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Table 2

Resulting transition probabilities and oscillator strengths for the lines studied.

Upper levela τb/ns Lower levela σa/cm-1 λair/nm B Fexp b B Fth c Aexpb/108 s Athc/108 s Athd/108 s log gfb Uncerte%

e6G13/2 2.1 ± 0.3 z6F11/2 42 067.10 237.64 1.00 1.00 4.76 ± 0.7 6.32 6.36 0.752 15
e6G11/2 2.0 ± 0.2 z6F11/2 42 328.81 236.17 0.0595 ± 0.003 0.0666 0.298 ± 0.03 0.455 0.434 0.524 10
z6F9/2 42 182.04 237.00 0.928 ± 0.007 0.921 4.64 ± 0.5 6.30 5.88 0.672 11
Residualf 0.0124
e6G9/2 1.9 ± 0.2 z6F9/2 42 412.97 235.70 0.146 ± 0.006 0.141 0.769 ± 0.09 0.969 0.928 0.193 12
z6F7/2 42 290.75 236.39 0.826 ± 0.01 0.832 4.34 ± 0.5 5.72 5.31 0.561 12
z6P7/2 41 869.55 238.76 0.0137 ± 0.005 0.0133 0.072 ± 0.03 0.0916 0.106 1.210 42
Residual 0.0145
e6G7/2 1.8 ± 0.2 z6F7/2 42 473.69 235.37 0.171 ± 0.04 0.129 0.949 ± 0.2 0.832 1.39 0.200 21
z6F5/2 42 375.90 235.91 0.420 ± 0.08 0.382 2.33 ± 0.5 2.46 4.74 0.192 21
z4P5/2 37 743.27 264.87 0.0070 ± 0.003 0.144 0.039 ± 0.02 0.926 0.0554 1.484 51
Residual 0.345
e6G5/2 1.9 ± 0.2 z6F5/2 42 510.02 235.17 0.276 ± 0.01 0.274 1.45 ± 0.2 1.91 1.72 0.142 14
z6F3/2 42 443.55 235.54 0.692 ± 0.01 0.693 3.64 ± 0.4 4.82 4.42 0.259 11
Residual 0.032
e6G3/2 1.7 ± 0.3 z6F5/2 42 603.41 234.65 0.0281 ± 0.001 0.0267 0.165 ± 0.03 0.186 0.178 1.264 18
z6F3/2 42 536.96 235.02 0.343 ± 0.01 0.293 2.02 ± 0.3 2.04 1.93 0.174 15
z6F1/2 42 498.42 235.23 0.613 ± 0.01 0.671 3.60 ± 0.6 4.68 4.38 0.077 17
Residual 0.0092

Notes.

(a)

Complete description of transition: 3d6(5D)4p z6F, z6P, z4P3d6(5D)4d e6G. Transition energies are from Nave & Johansson (2013) where available or else from Kurucz (2013);

(b)

this work;

(e)

uncertainty in the experimental A values;

(f)

residual is the sum of all theoretical BFs for the unobserved lines from this level.

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