335 research outputs found

    Vacuum polarization calculations for hydrogenlike and alkalilike ions

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    Complete vacuum polarization calculations incorporating finite nuclear size are presented for hydrogenic ions with principal quantum numbers n=1-5. Lithiumlike, sodiumlike, and copperlike ions are also treated starting with Kohn-Sham potentials, and including first-order screening corrections. In both cases dominant Uehling terms are calculated with high accuracy, and smaller Wichmann- Kroll terms are obtained using numerical electron Green's functions.Comment: 23 pages, 1 figur

    Recoil corrections in the hydrogen isoelectronic sequence

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    A version of the Bethe-Salpeter equation appropriate for calculating recoil corrections in highly charged hydrogenlike ions is presented. The nucleus is treated as a scalar particle of charge Z, and the electron treated relativistically. The known recoil corrections of order m2/M(Zα)4m^2/M(Z\alpha)^4 are derived in both this formalism and in NRQED

    Electron Self Energy for Higher Excited S Levels

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    A nonperturbative numerical evaluation of the one-photon electron self energy for the 3S and 4S states with charge numbers Z=1 to 5 is described. The numerical results are in agreement with known terms in the expansion of the self energy in powers of Zalpha.Comment: 3 pages, RevTeX, to appear in Phys. Rev.

    Radiative and interelectronic-interaction corrections to the hyperfine splitting in highly charged B-like ions

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    The ground-state hyperfine splitting values of high-Z boronlike ions are calculated. Calculation of the interelectronic-interaction contribution is based on a combination of the 1/Z perturbation theory and the large-scale configuration-interaction Dirac-Fock-Sturm method. The screened QED corrections are evaluated utilizing an effective screening potential approach. Total hyperfine splitting energies are presented for several B-like ions of particular interest: {}^{45}Sc{}^{16+}, {}^{57}Fe{}^{21+}, {}^{207}Pb{}^{77+}, and {}^{209}Bi{}^{78+}. For lead and bismuth the experimental values of the 1s hyperfine splitting are employed to improve significantly the theoretical results by reducing the uncertainty due to the nuclear effects.Comment: 12 pages, 2 figures, 3 table

    Lamb shift in muonic deuterium atom

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    We present new investigation of the Lamb shift (2P_{1/2}-2S_{1/2}) in muonic deuterium (mu d) atom using the three-dimensional quasipotential method in quantum electrodynamics. The vacuum polarization, nuclear structure and recoil effects are calculated with the account of contributions of orders alpha^3, alpha^4, alpha^5 and alpha^6. The results are compared with earlier performed calculations. The obtained numerical value of the Lamb shift 202.4139 meV can be considered as a reliable estimate for the comparison with forthcoming experimental data.Comment: 24 pages, 11 figures. arXiv admin note: text overlap with arXiv:hep-ph/061229

    Hadronic Vacuum Polarization and the Lamb Shift

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    Recent improvements in the determination of the running of the fine-structure constant also allow an update of the hadronic vacuum-polarization contribution to the Lamb shift. We find a shift of -3.40(7) kHz to the 1S level of hydrogen. We also comment on the contribution of this effect to the determination by elastic electron scattering of the r.m.s. radii of nuclei.Comment: 7 pages, latex, 1 figure -- Submitted to Phys. Rev. A -- epsfig.sty require

    Relativistic, QED, and nuclear mass effects in the magnetic shielding of 3^3He

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    The magnetic shielding σ\sigma of 3^3He is studied. The complete relativistic corrections of order O(α2)O(\alpha^2), leading QED corrections of order O(α3lnα)O(\alpha^3 \ln\alpha), and finite nuclear mass effects of order O(m/mN)O(m/m_{\rm N}) are calculated with high numerical precision. The resulting theoretical predictions for σ=59.967 43(10)106\sigma = 59.967~43(10)\cdot 10^{-6} are the most accurate to date among all elements and support the use of 3^3He as a NMR standard.Comment: 10 pages, corrected minor errors in Eqs.(6,7

    Hadronic Vacuum Polarization Contribution to the Muonium Hyperfine Splitting

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    We discuss hadronic effects in the muonium hyperfine structure and derive an expression for the hadronic contribution to the hfs interval in form of the one-dimensional integral of the cross section of e+e- annihilation into hadrons. Higher-order hadronic contributions are also considered

    Precise calculation of transition frequencies of hydrogen and deuterium based on a least-squares analysis

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    We combine a limited number of accurately measured transition frequencies in hydrogen and deuterium, recent quantum electrodynamics (QED) calculations, and, as an essential additional ingredient, a generalized least-squares analysis, to obtain precise and optimal predictions for hydrogen and deuterium transition frequencies. Some of the predicted transition frequencies have relative uncertainties more than an order of magnitude smaller than that of the g-factor of the electron, which was previously the most accurate prediction of QED.Comment: 4 pages, RevTe

    Stark shift and parity non-conservation for near-degenerate states of xenon

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    We identify a pair of near-degenerate states of opposite parity in atomic Xe, the 5p^5 10s \,\, ^2[3/2]_2^o at E=94759.927\rm{E}=94759.927 cm1^{-1} and 5p^5 6f \,\, ^2[5/2]_2 at E=94759.935\rm{E}= 94759.935 cm1^{-1}, for which parity- and time-odd effects are expected to be enhanced by the small energy separation. We present theoretical calculations which indicate narrow widths for both states and we report a calculated value for the weak matrix element, arising from configuration mixing, of W=2.1|W|=2.1 Hz for 132^{132}Xe. In addition, we measured the Stark effect of the 5p56f5p^5\,6f 2[5/2]2^2[5/2]_{2} and 5p56f 2[3/2]25p^5 \,6f \ ^2[3/2]_2 (E=94737.121cm1\rm{E} =94737.121\,\rm{cm}^{-1}) states. The Stark-shift of the 6f6f states is observed to be negative, revealing the presence of nearby 6g6g states at higher energies, which have not been observed before. The Stark-shift measurements imply an upper limit on the weak matrix element of W ⁣< ⁣5|W|\!<\!5 Hz for the near-degenerate states (10s \,\, ^2[3/2]_2^o and 6f \,\, ^2[5/2]_2), which is in agreement with the presented calculations.Comment: 11 pages, 6 figure
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