Relativistic two fermion treatment of hyperfine transitions
arXiv:1408.2433 · doi:10.1088/0953-4075/48/8/085002
Abstract
A system of two fermions with different masses and interacting by the Coulomb potential is presented in a completely covariant framework. The spin-spin interaction, including the anomalous magnetic moments of the two fermions, is added by means of a Breit term. We solve the resulting fourth order differential system by evaluating the spectrum and the eigenfunctions. The interaction vertex with an external electromagnetic field is then determined. The relativistic eigenfunctions are used to study the photon emission from a hyperfine transition and are checked for the calculation of the Lamb shift due to the electron vacuum polarization in the muonic Hydrogen.
arXiv comment8 pages
References in corpus (12)
- Precision physics of simple atoms: QED tests, nuclear structure and fundamental constants
- Potential model calculations and predictions for heavy quarkonium
- Hyperfine Structure of the Ground and First Excited States in Light Hydrogen-Like Atoms and High-Precision Tests of QED
- The contributions to the Lamb shift and the fine structure in light muonic atoms
- Hyperfine splittings in the system
- Non-Perturbative Relativistic Calculation of the Muonic Hydrogen Spectrum
- The Hyperfine Splittings in Heavy-Light Mesons and Quarkonia
- Fine and hyperfine structure of the muonic ^3He ion
- Unified covariant treatment of hyperfine splitting for heavy and light mesons
- Two fermion relativistic bound states
- Two fermion relativistic bound states: hyperfine shifts
- Semirelativistic Bound-State Equations: Trivial Considerations