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Table B.3

Presentation of log(𝑔f) values for Si I based on the experimental branching fractions and the theoretical lifetimes of this work together with the wavelength, λ; wavenumber, σ; branching fraction, BF; transition probability, A; and corresponding theoretical log(𝑔f) values of this work.

Upper Level Lower Level λ (nm) σ (cm−1) BF BF Unc. % Aul (s−1) log(𝑔f) Experimental log(𝑔f) Calculated
3s23p4p 3D1 1199.157 8336.911 0.6373 2 1.05E+07 −0.168 ± 0.02 −0.175 ± 0.02
τ = 60.7 ns 1210.354 8259.789 0.3158 3 5.23E+06 −0.465 ± 0.02 −0.426 ± 0.02
1239.583 8065.021 0.0165 12 2.73E+05 −1.727 ± 0.06 −1.721 ± 0.02
1422.453 7028.190 0.0254 6 4.20E+05 −1.419 ± 0.03 −1.457 ± 0.02
Residual 0.0051
3s23p4p 3D2 1198.419 8342.038 0.8351 1 1.39E+07 0.176 ± 0.03 0.174 ± 0.02
τ = 60.0 ns 1227.069 8147.270 0.1582 7 2.63E+06 −0.526 ± 0.08 −0.472 ± 0.02
Residual 0.0068
3s23p4p 3P1 1066.097 9377.438 0.3680 3 8.79E+06 −0.347 ± 0.02 −0.340 ± 0.01
τ = 41.9 ns 1074.938 9300.316 0.4359 3 1.04E+07 −0.266 ± 0.01 −0.263 ± 0.01
1097.931 9105.548 0.1640 4 3.92E+06 −0.673 ± 0.02 −0.631 ± 0.01
1239.015 8068.717 0.0099 22 2.35E+05 −1.789 ± 0.11 −1.799 ± 0.02
2642.418 3784.413 0.0046 24 1.10E+05 −1.463 ± 0.12 −1.340 ± 0.10
2654.652 3766.972 0.0176 8 4.19E+05 −0.876 ± 0.04 −0.904 ± 0.09
Residual 0.00001
3s23p4p 3P2 1060.343 9428.332 0.1973 5 4.77E+06 −0.396 ± 0.02 −0.389 ± 0.01
τ = 41.4 ns 1082.709 9233.564 0.7798 1 1.88E+07 0.219 ± 0.01 0.231 ± 0.01
2586.138 3866.769 0.0161 7 3.89E+05 −0.710 ± 0.03 −0.608 ± 0.09
Residual 0.0069
3s23p4p 3S1 1037.126 9639.385 0.1439 6 3.10E+06 −0.824 ± 0.03 −0.786 ± 0.01
τ = 46. 4 ns 1058.514 9444.617 0.7915 2 1.70E+07 −0.066 ± 0.02 −0.042 ± 0.01
Residual 0.0646

Notes. Wavelength and wavenumber values are derived from the energy levels given in the NIST database (Kramida et al. 2022). For 2000 Å< λ< 20 000 Å, the wavelength is given in vacuum, otherwise in air. Uncertainties of calculated BF for unobserved residual branches were assumed to be 50%.

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