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Table 4

List of the brightest Fe ix lines.

ij Levels Int Int Int gf Aji(s-1) λexp(Å) λth(Å)
Present S02 S02+B12

1–13 3s2 3p61S0–3s2 3p5 3d 1P1 1.0 1.0 1.0 3.17 2.3 × 1011 171.073 166.23 (–4.8)
1–4 3s2 3p61S0–3s2 3p5 3d 3P2 0.23 0.20 0.21 87. 241.739 238.01 (–3.7)
1–3 3s2 3p61S0–3s2 3p5 3d 3P1 8.4 × 10-2 7.2 × 10-2 7.5 × 10-2 3.2 × 10-4 1.2 × 107 244.909 241.25 (–3.7)
5–96 3s2 3p5 3d 3F4–3s2 3p4 3d23G5 4.6 × 10-2 4.6 × 10-2 4.9 × 10-2 5.56 8.9 × 1010 188.493 176.15 (–12.3)
1–10 3s2 3p61S0–3s2 3p5 3d 3D1 3.9 × 10-2 2.8 × 10-2 3.4 × 10-2 5.2 × 10-3 2.4 × 108 217.101 212.84 (–4.3)
5–110 3s2 3p5 3d 3F4–3s2 3p4 3d23D3 3.2 × 10-2 3.2 × 10-2 3.4 × 10-2 6.13 1.7 × 1011 176.945 165.85 (–11.1) R (bl)
1–7 3s2 3p61S0–3s2 3p5 3d 3F2 3.1 × 10-2 2.2 × 10-2 2.2 × 10-2 1.9 230.511 226.12 (–4.4)
1–9 3s2 3p61S0–3s2 3p5 3d 1D2 3.0 × 10-2 2.5 × 10-2 2.6 × 10-2 32. 218.937 214.36 (–4.6)
5–118 3s2 3p5 3d 3F4–3s2 3p4 3d23F4 2.8 × 10-2 2.7 × 10-2 3.0 × 10-2 6.99 1.7 × 1011 168.08 157.83 (–10.2) TN
13–148 3s2 3p5 3d 1P1–3s2 3p5 4p 1S0 2.1 × 10-2 2.7 × 10-2 3.1 × 10-2 0.19 3.3 × 1010 197.854 179.84 (–18.0)
6–95 3s2 3p5 3d 3F3–3s2 3p4 3d23G4 2.1 × 10-2 2.3 × 10-2 2.3 × 10-2 4.15 8.0 × 1010 189.935 177.34 (–12.6)
6–111 3s2 3p5 3d 3F3–3s2 3p4 3d23D2 1.2 × 10-2 1.1 × 10-2 1.2 × 10-2 4.17 1.6 × 1011 177.592 166.49 (–11.1) R
6–121 3s2 3p5 3d 3F3–3s2 3p4 3d23F3 9.5 × 10-3 8.2 × 10-3 9.2 × 10-3 4.71 1.5 × 1011 157.76
5–29 3s2 3p5 3d 3F4–3s2 3p4 3d25G6 6.7 × 10-3 4.0 × 10-3 4.7 × 10-3 22. 234.94
13–166 3s2 3p5 3d 1P1–3s2 3p4 3d21D2 6.7 × 10-3 2.7 × 10-3 5.99 2.3 × 1011 181.10 171.15 (–10) TN
5–40 3s2 3p5 3d 3F4–3s2 3p4 3d23G5 6.6 × 10-3 3.1 × 10-3 4.5 × 10-3 5.5 × 10-2 5.4 × 108 223.31
8–118 3s2 3p5 3d 3D3–3s2 3p4 3d23F4 5.7 × 10-3 6.6 × 10-3 6.5 × 10-3 1.59 3.5 × 1010 176.945 165.88 (–11.1) TN (bl)
5–24 3s2 3p5 3d 3F4–3s2 3p4 3d25F5 5.2 × 10-3 2.9 × 10-3 3.6 × 10-3 2.9 × 10-4 2.4 × 106 243.40
7–97 3s2 3p5 3d 3F2–3s2 3p4 3d23G3 5.2 × 10-3 5.3 × 10-3 5.6 × 10-3 2.36 5.7 × 1010 191.206 178.53 (–12.7)
4–85 3s2 3p5 3d 3P2–3s2 3p4 3d23D3 4.9 × 10-3 4.4 × 10-3 4.4 × 10-3 1.84 4.3 × 1010 194.784 182.41 (–12.4) TN (bl)
1–11 3s2 3p61S0–3s2 3p5 3d 3D2 4.7 × 10-3 1.6 × 10-2 1.8 × 10-2 5.8 216.162 211.77 (–4.4)
8–105 3s2 3p5 3d 3D3–3s2 3p4 3d23F4 4.2 × 10-3 2.7 × 10-3 2.2 × 10-3 1.41 2.6 × 1010 192.630 180.45 (–12.2) TN (bl)
1–101 3s2 3p61S0–3s2 3p5 4s 1P1 1.1 × 10-2 8.6 × 10-3 1.2 × 10-2 0.23 4.6 × 1010 103.566 98.65 (–4.9)
1–94 3s2 3p61S0–3s2 3p5 4s 3P1 6.2 × 10-3 4.8 × 10-3 6.1 × 10-2 0.10 1.9 × 1010 105.208 100.16 (–5.0)
5–301 3s2 3p5 3d 3F4–3s2 3p5 4f 3G5 5.8 × 10-3 5.9 × 10-3 5.41 2.4 × 1011 113.793 107.88 (–5.9)
13–256 3s2 3p5 3d 1P1–3s 3p6 4s 1S0 5.7 × 10-3 4.6 × 10-3 2.8 × 10-2 8.2 × 109 147.274 141.09 (–6.2) TN
