Relativistic two-electron atomic and molecular energies using coupling and double groups: role of the triplet contributions to singlet states
arXiv:2211.14180 · doi:10.1063/5.0136360
Abstract
The triplet contribution is computed to the 1 and 2 states of the He atom, to the state of the Li and Be ions, and to the ground state of the H molecule by extensive use of double-group symmetry (equivalent to coupling for the atomic systems) during the course of the variational solution of the no-pair Dirac-Coulomb-Breit wave equation. The no-pair Dirac-Coulomb-Breit energies are converged within a sub-parts-per-billion relative precision using an explicitly correlated Gaussian basis optimized to the non-relativistic energies. The fine-structure constant dependence of the triplet sector contribution to the variational energy is at leading order, in agreement with the formal perturbation theory result available from the literature.
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Cited by in corpus (8)
- The Bethe-Salpeter QED wave equation for bound-state computations of atoms and molecules
- Bound-state relativistic quantum electrodynamics: a perspective for precision physics with atoms and molecules
- Regularized relativistic corrections for polyelectronic and polyatomic systems with explicitly correlated Gaussians
- Pre-Born-Oppenheimer Dirac-Coulomb-Breit computations for two-body systems
- QED corrections to the correlated relativistic energy: one-photon processes
- One-particle operator representation over two-particle basis sets for relativistic QED computations
- Rovibrational computations for the He a state including non-adiabatic, relativistic, and QED corrections
- Double-pair Coulomb and Breit photon correction to the correlated relativistic energy