Perturbation Approach to the Self Energy of non-S Hydrogenic States
arXiv:physics/0304068 · doi:10.1103/PhysRevA.68.042101
Abstract
We present results on the self-energy correction to the energy levels of hydrogen and hydrogenlike ions. The self energy represents the largest QED correction to the relativistic (Dirac-Coulomb) energy of a bound electron. We focus on the perturbation expansion of the self energy of non-S states, and provide estimates of the so-called A60 perturbative coefficient, which can be considered as a relativistic Bethe logarithm. Precise values of A60 are given for many P, D, F and G states, while estimates are given for other electronic states. These results can be used in high-precision spectroscopy experiments in hydrogen and hydrogenlike ions. They yield the best available estimate of the self-energy correction of many atomic states.
18 pages (in 2-column format), 21 figures. Version 2 (June 20, 2003) includes minor modifications
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- Mass Measurements and the Bound--Electron g Factor
- Improved all-order results for the one-loop QED correction to the hyperfine structure in light H-like atoms
- Three-Loop Reducible Radiative Photon Contributions to Lamb Shift and Hyperfine Splitting
- Relativistic and Radiative Energy Shifts for Rydberg States
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- Quantum Electrodynamic Corrections to Cyclotron States in a Penning Trap
- Relativistic Ritz approach to hydrogen-like atoms I: theoretical considerations
- Techniques in Analytic Lamb Shift Calculations
- Precision Rydberg State Spectroscopy with Slow Electrons and Proton Radius Puzzle
- Toward high-precision values of the self energy of non-S states in hydrogen and hydrogen-like ions