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How tight is the Lieb-Oxford bound?
Mariana M Odashima1, K Capelle
1Departamento de Física e Informática, Instituto de Física de São Carlos, Universidade de São Paulo, Caixa Postal 369, São Carlos, 13560-970 São Paulo, Brazil.
Researchers explored the Lieb-Oxford bound for exchange-correlation energy in density-functional theory. Findings suggest a tighter universal bound (C≤1) than the commonly used 1.68, impacting functional development.
Area of Science:
- Quantum Chemistry
- Computational Materials Science
- Condensed Matter Physics
Background:
- Density-functional theory (DFT) relies on accurate exchange-correlation (xc) functionals for describing electronic structure.
- Universal constraints on xc energy are crucial for developing improved DFT functionals.
- The Lieb-Oxford bound is a fundamental constraint on the xc energy.
Purpose of the Study:
- To investigate the universal property of the Lieb-Oxford lower bound for xc functionals.
- To determine the optimal prefactor C in the Lieb-Oxford bound across various systems.
- To assess the impact of the bound's prefactor on the performance of modern xc functionals.
Main Methods:
- Surveyed exact or near-exact data for xc energies of atoms, ions, molecules, and solids.
- Included data from model Hamiltonians: electron liquid, Hooke's atom, and Hubbard model.
- Analyzed physically realistic density distributions to evaluate the Lieb-Oxford bound.
Main Results:
- All investigated physically realistic density distributions are consistent with a tighter Lieb-Oxford bound prefactor (C≤1).
- Class-specific, but not fully universal, bounds were derived for large system categories.
- The commonly used Lieb-Oxford bound prefactor of 1.68 may be too large for many systems.
Conclusions:
- A tighter universal Lieb-Oxford bound (C≤1) is supported by a wide range of physical systems.
- Revisiting the prefactor C in the Lieb-Oxford bound is essential for developing more accurate xc functionals.
- Changes to the prefactor C will significantly influence the predictive power of current DFT functionals.
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