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Table 5

Comparison of our fine-tuned oscillator strengths in the length gauge with the limited experimental determinations currently available.

Lower level Upper level λexp (Å) Model 2 Ferrero ZF FL Fechalk JT
3d9 2D5∕2 3d8(1G)4p 2F 1317.22 0.0686 0.0571
3d8(1D)4p 2D 1454.84 0.0520 0.0276 0.0323 0.0260
3d8(1D)4p 2D 1467.26 0.0037 0.0060 0.0063
3d8(1D)4p 2F 1467.76 0.1750 0.0097 0.0099
3d8(1D)4p 2F 1477.22 0.0011 0.0010
3d8(3F)4p 2D 1703.40 0.0115 0.0060
3d8(3F)4p 2F 1709.60 0.0181 0.0356 0.0351 0.0324
3d8(3F)4p 2F 1751.91 0.0423 0.0264 0.0227
3d8(3F)4s 4F9∕2 3d8(3F)4p 4F 2125.91 0.0053 0.0050 0.0022
3d8(3F)4s 4F7∕2 3d8(3F)4p 4F 2138.58 0.0137 0.0173 0.0091
3d8(3F)4s 4F5∕2 3d8(3F)4p 4F 2158.74 0.0234 0.0233 0.0171
3d8(3F)4s 4F9∕2 3d8(3F)4p 4F 2165.55 0.1378 0.2596 0.1660
3d8(3F)4s 4F7∕2 3d8(3F)4p 4F 2169.09 0.1109 0.1567 0.1064
3d8(3F)4s 4F5∕2 3d8(3F)4p 4F 2175.14 0.1297 0.1959 0.1264
3d8(3F)4s 4F9∕2 3d8(3F)4p 4G 2179.45 0.0035 0.0015
3d8(3F)4s 4F3∕2 3d8(3F)4p 4F 2184.60 0.2370 0.3250 0.2032
3d8(3F)4s 2F7∕2 3d8(3F)4p 2F 2224.36 0.0900 0.0173
3d8(3F)4s 2F7∕2 3d8(3F)4p 2D 2278.77 0.1145 0.1936
3d8(3F)4s 2F7∕2 3d8(3F)4p 2F 2296.55 0.2444 0.1725
3d8(3F)4s 2F5∕2 3d8(3F)4p 2F 2298.27 0.1554 0.2197
3d8(3F)4s 2F7∕2 3d8(3F)4p 2G 2334.59 0.0357 0.0818 0.0656
3d8(3F)4s 2F5∕2 3d8(3F)4p 2D 2356.40 0.0397 0.0247
3d8(3F)4s 2F5∕2 3d8(3F)4p 2F 2375.42 0.0441 0.0728
3d8(3F)4s 2F7∕2 3d8(3F)4p 2G 2394.52 0.3248 0.2473 0.1849
3d8(3F)4s 2F5∕2 3d8(3F)4p 2G 2416.14 0.3315 0.3094 0.2248

References. The quoted oscillator strengths are from the works of Ferrero: Ferrero et al. (1997), ZF: Zsargó & Federman (1998), FL: Fedchak & Lawler (1999), Fedchalk: Fedchak et al. (2000), and JT: Jenkins & Tripp (2006).

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