Excitation energies from density functional perturbation theory
Claudia Filippi (University of Illinois at Urbana-Champaign) C. J., Umrigar (Cornell University) X. Gonze (Universit\'e Catholique de Louvain)

TL;DR
This paper explores two perturbative methods based on density functional theory to accurately compute atomic excitation energies, comparing their performance and improvements over existing approaches using various exchange-correlation potentials.
Contribution
It introduces and evaluates two perturbative schemes for excitation energies using the Kohn-Sham Hamiltonian with accurate exchange-correlation potentials, comparing their effectiveness and improvements over prior methods.
Findings
First-order corrections improve excitation energies, especially in one scheme.
Zeroth-order Kohn-Sham eigenvalue differences nearly bracket experimental energies.
Perturbation theory results are compared with $ riangle$SCF and TDDFT methods.
Abstract
We consider two perturbative schemes to calculate excitation energies, each employing the Kohn-Sham Hamiltonian as the unperturbed system. Using accurate exchange-correlation potentials generated from essentially exact densities and their exchange components determined by a recently proposed method, we evaluate energy differences between the ground state and excited states in first-order perturbation theory for the Helium, ionized Lithium and Beryllium atoms. It was recently observed that the zeroth-order excitations energies, simply given by the difference of the Kohn-Sham eigenvalues, almost always lie between the singlet and triplet experimental excitations energies, corrected for relativistic and finite nuclear mass effects. The first-order corrections provide about a factor of two improvement in one of the perturbative schemes but not in the other. The excitation energies within…
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