1991
DOI: 10.1016/0003-4916(91)90017-3
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Analytic calculation of radiative-recoil corrections to muonium hyperfine splitting: Muon-line contribution

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Cited by 20 publications
(46 citation statements)
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“…Complete formal analysis of the recoil corrections in the framework of the relativistic two-particle equations, with derivation of all relevant kernels, perturbation theory contributions, and necessary subtraction terms may be performed along the same lines as was done for hyperfine splitting in [129]. However, these results may also be understood without a cumbersome formalism by starting with the simple scattering approximation.…”
Section: Fig 35 Irreducible Kernels With Arbitrary Number Of the Exmentioning
confidence: 99%
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“…Complete formal analysis of the recoil corrections in the framework of the relativistic two-particle equations, with derivation of all relevant kernels, perturbation theory contributions, and necessary subtraction terms may be performed along the same lines as was done for hyperfine splitting in [129]. However, these results may also be understood without a cumbersome formalism by starting with the simple scattering approximation.…”
Section: Fig 35 Irreducible Kernels With Arbitrary Number Of the Exmentioning
confidence: 99%
“…More interesting is the low momentum behavior of the electron factor. Due to the generalized low energy theorem for the Compton scattering (see, e.g., [129]), the electron factor has a pole at small momenta and the residue at this pole is completely determined by the one loop anomalous magnetic moment. Hence, naive substitution of the electron factor in eq.…”
Section: Fig 68 Diagrams With Radiative Insertions In the Electron mentioning
confidence: 99%
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“…5, 6 we include in the integral radiatively corrected virtual Compton scattering amplitude instead of the skeleton one. A generalized low energy theorem holds for the virtual Compton scattering amplitude with subtracted anomalous magnetic moment contribution (see more on this subtraction below) [7,8]. According to this theorem the electron (muon) factor L µν (k) is suppressed by an additional factor k 2 /m 2 (k 2 /M 2 ) in comparison with the respective skeleton factor.…”
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confidence: 99%
“…5 with the electron polarization loops generate nonrecoil and logarithm squared, single-logarithmic, and nonlogarithmic radiative-recoil contributions to HFS. It turns out that the gauge invariant anomalous magnetic moment in these diagrams does not generate radiative-recoil corrections (see, e.g., [8,9]). Then the radiatively corrected electron factor L µν provides an additional suppression factor k 2 /m 2 in the skeleton integral over the exchanged momenta.…”
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confidence: 99%