Table E.1.
Wavelengths, excitation potentials, and oscillator strengths of atomic lines used in this study, sorted by element, with NIST data quality flags.
| Element / λ | Exc. Potential | Osc. Str. | NIST Flag | Element / λ | Exc. Potential | Osc. Str. | NIST Flag |
|---|---|---|---|---|---|---|---|
| Å | eV | Å | eV | ||||
| Mg (12) | Fe (26) | ||||||
| 5528.405 (I) | 4.343 | -0.620 | B+ | 5191.455 (I) | 3.038 | -0.551 | B |
| 5711.088 (I) | 4.343 | -1.830 | B+ | 5194.942 (I) | 1.557 | -2.090 | A |
| 5198.711 (I) | 2.223 | -2.135 | B | ||||
| Sr (38) | 5215.179 (I) | 3.266 | -0.871 | B | |||
| 4077.714 (II) | 0.000 | 0.150 | AA | 5229.845 (I) | 3.283 | -0.967 | |
| 4215.524 (II) | 0.000 | -0.170 | AA | 5232.940 (I) | 2.940 | -0.058 | B+ |
| 4607.331 (I) | 0.000 | 0.280 | AA | 5242.491 (I) | 3.634 | -0.967 | B |
| 4722.278 (I) | 1.797 | -0.130 | B+ | 5247.050 (I) | 0.087 | -4.946 | A |
| 4962.263 (I) | 1.846 | 0.250 | AA | 5169.033 (II) | 2.891 | -1.250 | C |
| 5256.899 (I) | 2.270 | 0.390 | B+ | 5197.577 (II) | 3.230 | -2.348 | C |
| 5234.625 (II) | 3.221 | -2.279 | |||||
| Zr (40) | |||||||
| 4359.74 (II) | 1.236 | -0.5100 | Y (39) | ||||
| 4496.97 (II) | 0.713 | -0.8900 | 4374.933 (II) | 0.408 | 0.160 | A | |
| 4687.80 (I) | 0.730 | 0.5500 | 4689.767 (I) | 2.002 | -0.170 | A | |
| 4739.48 (I) | 0.650 | 0.2300 | 4883.682 (II) | 1.083 | 0.070 | B | |
| 6127.44 (I) | 0.154 | -1.0600 | 5205.722 (II) | 1.032 | -0.340 | B+ | |
| 5503.464 (I) | 1.965 | 0.370 | A | ||||
| Ba (56) | 5509.894 (II) | 0.992 | -1.010 | B+ | |||
| 4554.033 (II) | 0.000 | -0.562 | B (hfs) | ||||
| 5853.675 (II) | 0.604 | -1.914 | B (hfs) | Mo (42) | |||
| 6141.713 (II) | 0.704 | -1.158 | B (hfs) | 5506.493 (I) | 1.334 | 0.060 | A+ |
| 6496.898 (II) | 0.604 | -1.111 | B (hfs) | 5533.031 (I) | 1.334 | -0.070 | A+ |
| 5570.444 (I) | 1.334 | -0.340 | A | ||||
| Ce (58) | |||||||
| 4628.161 (II) | 0.516 | 0.140 | B+ | La (57) | |||
| 5274.229 (II) | 1.044 | 0.130 | B+ | 4920.98 (II) | 0.126 | -0.580 | B+ |
| 5330.556 (II) | 0.869 | -0.400 | B | 4921.79 (II) | 0.244 | -0.450 | B+ |
| 5353.524 (II) | 0.879 | 0.090 | B+ | 5114.56 (II) | 0.235 | -1.999 | B+ (hfs) |
| 5122.99 (II) | 0.321 | -2.212 | B+ (hfs) | ||||
| Eu (63) | 5301.98 (II) | 0.403 | -2.300 | B+ (hfs) | |||
| 4129.70 (II) | 0.000 | 0.109 | (hfs) | 5805.78 (II) | 0.126 | -2.940 | B (hfs) |
| 4594.03 (I) | 0.000 | 0.680 | B+ | ||||
| 5577.14 (I) | 1.667 | 0.000 | B+ | Nd (60) | |||
| 6645.11 (II) | 1.379 | -0.517 | (hfs) | 4232.378 (II) | - - | - - | B |
| 4247.367 (II) | 0.000 | -0.210 | B+ | ||||
| Pb (82) | 5212.365 (II) | 0.204 | -0.960 | B+ | |||
| 4057.807 (I) | 1.319 | -0.170 | C+ | 5361.474 (II) | 0.680 | -0.370 |
Notes. Oscillator strengths for lines that include hyper-fine splitting (hfs) are the total log(gf) from all contributing components. The ionization state is identified by the roman numerals in the parentheses, where (I) is the ground state, and (II) is the first ionized state.
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