1981
DOI: 10.1103/physrevlett.46.232
|View full text |Cite
|
Sign up to set email alerts
|

Measurement of the Lamb Shift in Hydrogen,n=2

Abstract: A measurement based on the fast-atomic-beam separated-oscillatory-field method of sub-natural-linewidth spectroscopy gives, for the Lamb shift in hydrogen, S(w =2) = 1057.845(9) MHz. The result is not in good agreement with theory.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

5
153
0

Year Published

1996
1996
2018
2018

Publication Types

Select...
6
3
1

Relationship

0
10

Authors

Journals

citations
Cited by 261 publications
(158 citation statements)
references
References 10 publications
5
153
0
Order By: Relevance
“…One is the classic 2S 1/2 -2P 1/2 Lamb shift measured by several groups [20], [21], [19], and the second is the combined Lamb shift L(4S − 2S) − 1 4 L(2S − 1S) as measured by the Hänsch group (for a review see [22]). The experimental value of 2S Lamb shift can be extracted from E(2S-2P 1/2 ) having the precise value for 2P 1/2 Lamb shift, and can also be determined from the combined Lamb shift through the formula…”
Section: Results and Conclusionmentioning
confidence: 99%
“…One is the classic 2S 1/2 -2P 1/2 Lamb shift measured by several groups [20], [21], [19], and the second is the combined Lamb shift L(4S − 2S) − 1 4 L(2S − 1S) as measured by the Hänsch group (for a review see [22]). The experimental value of 2S Lamb shift can be extracted from E(2S-2P 1/2 ) having the precise value for 2P 1/2 Lamb shift, and can also be determined from the combined Lamb shift through the formula…”
Section: Results and Conclusionmentioning
confidence: 99%
“…A natural way to obtain a self-consistent value of the 1S Lamb shift independent of the experimental data on the 2S −2P splitting, is provided by the theoretical relation between the 1S and 2S Lamb shifts discussed above in Section XXXIX C. An important advantage of the self-consistent method is that it produces an unbiased value of the L(1S) Lamb shift independent of the widely scattered experimental data on the 2S − 2P interval. Spectacular experimental progress in the frequency measurement now allows one to obtain self-consistent values of 1S Lamb shift from the experimental data [3], with comparable or even better accuracy (see five lines in Table XXI below the theoretical values in the middle of the Table) than in the method based on experimental results of the classic Lamb shift in [320,316]. The original experimental numbers from [3,311] in the fourth and fifth lines in Table XXI are averages of the self-consistent values and the values based on the classic Lamb shift.…”
Section: Comparison Of Theory and Experimentsmentioning
confidence: 99%
“…6 confirms the presence of two irreducible submatrices of H Fz =0 . Indeed, the two uncoupled subspaces are spanned by the states |Ψ i with i = 1, 2, 5, 7,8,11,15,16,18,21,22, 24 (subspace I), and |Ψ j with j = 3, 4,6,9,10,12,13,14,17,19,20,23 (subspace II). An ordering of the eigenvalues reveals that one can have coupling among the S-S and P -P states (distributed among atoms A and B), forming submanifold I, and among all S-P and P -S states (distributed among atoms A and B), forming submanifold II.…”
Section: S-2s Interaction In Hydrogenmentioning
confidence: 99%