Table 3
Strongest contributions to the dominant absorption troughs for components C, D, and E.
Comp | Ion and dominant | λ a | E b | W 1 c | W 2 d | ΔWe |
transition/blend | (Å) | (keV) | (eV) | (eV) | (eV) | |
|
||||||
C | O vii 1s–3p...7p | 18.63 | 0.663 | 0.99 | 0.75 | −0.24 |
C | Fe ix | 16.54 | 0.721 | 0.17 | 0.06 | −0.11 |
C | Fe x | 16.36 | 0.729 | 0.52 | 0.23 | −0.29 |
C | Fe xi | 16.18 | 0.738 | 0.84 | 0.43 | −0.41 |
C | Fe xii | 16.03 | 0.745 | 0.69 | 0.53 | −0.16 |
C | Fe xiii | 15.89 | 0.756 | 0.60 | 0.55 | −0.05 |
C | Fe xiv | 15.63 | 0.767 | 0.27 | 0.32 | +0.05 |
C | O viii 1s–3p,4p,5p | 16.01 | 0.768 | 1.58 | 1.50 | −0.06 |
C | Fe xv | 15.36 | 0.777 | 0.16 | 0.23 | +0.07 |
C | Fe xvi | 15.26 | 0.786 | 0.13 | 0.22 | +0.09 |
C | Fe xvii 2p–3s,3d | 15.01 | 0.789 | 0.57 | 1.07 | +0.50 |
|
||||||
D | O viii 1s–3p,4p,5p | 16.01 | 0.766 | 0.41 | 0.26 | −0.15 |
D | Fe xvii | 15.01 | 0.794 | 0.47 | 0.25 | −0.22 |
D | Fe xviii | 14.20 | 0.836 | 1.27 | 0.89 | −0.38 |
D | Fe xix | 13.52 | 0.881 | 1.54 | 1.41 | −0.13 |
D | Ne ix 1s–2p | 13.45 | 0.891 | 0.20 | 0.11 | −0.09 |
D | Fe xx 2p-3d | 12.84 | 0.929 | 0.65 | 0.86 | +0.21 |
|
||||||
E | Fe xx 2p–3d | 12.84 | 0.935 | 0.07 | 0.00 | −0.07 |
E | Ne x 1s–2p | 12.13 | 0.987 | 0.66 | 0.46 | −0.16 |
E | Fe xxi 2p–3d | 12.29 | 0.987 | 0.40 | 0.07 | −0.33 |
E | Fe xxii 2s–3p | 11.71 | 1.038 | 0.84 | 0.19 | −0.65 |
E | Fe xxiii 2s–3p | 10.98 | 1.092 | 1.01 | 0.47 | −0.54 |
E | Fe xxiv 2s–3p | 10.62 | 1.127 | 1.06 | 0.76 | −0.30 |
Notes.
Laboratory wavelength of the strongest individual spectral line of the ion that contributes to the blend.
Predicted energy of the line centroid of all lines from the given ion that contribute to the blend, in the observer’s frame (thus accounting for cosmological redshift).
Total equivalent width of all the lines of the ion contributing to the blend, for the parameters of the time-averaged spectrum (see Table 1).
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