Electronic excited states in extreme limits via ensemble density functionals
arXiv:2205.07136 · doi:10.1103/PhysRevLett.130.106401
Abstract
Density functional theory (DFT) has greatly expanded our ability to affordably compute and understand electronic ground states, by replacing intractable {\em ab initio} calculations by models based on paradigmatic physics from high- and low-density limits. But, a comparable treatment of excited states lags behind. Here, we solve this outstanding problem by employing a generalization of density functional theory to ensemble states (EDFT). We thus address important paradigmatic cases of all electronic systems in strongly (low-density) and weakly (high-density) correlated regimes. We show that the high-density limit connects to recent, exactly-solvable EDFT results. The low-density limit reveals an unnoticed and most unexpected result -- density functionals for strictly correlated {\em ground} states can be reused {\em directly} for excited states. Non-trivial dependence on excitation structure only shows up at third leading order. Overall, our results provide foundations for effective models of excited states that interpolate between exact low- and high-density limits, which we illustrate on the cases of singlet-singlet excitations in H and a ring of quantum wells.
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- 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
- Solving one-body ensemble N-representability problems with spin
- Refining ensemble -representability of one-body density matrices from partial information