Table 1
Relative intensities of the brightest soft X-ray lines in Fe xv.
i–j | Levels | Int | Int | gf | Aji (s-1) | λexp (Å) | λth (Å) | New | |||
1.0 × 108 | 1.0 × 1019 | ||||||||||
|
|||||||||||
5–37 | 3s 3p 1P1–3s 4s 1S0 | 1.0 | 5.1 × 10-2 | 0.16 | 2.2 × 1011 | 69.66 (? CW73) | 69.93 (0.3) | 69.661 (K97) | |||
14–53 | 3s 3d 1D2–3s 4f 1F3 | 0.36 | 2.4 × 10-2 | 3.45 | 6.0 × 1011 | 73.50 (CW73) | 73.82 (0.3) | ||||
5–45 | 3s 3p 1P1–3s 4d 1D2 | 0.28 | 1.8 × 10-2 | 0.64 | 2.4 × 1011 | 59.404 (F72) | 59.63 (0.2) | ||||
1–41 | 3s21S0–3s 4p 1P1 | 0.20 | 1.4 × 10-2 | 0.29 | 2.3 × 1011 | 52.911 (E36) | 52.96 (0.1) | ||||
7–53 | 3p21D2–3s 4f 1F3 | 0.12 | 8.1 × 10-3 | 0.89 | 2.1 × 1011 | 63.96 (? CW73) | 63.95 (–0.0) | 63.961 (K97) | |||
5–93 | 3s 3p 1P1–3s 5s 1S0 | 7.6 × 10-2 | 3.9 × 10-3 | 4.5 × 10-2 | 1.4 × 1011 | – | 46.28 | ? 46.30 (bl) | |||
13–52 | 3s 3d 3D3–3s 4f 3F4 | 6.2 × 10-2 | 8.0 × 10-2 | 5.81 | 8.7 × 1011 | 70.054 (E36) | 70.17 (0.1) | ||||
5–113 | 3s 3p 1P1–3s 5d 1D2 | 4.6 × 10-2 | 3.0 × 10-3 | 0.27 | 1.8 × 1011 | – | 43.78 | ? 43.75 (bl) | |||
12–51 | 3s 3d 3D2–3s 4f 3F3 | 4.2 × 10-2 | 5.5 × 10-2 | 4.01 | 7.8 × 1011 | 69.987 (E36) | 70.11 (0.1) | ||||
11–50 | 3s 3d 3D1–3s 4f 3F2 | 3.3 × 10-2 | 3.7 × 10-2 | 2.70 | 7.3 × 1011 | 69.945 (E36) | 70.07 (0.1) | ||||
4–44 | 3s 3p 3P2–3s 4d 3D3 | 3.2 × 10-2 | 4.3 × 10-2 | 1.43 | 4.3 × 1011 | 56.200 (E36) | 56.22 (0.0) | ||||
7–41 | 3p21D2–3s 4p 1P1 | 3.1 × 10-2 | 2.2 × 10-3 | 9.3 × 10-2 | 3.6 × 1010 | 75.167 (E36) | 75.31 (0.1) | ||||
14–117 | 3s 3d 1D2–3s 5f 1F3 | 2.9 × 10-2 | 2.2 × 10-3 | 0.60 | 2.1 × 1011 | – | 52.35 | ? 52.36 | |||
13–40 | 3s 3d 3D3–3s 4p 3P2 | 2.8 × 10-2 | 8.0 × 10-2 | 0.30 | 5.7 × 1010 | – | 82.98 | ? 82.750 (K97) | |||
1–39 | 3s21S0–3s 4p 3P1 | 2.6 × 10-2 | 3.4 × 10-2 | 0.12 | 9.2 × 1010 | – | 53.17 | ? 53.11 (bl) |
Notes. The relative line intensities (photons) Int = NjAji/Ne were calculated at log Ne [cm-3] = 8,19 and log Te [K] = 6.3. The lines are ordered with decreasing intensity. The oscillator strengths and transition probabilities are shown. The last three columns show the experimental wavelengths λexp(Å), when known, the target wavelengths λth(Å), with their difference in parenthesis, and finally the new wavelengths proposed here. We also add next to the experimental wavelength the reference (E36: Edlén 1936a; F72: Fawcett et al. 1972; CW73: Cowan & Widing 1973). A question mark indicates a tentative identification.
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