Building Kohn-Sham potentials for ground and excited states
arXiv:2101.01127 · doi:10.1007/s00205-022-01804-1
Abstract
We analyze the inverse problem of Density Functional Theory using a regularized variational method. First, we show that given and a target density , there exist potentials having bound mixed states which densities are arbitrarily close to . The state can be chosen pure in dimension and without interactions, and we provide numerical and theoretical evidence consistently leading us to conjecture that the same pure representability result holds for , but that the set of pure-state -representable densities is not dense for . Finally, we present an inversion algorithm taking into account degeneracies, removing the generic blocking behavior of standard ones.
References in corpus (3)
Cited by in corpus (14)
- The structure of the density-potential mapping. Part I: Standard density-functional theory
- Exact Excited-State Functionals of the Asymmetric Hubbard Dimer
- Seven Useful Questions in Density Functional Theory
- Ensemble density functional theory of ground and excited energy levels
- Density-potential inversion from Moreau-Yosida regularization
- Some properties of the potential-to-ground state map in quantum mechanics
- Geometry of Degeneracy in Potential and Density Space
- Nuclear energy density functionals from empirical ground-state densities
- Solution of the v-representability problem on a one-dimensional torus
- Excited-State-Specific Kohn-Sham Formalism for the Asymmetric Hubbard Dimer
- Excited States of the Uniform Electron Gas
- Exact static linear response of excited states from ensemble density functional theory
- The complete inverse Kohn-Sham problem: from the density to the energy
- Perspective on Moreau-Yosida Regularization in Density-Functional Theory