Accuracy of electron densities obtained via Koopmans-compliant hybrid functionals
arXiv:1803.11076 · doi:10.1103/PhysRevMaterials.2.040801
Abstract
We evaluate the accuracy of electron densities and quasiparticle energy gaps given by hybrid functionals by directly comparing these to the exact quantities obtained from solving the many-electron Schrodinger equation. We determine the admixture of Hartree-Fock exchange to approximate exchange-correlation in our hybrid functional via one of several physically justified constraints, including the generalized Koopmans' theorem. We find that hybrid functionals yield strikingly accurate electron densities and gaps in both exchange-dominated and correlated systems. We also discuss the role of the screened Fock operator in the success of hybrid functionals.
References in corpus (9)
- The GW method
- Localization and delocalization errors in density functional theory and implications for band-gap prediction
- Understanding Band Gaps of Solids in Generalized Kohn-Sham Theory
- Fundamental gaps of finite systems from the eigenvalues of a generalized Kohn-Sham method
- Density-based mixing parameter for hybrid functionals
- Polaronic hole localization and multiple hole binding of acceptors in oxide wide-gap semiconductors
- Koopmans' condition for density-functional theory
- Exact time-dependent density-functional potentials for strongly correlated tunneling electrons
- Local density approximations from finite systems
Cited by in corpus (7)
- Small Polarons in Transition Metal Oxides
- N-centered ensemble density-functional theory for open systems
- Advantageous nearsightedness of many-body perturbation theory contrasted with Kohn-Sham density functional theory
- Exact exchange-correlation potentials for calculating the fundamental gap with a fixed number of electrons
- Insights into one-body density matrices using deep learning
- Accurate real-time evolution of electron densities and ground-state properties from generalized Kohn-Sham theory
- Exact expressions for the height of the interatomic step in the exchange-correlation potential from the derivative discontinuity of the energy