Table 5.
Comparison with measured centroid wavelengths (Å) for the Kα1, 2 and Kβ unresolved transition arrays in Fe X and Fe II.
| Method | Fe X |
Fe II (Solid-State Fe) |
||||
|---|---|---|---|---|---|---|
| Kα1 | Kα2 | Kα1 | Kα2 | Kβ | ||
| Experiment | 1.9388(5) | 1.9413(5) | 1.936041(3) | 1.939973(3) | 1.756604(4) | |
| MCDF/RATIP(μ = 0) | 1.9367 | 1.9405 | 1.9322 | 1.9363 | 1.7562 | |
| MCDF/RATIP(μ = 0.1) | 1.9369 | 1.9406 | 1.9324 | 1.9364 | 1.7564 | |
| MCDF/RATIP(μ = 0.25) | 1.9375 | 1.9412 | 1.9328 | 1.9368 | 1.7567 | |
Notes. The MCDF/RATIP wavelengths (as function of the plasma screening parameter μ (au.), Paper III and this work for, respectively, Fe X and Fe II) have been weighted with their corresponding transition probabilities. The experimental wavelengths are taken from the EBIT measurements of Decaux et al. (1995) for Fe X and from the solid-state measurements of Hölzer et al. (1997) for Fe II.
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