Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...

transition λ (nm) source Aik(·10 6 1/s) source
5S1/2 → 5P1/2 794.9788509 [34] 36.1285 [34]
5S1/2 → 5P3/2 780.241209686 [34] 38.1156 [34]
5S1/2 → 6P1/2 421.6726 [18] 1.769 [35]
5S1/2 → 6P3/2 420.2989 [18] 1.499 [35]
5S1/2 → 7P1/2 359.2597 [18] 0.2890 [35]
5S1/2 → 7P3/2 358.8073 [18] 8.300 [35]
5S1/2 → 8P1/2 335.1775 [18] 8.912 · 10 −2 [35]
5S1/2 → 8P3/2 334.9658 [18] 0.1370 [35]
5S1/2 → 9P1/2 323.0088 [18] 4.231 · 10 −2 [35]
5S1/2 → 9P3/2 322.8911 [18] 6.380 · 10 −2 [35]
5S1/2 → 10P1/2 315.9173 [18] 2.209 · 10 −2 [35]
5S1/2 → 10P3/2 315.8444 [18] 3.716 · 10 −2 [35]
5S1/2 → 11P1/2 311.3950 [18] 1.398 · 10 −2 [35]
5S1/2 → 11P3/2 311.3468 [18] 2.763 · 10 −2 [35]
5S1/2 → 12P1/2 308.3229 [18] 7.692 · 10 −3 [35]
5S1/2 → 12P3/2 308.2893 [18] 1.639 · 10 2 [35]
5S1/2 → 13P1/2 306.1375 [18] 4.955 · 10 −3 [35]
5S1/2 → 13P3/2 306.1131 [18] 1.155 · 10 −2 [35]
Table C.1: Wavelengths and Einstein-coefficients for the calculation of the energy shift
of the ground state
transition λ (nm) source Aik(·10 6 1/s) source
5P3/2 → 6S1/2 1366.875 [18] 14.63 [36]
5P3/2 → 7S1/2 741.02136 [18] 4.552 [19]
5P3/2 → 8S1/2 616.13310 [18] 2.183 [19]
5P3/2 → 4D3/2 1529.261 [18] 1.776 [19]
5P3/2 → 4D5/2 1529.366 [18] 10.67 [19]
5P3/2 → 5D3/2 776.15716 [18] 0.6711 [19]
5P3/2 → 5D5/2 775.97855 [18] 3.937 [19]
5P3/2 → 6D3/2 630.09666 [18] 0.6305 [19]
5P3/2 → 6D5/2 630.00670 [18] 3.717 [19]
Table C.2: Wavelengths and Einstein-coefficients for the calculation of the energy shift
of the 5P3/2 state
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