1992
DOI: 10.1016/0370-2693(92)91649-t
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Coulomb line vacuum polarization corrections to Lamb shift of order α2(Zα)5m

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Cited by 37 publications
(41 citation statements)
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“…(67) Corrections of order α 2 (Zα) 5 have the same physical origin as corrections of order α(Zα) 5 , and the scattering approximation is sufficient for their calculation [70]. We consider now corrections of higher order in α than in the previous section and there is a larger variety of relevant graphs.…”
Section: Total Correction Of Ordermentioning
confidence: 99%
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“…(67) Corrections of order α 2 (Zα) 5 have the same physical origin as corrections of order α(Zα) 5 , and the scattering approximation is sufficient for their calculation [70]. We consider now corrections of higher order in α than in the previous section and there is a larger variety of relevant graphs.…”
Section: Total Correction Of Ordermentioning
confidence: 99%
“…We consider now corrections of higher order in α than in the previous section and there is a larger variety of relevant graphs. All six gauge invariant sets of diagrams [70] 5 , corrections to the energy shifts are given by the matrix elements of the diagrams in Fig. 20 calculated between free electron spinors with all external electron lines on the mass shell, projected on the respective spin states, and multiplied by the square of the Schrödinger-Coulomb wave function at the origin [70].…”
Section: Total Correction Of Ordermentioning
confidence: 99%
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“…The next three corrections respectively give radiative recoil [10], additional pure recoil [23,24], and higher order radiative effects which involve double Coulomb exchange [25][26][27]. The first two terms above give -0.0025 MHz and 0.0032 MHz, respectively while the last is incomplete but gives 0.0057 MHz from the diagrams calculated to date.…”
Section: Theoretical Expression For the Lamb Shift (2s½-2p½)mentioning
confidence: 93%