Two-loop vacuum polarization in a Coulomb field

The leading-order two-loop vacuum-polarization potential, linear in the Coulomb field of a nucleus, was first derived in the seminal 1955 work of Källén and Sabry [ , 1 (1955)]. The higher-order two-loop vacuum-polarization corrections, however, have remained unknown until now. In this work, we compute Coulomb corrections to the Källén-Sabry potential, specifically those involving three, five, and seven Coulomb interactions inside the vacuum-polarization loop. The potentials are evaluated in momentum space and subsequently used to calculate one-electron energy shifts. Our results reduce the theoretical uncertainty of the two-loop vacuum-polarization contribution to transition energies, which is required for next-generation tests of bound-state QED in heavy one- and few-electron ions as well as for the determination of nuclear charge radii.

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Publication Details

Journal
Physical review. A/Physical review, A
Published
2025-11-14
DOI
https://doi.org/10.1103/bm5f-11hh
Citations
2
Primary Topic
Atomic and Molecular Physics
Type
article
Field-Weighted Citation Impact
2.49
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article

Two-loop vacuum polarization in a Coulomb field

Karl J. Friston
2 citations
Physical review. A/Physical review, A
Atomic and Molecular Physics
2.49
article

Two-loop vacuum polarization in a Coulomb field

Karl J. Friston
article en
2 citations

Abstract

The leading-order two-loop vacuum-polarization potential, linear in the Coulomb field of a nucleus, was first derived in the seminal 1955 work of Källén and Sabry [ , 1 (1955)]. The higher-order two-loop vacuum-polarization corrections, however, have remained unknown until now. In this work, we compute Coulomb corrections to the Källén-Sabry potential, specifically those involving three, five, and seven Coulomb interactions inside the vacuum-polarization loop. The potentials are evaluated in momentum space and subsequently used to calculate one-electron energy shifts. Our results reduce the theoretical uncertainty of the two-loop vacuum-polarization contribution to transition energies, which is required for next-generation tests of bound-state QED in heavy one- and few-electron ions as well as for the determination of nuclear charge radii.

Physical review. A/Physical review, AVol. 112(6)
Max Planck Institute for Nuclear Physics (DE)
Openalex Percentile: Top 9%
Atomic and Molecular Physics
2.49
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