QED radiative corrections and many-body effects in atoms: vacuum polarization and binding energy shifts in alkali metals

@article{Ginges2015QEDRC,
  title={QED radiative corrections and many-body effects in atoms: vacuum polarization and binding energy shifts in alkali metals},
  author={J. S. M. Ginges and Julian C. Berengut},
  journal={Journal of Physics B: Atomic, Molecular and Optical Physics},
  year={2015},
  volume={49}
}
  • J. GingesJ. Berengut
  • Published 4 November 2015
  • Physics
  • Journal of Physics B: Atomic, Molecular and Optical Physics
We calculate vacuum polarization corrections to the binding energies in neutral alkali atoms Na through to the superheavy element E119. We employ the relativistic Hartree–Fock method to demonstrate the importance of relaxation of the electronic core and the correlation potential method to study the effects of second and higher orders of perturbation theory. These many-body effects are sizeable for all orbitals, though particularly important for orbitals with angular momentum quantum number l… 

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References

SHOWING 1-10 OF 36 REFERENCES

QED corrections to the parity-nonconserving 6s-7s amplitude in 133Cs.

The complete gauge-invariant set of the one-loop QED corrections to the parity-nonconserving 6s-7s amplitude in 133Cs is evaluated to all orders in alphaZ using a local version of the

Revisiting parity nonconservation in cesium.

The interpretation of the PNC measurements in cesium still indicates reasonable agreement with the standard model (1.5σ); however, the sum-over-states approach gives new constraints on physics beyond it.

Phys

  • Rev. A 66, 042501
  • 2002

Phys

  • Lett. A 140, 493
  • 1989

Phys

  • Rev. A 91, 042505
  • 2015

Phys

  • Rev. A 82, 062503
  • 2010

Phys

  • Rev. A 59, 2707
  • 1999

Phys

  • Rev. Lett. 109, 203003
  • 2012

Phys

  • Rev. 99, 510
  • 1955

Phys

  • Rev. A 87, 054502
  • 2013