The Lamb shift of the state in hydrogen: two-loop and three-loop contributions
arXiv:1906.11105 · doi:10.1016/j.physletb.2019.06.023
Abstract
We consider the Lamb shift in hydrogen and helium ions, a quantity, required for an accurate determination of the Rydberg constant and the proton charge radius by means of hydrogen spectroscopy, as well as for precision tests of the bound-state QED. The dominant QED contribution to the uncertainty originates from external-field contributions (i.e., the contributions at the non-recoil limit). We discuss the two- and three-loop cases and in particular, we revisit calculations of the coefficients in standard notation. We have found a missing logarithmic contribution of order . We have also obtained leading pure self-energy logarithmic contributions of order and and estimated the subleading terms of order , , and . The determination of those higher-order contributions enabled us to improve the overall accuracy of the evaluation of the two-loop self-energy of the electron. We investigated the asymptotic behavior of the integrand related to the next-to-leading three-loop term (order , coefficient in standard notation) and applied it to approximate integration over the loop momentum. Our result for contributions to the Lamb shift for the total three loop next-to-leading term is . Altogether, we have completed the evaluation of the logarithmic contributions to the Lamb shift of order and reduced the overall uncertainty by approximately a factor of three for H, D, and He as compared with the most recent CODATA compilation.
arXiv comment7 pages, 3 figures
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