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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, z4P−3d6(5D)4d e6G. Transition energies are from Nave & Johansson (2013) where available or else from Kurucz (2013);
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