Sum-rules of the response potential in the strongly-interacting limit of DFT
arXiv:1806.04196 · doi:10.1140/epjb/e2018-90301-8
Abstract
The response part of the exchange-correlation potential of Kohn-Sham density functional theory plays a very important role, for example for the calculation of accurate band gaps and excitation energies. Here we analyze this part of the potential in the limit of infinite interaction in density functional theory, showing that in the one-dimensional case it satisfies a very simple sum rule.
arXiv comment7 pages
References in corpus (15)
- Exact factorization of the time-dependent electron-nuclear wavefunction
- Optimal-transport formulation of electronic density-functional theory
- Strong correlation in Kohn-Sham density functional theory
- Exact Kohn-Sham potential of strongly correlated finite systems
- How is the derivative discontinuity related to steps in the exact Kohn-Sham potential?
- Exact single-electron approach to the dynamics of molecules in strong laser fields
- Smoothing of transport plans with fixed marginals and rigorous semiclassical limit of the Hohenberg-Kohn functional
- Kohn-Sham density functional theory for quantum wires in arbitrary correlation regimes
- Wigner localization in quantum dots from Kohn-Sham density functional theory without symmetry breaking
- Origin of static and dynamic steps in exact Kohn-Sham potentials
- Response potential in the strong-interaction limit of DFT: Analysis and comparison with the coupling-constant average
- Kohn-Sham potential for a strongly correlated finite system with fractional occupancy
- Augmented potential, energy densities, and virial relations in the weak- and strong-interaction limits of DFT
- No-go theorem for the description of Mott phenomena with conventional Density Functional Theory methods
- The strictly-correlated electron functional for spherically symmetric systems revisited