13–353 3s2 3p5 3d 1P1–3s2 3p5 4f 1D2 3.6 × 10-3 2.5 × 10-3 2.46 1.8 × 1011 133.923 126.82 (–7.1)
1–207 3s2 3p61S0–3s2 3p5 4d 1P1 3.5 × 10-3 2.3 × 10-3 0.40 1.2 × 1011 83.457 79.98 (–3.5)
6–308 3s2 3p5 3d 3F3–3s2 3p5 4f 3G4 2.4 × 10-3 2.5 × 10-3 3.63 2.0 × 1011 114.024 108.05 (–6.0)
1–224 3s2 3p61S0–3s2 3p5 4d 3D1 2.0 × 10-3 1.8 × 10-3 0.12 3.9 × 1010 82.430 79.07 (–3.4)
10–335 3s2 3p5 3d 3D1–3s2 3p5 4f 3F2 1.3 × 10-3 1.4 × 10-3 1.49 1.4 × 1011 116.803 110.39 (–6.4)
5–775 3s2 3p5 3d 3F4–3s2 3p5 5f 3G5 1.2 × 10-3 1.5 × 10-3 1.62 1.1 × 1011 91.980? 87.92 (–4.1)
13–545 3s2 3p5 3d 1P1–3s2 3p5 5p 1S0 1.2 × 10-3 6.9 × 10-4 9.9 × 10-3 4.5 × 109 113.15
101–148 3s2 3p5 4s 1P1–3s2 3p5 4p 1S0 2.3 × 10-3 1.4 × 10-3 1.4 × 10-3 0.29 3.5 × 109 803.98 694.59 (–109.4)
94–148 3s2 3p5 4s 3P1–3s2 3p5 4p 1S0 7.8 × 10-4 4.6 × 10-4 4.7 × 10-4 7.7 × 10-2 1.2 × 109 717.09 628.01 (–89.1)
5–12 3s2 3p5 3d 3F4–3s2 3p5 3d 1F3 8.1 × 10-2 7.5 × 10-2 7.8 × 10-2 84. 2498.84 2433.32 (–65.5)
5–6 3s2 3p5 3d 3F4–3s2 3p5 3d 3F3 7.3 × 10-2 7.3 × 10-2 7.2 × 10-2 1.1 28 562.50 29 165.41 (602.9)
4–8 3s2 3p5 3d 3P2–3s2 3p5 3d 3D3 6.4 × 10-2 6.1 × 10-2 6.3 × 10-2 14. 2384.19 2226.95 (–157.2)
6–7 3s2 3p5 3d 3F3–3s2 3p5 3d 3F2 5.0 × 10-2 5.2 × 10-2 5.3 × 10-2 3.0 22 183.25 22 158.82 (–24.4)
4–11 3s2 3p5 3d 3P2–3s2 3p5 3d 3D2 4.7 × 10-2 3.2 × 10-2 3.3 × 10-2 58. 2043.01 1920.65 (–122.4)
6–8 3s2 3p5 3d 3F3–3s2 3p5 3d 3D3 3.9 × 10-2 3.5 × 10-2 3.8 × 10-2 8.5 3802.10 3659.44 (–142.7)
6–9 3s2 3p5 3d 3F3–3s2 3p5 3d 1D2 2.3 × 10-2 2.1 × 10-2 2.4 × 10-2 25. 3644.08 3472.95 (–171.1)
7–9 3s2 3p5 3d 3F2–3s2 3p5 3d 1D2 1.7 × 10-2 1.5 × 10-2 1.7 × 10-2 19. 4360.36 4118.42 (–241.9)
7–12 3s2 3p5 3d 3F2–3s2 3p5 3d 1F3 1.6 × 10-2 1.5 × 10-2 1.6 × 10-2 16. 3124.06 3016.18 (–107.9)
7–8 3s2 3p5 3d 3F2–3s2 3p5 3d 3D3 1.2 × 10-2 1.1 × 10-2 1.2 × 10-2 2.6 4588.55 4383.33 (–205.2)

Notes. Columns 3–5 show the intensities (photons) of the strongest lines, relative to the resonance transition at 171 Å. The intensities were calculated at log Te [K] = 5.85, the temperature of peak ion abundance in ionization equilibrium, and at log Ne [cm-3] = 8. Column 3 shows the present values, while Cols. 4, 5 those with the previous R-matrix calculation (Storey et al. 2002, S02) and the combined R-matrix + DW data (O’Dwyer et al. 2012), S02+B12. Columns 6, 7 show the gf and A values calculated in this work. The last two columns show the wavelengths corresponding to the experimental and target energies. Values in parenthesis list the corresponding wavelength difference. TN is a new tentative identification. R indicates a revised wavelength and bl indicates that the line is blended.

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