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Table 3

Emission lines selected for Doppler shift measurements.

Indexa λ b Elem. T max Flux contrib.c Line

(Å) (MK) Accr. Cor. subsetd

1a 6.1804 Si xiv 15.8 0.00 1.00 h
1b 6.1858 Si xiv 15.8 0.00 1.00 h
2 6.6479 Si xiii 10.0 0.01 0.99 h
3 6.7403 Si xiii 10.0 0.02 0.98 h
4a 8.4192 Mg xii 10.0 0.00 1.00 h
4b 8.4246 Mg xii 10.0 0.00 1.00 h
5 9.1687 Mg xi 6.3 0.31 0.69 h
6a 9.7080 Ne x 6.3 0.07 0.93 h
6b 9.7085 Ne x 6.3 0.07 0.93 h
7a 10.2385 Ne x 6.3 0.09 0.91 h
7b 10.2396 Ne x 6.3 0.09 0.91 h
8 13.6990 Ne ix 4.0 0.96 0.04 c
9 15.0140 Fe xvii 5.0 0.73 0.27 h
10a 16.0055 O viii 3.2 0.92 0.08 c
10b 16.0067 O viii 3.2 0.92 0.08 c
11 16.7800 Fe xvii 5.0 0.77 0.23 h
12 17.0510 Fe xvii 5.0 0.76 0.24 h
13 17.0960 Fe xvii 5.0 0.78 0.22 h
14a 18.9671 O viii 3.2 0.94 0.06 c
14b 18.9725 O viii 3.2 0.94 0.06 c
15 21.6015 O vii 2.0 1.00 0.00 c

Notes.

(a)

Lines indicated with the same index number, but different letters, are the two components of H-like resonance doublets.

(b)

APED predicted wavelengths.

(c)

Fractional contributions to individual line fluxes due to accretion and corona components, on the basis of the model C obtained by Brickhouse et al. (2010).

(d)

“c” and “h” indicate whether the line has been included in the cool or hot line subsample.

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