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Table 2

Comparison of experimental and theoretical weighted oscillator strength, log(gf), for S I.

Upper state Lower state λvac. ab initio Fine-tuned ZB2006a DH2008b Experiments
(Å) B C B C B C
3p3(2P)4s3P2oMathematical equation: $\[3 \mathrm{p}^{3}(^{2} \mathrm{P}) 4 \mathrm{s}~^{3} \mathrm{P}_{2}^\mathrm{o}\]$ 3p4(3P) 3P2 1295.653 −0.389 −0.397 −0.391 −0.398 −0.385 −0.412 −0.434 −0.362±0.030c
3p3(2P)4s3P1oMathematical equation: $\[3 \mathrm{p}^{3}(^{2} \mathrm{P}) 4 \mathrm{s}~^{3} \mathrm{P}_{1}^\mathrm{o}\]$ 3p4(3P) 3P2 1296.174 −0.874 −0.882 −0.878 −0.886 −0.870 −0.888 −0.907 −0.959±0.039c
3p3(2P)4s3P2oMathematical equation: $\[3 \mathrm{p}^{3}(^{2} \mathrm{P}) 4 \mathrm{s}~^{3} \mathrm{P}_{2}^\mathrm{o}\]$ 3p4(3P) 3P1 1302.336 −0.801 −0.809 −0.801 −0.808 −0.805 −0.827 −0.845 −0.815±0.043c
3p3(2P)4s3P1oMathematical equation: $\[3 \mathrm{p}^{3}(^{2} \mathrm{P}) 4 \mathrm{s}~^{3} \mathrm{P}_{1}^\mathrm{o}\]$ 3p4(3P) 3P1 1302.862 −1.078 −1.087 −1.078 −1.086 −1.074 −1.084 −1.103 −0.932±0.067c
3p3(2P)4s3P1oMathematical equation: $\[3 \mathrm{p}^{3}(^{2} \mathrm{P}) 4 \mathrm{s}~^{3} \mathrm{P}_{1}^\mathrm{o}\]$ 3p4(3P) 3P0 1305.883 −0.910 −0.919 −0.910 −0.917 −0.914 −0.921 −0.939 −0.824±0.038c
3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 3p4(3P) 3P2 1807.312 −0.367 −0.374 −0.370 −0.379 −0.371 −0.369 −0.394 −0.319±0.032c
3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 3p4(3P) 3P1 1820.342 −0.597 −0.605 −0.600 −0.610 −0.601 −0.599 −0.624 −0.593±0.056c
3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 3p4(3P) 3P0 1826.245 −1.077 −1.084 −1.080 −1.089 −1.080 −1.078 −1.103 −1.252±0.085c

Abundance diagnostic S I lines

3p3(4S)5p 5P3 3p3(4S)4s5S2oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{5} \mathrm{S}_{2}^\mathrm{o}\]$ 4695.422 −1.667 −1.690 −1.675 −1.686 −1.716 −1.599 −1.607
3p3(4S)5p 5P2 3p3(4S)4s5S2oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{5} \mathrm{S}_{2}^\mathrm{o}\]$ 4696.753 −1.825 −1.849 −1.833 −1.845 −1.873 −1.753 −1.757
3p3(4S)5d5D2oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 5 \mathrm{d}~{ }^{5} \mathrm{D}_{2}^\mathrm{o}\]$ 3p3(4S)4p 5P3 6758.611 −1.858 −1.896 −1.857 −1.869 −1.784
3p3(4S)5d5D3oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 5 \mathrm{d}~{ }^{5} \mathrm{D}_{3}^{\mathrm{o}}\]$ 3p3(4S)4p 5P3 6758.886 −1.014 −1.051 −1.012 −1.024 −0.940
3p3(4S)5d5D4oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 5 \mathrm{d}~{ }^{5} \mathrm{D}_{4}^\mathrm{o}\]$ 3p3(4S)4p 5P3 6759.043 −0.428 −0.465 −0.427 −0.438 −0.353
3p3(4S)4d5D0oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 4 \mathrm{d}~^{5} \mathrm{D}_{0}^\mathrm{o}\]$ 3p3(4S)4p 5P1 8672.585 −0.911 −0.962 −0.918 −0.932 −0.908 −0.826 −0.873
3p3(4S)4d5D4oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 4 \mathrm{d}~^{5} \mathrm{D}_{4}^\mathrm{o}\]$ 3p3(4S)4p 5P3 8697.023 +0.047 −0.004 +0.040 +0.027 +0.052 +0.186 +0.182
3p3(4S)4p 3P2 3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 10458.308 0.259 +0.273 +0.259 +0.262 +0.256 +0.270 +0.274 +0.250±0.009d
3p3(4S)4p 3P0 3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 10459.618 −0.440 −0.426 −0.440 −0.436 −0.444 −0.429 −0.426 −0.447±0.011d
3p3(4S)4p 3P1 3p3(4S)4s3S1oMathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 4 \mathrm{s}~^{3} \mathrm{S}_{1}^\mathrm{o}\]$ 10462.267 +0.037 +0.051 +0.037 +0.041 +0.035 +0.048 +0.052 +0.030±0.010d

Notes. B: Babushkin gauges. C: Coulomb gauges. The vacuum wavelengths are used in the table. (a)Zatsarinny & Bartschat (2006). (b)Deb & Hibbert (2008). (c)Beam-foil technique by Beideck et al. (1994). (d)Laser spectroscopy by Zerne et al. (1997).

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