Abstract
We obtain the shielding of the nuclear magnetic moment by an electron in the state in a hydrogenlike ion with arbitrary nuclear charge . The calculation is based on the decomposition of the shielding correction into two terms corresponding to the intermediate states with and . The former is evaluated using the projection of the correction to the electron wave function due to the external magnetic field, while the latter is calculated by applying the projection of the correction to the wave function due to the hyperfine interaction between the electron and the nucleus.
- Received 29 May 2008
DOI:https://doi.org/10.1103/PhysRevA.79.012512
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