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-
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8
-
-
85015774156
-
-
note
-
-1 (inverse seconds). At Z = 1, this is equivalent to the "famous" value of 1.3 Hz which is nowadays most frequently quoted in the literature.
-
-
-
-
12
-
-
0000120236
-
-
T. Udem, A. Huber, B. Gross, J. Reichert, M. Prevedelli, M. Weitz, and T. W. Hänsch, Phys. Rev. Lett. 79, 2646 (1997).
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Udem, T.1
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0033089735
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A. Huber, B. Gross, M. Weitz, and T. W. Hänsen, Phys. Rev. A 59, 1844 (1999).
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Huber, A.1
Gross, B.2
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Hänsen, T.W.4
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14
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0000306406
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J. Reichert, M. Niering, R. Holzwarth, M. Weitz, T. Udem, and T. W. Hänsch, Phys. Rev. Lett. 84, 3232 (2000).
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Reichert, J.1
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Hänsch, T.W.6
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15
-
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0033703942
-
-
M. Niering, R. Holzwarth, J. Reichert, P. Pokasov, T. Udem, M. Weitz, T. W. Hänsch, P. Lemonde, G. Santarelli, M. Abgrall, P. Laurent, C. Salomon, and A. Clairon, Phys. Rev. Lett. 84, 5496 (2000).
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Niering, M.1
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Hänsch, T.W.7
Lemonde, P.8
Santarelli, G.9
Abgrall, M.10
Laurent, P.11
Salomon, C.12
Clairon, A.13
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16
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0001595265
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B. de Beauvoir, F. Nez, L. Julien, B. Cagnac, F. Biraben, D. Touahri, L. Hilico, O. Acef, A. Clairon, and J. J. Zondy, Phys. Rev. Lett. 78, 440 (1997).
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Clairon, A.9
Zondy, J.J.10
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17
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0034288279
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B. de Beauvoir, C. Schwob, O. Acef, L. Jozefowski, L. Hilico, F. Nez, L. Julien, A. Clairon, and F. Biraben, Eur. Phys. J. D 12, 61 (2000).
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27
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0003684962
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(Cambridge University Press, Cambridge, England), V.1. 1
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S. Weinberg, The Quantum Theory of Fields (Cambridge University Press, Cambridge, England, 1995), V.1. 1.
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Weinberg, S.1
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Schlicher, R.R.1
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33
-
-
85015741892
-
-
note
-
In a number of cases, the formulation of a quantum electrodynamic bound-state problem may be simplified drastically when employing the concepts of an effective low-energy field theory known as nonrelativistic quantum electrodynamics [19]. The basic idea consists in a correspondence between fully relativistic quantum electrodynamics and effective low-energy couplings between the electron and the radiation field, which may still lead to ultraviolet divergent expressions. However, the ultraviolet divergences may be matched against effective high-energy operators, which leads to a cancellation of the cutoff parameters. Within the context of higher-order binding corrections to the one-loop self-energy problem, this has been discussed in [23,24].
-
-
-
-
35
-
-
85015737245
-
-
note
-
2 in the propagator denominators of the second and third terms in curly brackets in Eq. (31) of [39] should be interchanged as indicated in Eq. (2). The further calculations described in [39], especially the double logarithms indicated in Eqs. (32) and (33) of [39], do not receive any corrections.
-
-
-
-
36
-
-
85015723309
-
-
note
-
The other terms in Eq. (2) (not only the first three in curly brackets) may also generate imaginary parts, but they do so only if the reference state is a higher excited S or P state in which case one-photon decay is possible. Indeed, for higher excited S or P states, the additional imaginary energy shifts find a natural interpretation as radiative corrections to the one-photon decay width of these states [41].
-
-
-
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37
-
-
3042830136
-
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e-print physics/9702027; a related publication is
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S. G. Karshenboim and V. G. Ivanov, e-print physics/9702027; a related publication is Opt. Spectrosc. 83, 1 (1997).
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Karshenboim, S.G.1
Ivanov, V.G.2
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0003084053
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edited by T. Kinoshita (World Scientific, Singapore)
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Sapirstein, J.1
Yennie, D.R.2
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53
-
-
85015738044
-
-
note
-
The accuracy of the present calculation for the total radiative effects should therefore be estimated as roughly 20% for Z = 1 and Z = 2.
-
-
-
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55
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0342560726
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A. J. Duncan, Z. A. Sheikh, H.-J. Beyer, and H. Kleinpoppen, J. Phys. B 30, 1347 (1997).
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0039028881
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Dunford, R.W.1
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58
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0000600798
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Y. B. Zel'dovich, Zh. Eksp. Teor. Fiz. 33, 1531 (1957) [Sov. Phys. JETP 6, 1184 (1958)].
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60
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