Relaxation effect and radiative corrections in many-electron atoms
arXiv:physics/0401043 · doi:10.1103/PhysRevA.69.054502
Abstract
We illuminate the importance of a self-consistent many-body treatment in calculations of vacuum polarization corrections to the energies of atomic orbitals in many-electron atoms. Including vacuum polarization in the atomic Hamiltonian causes a substantial re-adjustment (relaxation) of the electrostatic self-consistent field. The induced change in the electrostatic energies is substantial for states with the orbital angular momentum $l &;gt; 0$. For such orbitals, the relaxation mechanism determines the sign and even the order of magnitude of the total vacuum polarization correction. This relaxation mechanism is illustrated with numerical results for the Cs atom.
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- Electron structure of superheavy elements Uut, Fl and Uup (=113 to 115)
- Precision theoretical determination of electric-dipole matrix elements in atomic cesium
- Electric dipole transition amplitudes for atoms and ions with one valence electron
- QED radiative corrections to electric dipole amplitudes in heavy atoms
- All-order calculations of the spectra of superheavy elements E113 and E114
- Electric dipole polarizabilities of doubly ionized alkaline Earth metal ions from perturbed relativistic coupled-cluster theory
- Many-body and QED effects in electron-atom inelastic scattering in EELS
- Vacuum polarization corrections to hyperfine structure in many-electron atoms