4.4 Article

Generalized relativistic small-core pseudopotentials accounting for quantum electrodynamic effects: Construction and pilot applications

Journal

Publisher

WILEY
DOI: 10.1002/qua.27077

Keywords

excitation energy; intermediate Hamiltonians; quantum electrodynamics; relativistic coupled cluster theory; relativistic pseudopotential

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We describe a simple procedure to incorporate one-loop quantum electrodynamic (QED) corrections into the generalized nonlocal shape-consistent relativistic pseudopotential model. Pseudopotentials for Lu, Tl, and Ra are derived from solving reference atomic SCF problems with the Dirac-Coulomb-Breit Hamiltonian, with the model Lamb shift operator added. QED contributions to atomic valence excitation energies are shown to exceed the errors introduced by the pseudopotential approximation by an order of magnitude. We report pilot applications of the new model to calculate excitation energies of atomic systems using the relativistic Fock space coupled cluster method and discuss implications for molecular excited state calculations.
A simple procedure to incorporate one-loop quantum electrodynamic (QED) corrections into the generalized (Gatchina) nonlocal shape-consistent relativistic pseudopotential model is described. The pseudopotentials for Lu, Tl, and Ra replacing only inner core shells (with principal quantum numbers n <= 3 for the two former elements and n <= 4 for the latter one) are derived from the solutions of reference atomic SCF problems with the Dirac-Coulomb-Breit Hamiltonian to which the model Lamb shift operator added. QED contributions to atomic valence excitation energies evaluated at the SCF level are demonstrated to exceed the errors introduced by the pseudopotential approximation itself by an order of magnitude. Pilot applications of the new model to calculations of excitation energies of two-valence-electron atomic systems using the intermediate-Hamiltonian relativistic Fock space coupled cluster method reformulated here for incomplete main model spaces are reported. Implications for high-accuracy molecular excited state calculations are discussed.

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