QED corrections of order α(Zα)2EF to the hyperfine splitting of P1/2 and P3/2 states in hydrogenlike ions

The hyperfine structure (HFS) of a bound electron is modified by the self-interaction of the electron with its own radiation field. This effect is known as the self-energy correction. In this work, we discuss the evaluation of higher order self-energy corrections to the HFS of bound P states. These...

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Main Authors: Jentschura, Ulrich D. (Author) , Yerokhin, Vladimir (Author)
Format: Article (Journal)
Language:English
Published: 11 January 2010
In: Physical review. A, Atomic, molecular, and optical physics
Year: 2010, Volume: 81, Pages: 1-10
ISSN:1094-1622
DOI:10.1103/PhysRevA.81.012503
Online Access:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1103/PhysRevA.81.012503
Verlag, lizenzpflichtig, Volltext: https://link.aps.org/doi/10.1103/PhysRevA.81.012503
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Author Notes:Ulrich D. Jentschura (Department of Physics, Missouri University of Science and Technology, Rolla, Missouri, USA and Institut für Theoretische Physik, Universität Heidelberg, Germany), Vladimir A. Yerokhin (Max-Planck-Institut für Kernphysik, Heidelberg, Germany and Center for Advanced Studies, St. Petersburg State Polytechnical University, St. Petersburg, Russia)

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245 1 0 |a QED corrections of order α(Zα)2EF to the hyperfine splitting of P1/2 and P3/2 states in hydrogenlike ions  |c Ulrich D. Jentschura (Department of Physics, Missouri University of Science and Technology, Rolla, Missouri, USA and Institut für Theoretische Physik, Universität Heidelberg, Germany), Vladimir A. Yerokhin (Max-Planck-Institut für Kernphysik, Heidelberg, Germany and Center for Advanced Studies, St. Petersburg State Polytechnical University, St. Petersburg, Russia) 
246 3 3 |a QED corrections of order α(Zα) 2 E F to the hyperfine splitting of P 1/2 and P 3/2 states in hydrogenlike ions 
246 3 3 |a QED corrections of order α(Zα)2EF to the hyperfine splitting of P1/2 and P3/2 states in hydrogenlike ions 
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520 |a The hyperfine structure (HFS) of a bound electron is modified by the self-interaction of the electron with its own radiation field. This effect is known as the self-energy correction. In this work, we discuss the evaluation of higher order self-energy corrections to the HFS of bound P states. These are expressed in a semianalytic expansion involving powers of Zα and ln(Zα), where Z is the nuclear charge number and α is the fine-structure constant. We find that the correction of relative order α(Zα)2 involves only a single logarithm ln(Zα) for P1/2 states [but no term of order α(Zα)2ln2(Zα)], whereas for P3/2 states, even the single logarithm vanishes. By a Foldy-Wouthuysen transformation, we identify a nuclear-spin-dependent correction to the electron’s transition current, which contributes to the HFS of P states. A comparison of the obtained analytic results to a numerical approach is made. 
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