Nuclear-size self-energy and vacuum-polarization corrections to the bound-electron g factor
arXiv:1310.0200 · doi:10.1088/0953-4075/46/24/245002
Abstract
The finite nuclear-size effect on the leading bound-electron g factor and the one-loop QED corrections to the bound-electron g factor is investigated for the ground state of hydrogen-like ions. The calculation is performed to all orders in the nuclear binding strength parameter Zα (where Z is the nuclear charge and α is the fine structure constant) and for the Fermi model of the nuclear charge distribution. In the result, theoretical predictions for the isotope shift of the 1s bound-electron g factor are obtained, which can be used for the determination of the difference of nuclear charge radii from experimental values of the bound-electron g factors for different isotopes.
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Cited by in corpus (15)
- QED tests with highly-charged ions
- Stringent test of QED with hydrogenlike tin
- The -factor of light ions for an improved determination of the fine-structure constant
- -factor of Boronlike Argon
- Extraction of the electron mass from factor measurements on light hydrogenlike ions
- Two-loop binding corrections to the electron gyromagnetic factor
- Electron-correlation effects in the -factor of light Li-like ions
- Weighted difference of g-factors of light Li-like and H-like ions for an improved determination of the fine-structure constant
- QED corrections to the factor of Li- and B-like ions
- Testing Standard Model extensions with few-electron ions
- Self-energy screening effects in the factor of Li-like ions
- Electron correlation effects on the factor of lithiumlike ions
- Vacuum polarization and Wichmann-Kroll correction in the finite basis set approximation
- Factor of Boron-like Tin
- Improved bound-electron g-factor theory through complete two-loop QED calculations