Stationary conditions for excited states: the surprising impact of density-driven correlations
arXiv:2404.12593 · doi:10.1103/PhysRevA.111.032806
Abstract
Typical density functional theory (DFT) and approximations thereto solve the many-electron ground state problem by working from a numerically efficient non-interacting Kohn-Sham reference system; and benefit from useful minimization conditions that allow iteration (i.e. self-consistency) to the optimal energy and density. Ensembles of ground and excited states can also benefit from similar minimization conditions [see in source]. This work reveals that individual excited states also have state-specific stationary conditions, that can be deduced from the ensemble solution and apply to DFT and its interacting potential functional theory (PFT) counterpart. However, the state-specific stationary condition for the non-interacting Kohn-Sham PFT is revealed to be more complicated than the ground state problem, due in part to a contribution from density-driven correlations [Phys. Rev. Lett. 123, 016401 (2019); 124, 243001 (2020); 125, 233001 (2020)] that are neglected in ``SCF'' approaches. Some implications for self-consistency in exact theory and approximations are discussed.
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- Excited-State-Specific Kohn-Sham Formalism for the Asymmetric Hubbard Dimer
- State-specific density functionals for excited states from ensembles
- Excited States of the Uniform Electron Gas
- Exact static linear response of excited states from ensemble density functional theory
- Ensemble density functional theory of excited states: Exact N-centered formalism and practical opportunities