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The Fine Structure of the $\alpha $-Line of Heavy Hydrogen
In continuation of work reported earlier (Kuhn & Series 1950), the weak satellite $\alpha $-line in the 2P$_{\frac{3}{2}}$-3S$_{\frac{1}{2}}$ 6561 angstrom of the Balmer series of heavy hydrogen has been resolved. The light was produced as before in a U-tube cooled by liquid hydrogen, and analyz...
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Published in: | Proceedings of the Royal Society of London. Series A, Mathematical and physical sciences Mathematical and physical sciences, 1951-08, Vol.208 (1093), p.277-284 |
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Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In continuation of work reported earlier (Kuhn & Series 1950), the weak satellite $\alpha $-line in the 2P$_{\frac{3}{2}}$-3S$_{\frac{1}{2}}$
6561 angstrom of the Balmer series of heavy hydrogen has been resolved. The light was produced as before in a U-tube cooled
by liquid hydrogen, and analyzed by a double Fabry-Perot interferometer with spacings in the ratio 1:2. The satellite was
found to be at a distance 0$\cdot $1326 $\pm $ 0$\cdot $001 cm.$^{-1}$ from the neighbouring strong component 2P$_{\frac{3}{2}}$-3D$_{\frac{5}{2}}$,
in disagreement with the distance 0$\cdot $1409 cm.$^{-1}$ predicted by the Dirac relativistic theory of the hydrogen atom.
The difference 0$\cdot $0083$_{-0\cdot 003}^{+0\cdot 002}$ cm.$^{-1}$ (where the limits also include possible errors in certain
corrections) is interpreted as an upward shift of the 3S term, and is compared with the value 0$\cdot $0104 cm.$^{-1}$ predicted
by the radiation theory of Bethe and others (see, for example, Bethe, Brown & Stehn 1950). |
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ISSN: | 1364-5021 0080-4630 1471-2946 2053-9169 |
DOI: | 10.1098/rspa.1951.0159 |