Table 8
Relative intensities of the brightest Fe xi lines in the soft X-rays.
i − j | Levels | Int | Int | Int | Int | gf | Aji(s-1) | λexp(Å) | λth(Å) | |
1.0 × 108 | 1.0 × 108 | 1.0 × 108 | 1.0 × 1012 | |||||||
DW4 | RM4 | RM4+DW6 | RM4 | |||||||
|
||||||||||
6–596 | 3s 3p53P2–3s 3p4 4s 3P2 | 1.8 × 10-2 | 1.8 × 10-2 | 1.8 × 10-2 | 7.9 × 10-3 | 0.46 | 7.7 × 1010 | 88.933∗ | 85.51 (−3.4) | |
6–454 | 3s 3p53P2–3s2 3p3 4p 3P2 | 1.3 × 10-2 | 1.4 × 10-2 | 1.4 × 10-2 | 6.0 × 10-3 | 8.3 × 10-2 | 1.1 × 1010 | 100.575∗ | 96.36 (−4.2) | |
1–291 | 3s2 3p43P2–3s2 3p3 4s 3D3 | 6.0 × 10-3 | 8.7 × 10-3 | 9.7 × 10-3 | 5.2 × 10-3 | 0.37(0.51) | 4.5(6.6) × 1010 | 86.772 | 84.52 (−2.3) | |
1–265 | 3s2 3p43P2–3s2 3p3 4s 3S1 | 3.7 × 10-3 | 5.3 × 10-3 | 5.8 × 10-3 | 3.2 × 10-3 | 0.39(0.50) | 1.1(1.4) × 1011 | 89.185 | 86.85 (−2.3) | |
42–454 | 3s2 3p3 3d 3D3–3s2 3p3 4p 3P2 | 5.1 × 10-3 | 5.1 × 10-3 | 5.2 × 10-3 | 2.3 × 10-3 | 5.8 × 10-2 | 4.1 × 109 | 138.21∗ | 132.77 (−5.4) | |
7–596 | 3s 3p53P1–3s 3p4 4s 3P2 | 4.4 × 10-3 | 4.5 × 10-3 | 4.5 × 10-3 | 1.9 × 10-3 | 0.12 | 1.9 × 1010 | 89.703∗ | 86.20 (−3.5) | |
7–454 | 3s 3p53P1–3s2 3p3 4p 3P2 | 4.1 × 10-3 | 4.2 × 10-3 | 4.2 × 10-3 | 1.8 × 10-3 | 2.6 × 10-2 | 3.3 × 109 | 101.559∗ | 97.25 (−4.3) | |
1–536 | 3s2 3p43P2–3s2 3p3 4d 3D3 | 3.1 × 10-3 | 3.9 × 10-3 | 5.0 × 10-3 | 2.0 × 10-3 | 0.73(0.98) | 1.3(1.8) × 1011 | 72.635 | 70.98 (−1.7) | |
38–454 | 3s2 3p3 3d 3P2–3s2 3p3 4p 3P2 | 3.8 × 10-3 | 3.9 × 10-3 | 3.9 × 10-3 | 1.7 × 10-3 | 4.1 × 10-2 | 3.0 × 109 | 133.95∗ | 128.40 (−5.5) | |
16–749 | 3s2 3p3 3d 3D3–3s2 3p3 4f 3F4 | 3.7 × 10-3 | 3.8 × 10-3 | 3.9 × 10-3 | 1.9 × 10-3 | 3.40 | 2.9 × 1011 | − | 89.77 | |
42–813 | 3s2 3p3 3d 3D3–3s2 3p3 4f 3F4 | 3.1 × 10-3 | 3.2 × 10-3 | 3.2 × 10-3 | 1.6 × 10-3 | 2.31 | 1.6 × 1011 | − | 99.64 | |
16–377 | 3s2 3p3 3d 3D3–3s2 3p3 4p 3P2 | 2.3 × 10-3 | 2.7 × 10-3 | 2.9 × 10-3 | 1.5 × 10-3 | 0.16 | 1.3 × 1010 | − | 119.93 | |
24–424 | 3s2 3p3 3d 3G5–3s2 3p3 4p 3F4 | 2.1 × 10-3 | 2.5 × 10-3 | 2.8 × 10-3 | 2.2 × 10-3 | 0.47 | 2.2 × 1010 | 123.490 | 120.03 (−3.5) | |
2–265 | 3s2 3p43P1–3s2 3p3 4s 3S1 | 1.7 × 10-3 | 2.4 × 10-3 | 2.6 × 10-3 | 1.5 × 10-3 | 0.18(0.23) | 4.8(6.3) × 1010 | 90.204 | 87.79 (−2.4) | |
1–289 | 3s2 3p43P2–3s2 3p3 4s 3D2 | 1.4 × 10-3 | 2.3 × 10-3 | 2.5 × 10-3 | 1.9 × 10-3 | 0.16(0.21) | 2.8(3.8) × 1010 | 87.025 | 84.71 (−2.3) | |
39–454 | 3s2 3p3 3d 3S1–3s2 3p3 4p 3P2 | 2.2 × 10-3 | 2.3 × 10-3 | 2.3 × 10-3 | 9.9 × 10-4 | 2.4 × 10-2 | 1.8 × 109 | 134.34∗ | 129.08 (−5.2) | |
30–460 | 3s2 3p3 3d 3F3–3s2 3p3 4p 3D2 | 2.0 × 10-3 | 2.1 × 10-3 | 2.2 × 10-3 | 1.5 × 10-3 | 0.20 | 1.7 × 1010 | 123.572 | 120.21 (−3.4) | |
1–42 | 3s2 3p43P2–3s2 3p3 3d 3D3 | 1.0 | 1 | 1 | 0.44 | 4.82 | 1.5 × 1011 | 180.401 | 176.36 (−4.0) |
Notes. The lines are displayed in decreasing order of intensity (photons) Int = NjAji/Ne relative to the strongest EUV line. The intensities were calculated at log Te [K] = 6.15. Columns 3, 4, 5 show the relative intensities calculated at log Ne [cm-3] = 8 with the DW4, RM4, and RM4+DW6 ion models. Column 6 shows the values at log Ne [cm-3] = 12 from the RM4 ion model. Columns 7, 8 show the gf and A values calculated in this work. The values in brackets are those calculated by Bhatia et al. (2002). The next column shows the experimental wavelengths. Values indicated with ∗ are from Del Zanna (2012), the others are from Fawcett et al. (1972). The last column shows the wavelengths corresponding to the target energies. Values in parenthesis give the corresponding wavelength difference with the experimental ones.
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