaining why this approximation yields accurate total energies but fails for simple orbital related quantities such as the HOMO orbital energy. A simple modelling of the response
OpenAlex reports 25 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Density functional theory has received great interest mostly because of the accurate bonding energies and related properties (geometries, force constants) it provides. However, the Kohn-Sham molecular orbital method, that is almost exclusively used, is more than a convenient tool to generate the required electron density. The effective one-electron potential in the Kohn-Sham equations is intimately related to the physics of electron correlation. We demonstrate that it is useful to break down the exchange-correlation part of the potential into a part that is directly related to the total energy (the hole potential or screening potential) and a socalled response part that is related to "response" of the exchange-correlation hole to density change. The latter part is poorly represented by the generalized gradient approximation, explaining why this approximation yields accurate total energies but fails for simple orbital related quantities such as the HOMO orbital energy. A simple modelling of the response
Key concepts: Kohn–Sham equations, Density functional theory, Simple (philosophy), Electron, Physics, Orbital-free density functional theory, Quantum mechanics, Energy (signal processing)