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Table 4

Absorption line detections for Chandra non-dip spectrum.

Ion Transitiona E lab E obs Shift Width Fluxb EQWc
eV eV km s-1 eV (10-4) eV

Mg xii 1s − 2p 1472.3 1474.0 350 1.5 ± 1.5 6.5 ± 3 0.8 ± 0.3
Al xiii 1s − 2p 1728.6 1727.2 ± 2.6 240 ± 450 1.6 5 ± 2.5 0.6 ± 0.3
Mg xii 1s − 3p 1744.7 1745.4 ± 1.2 140 ± 200 1.0 6.0 ± 2.0 0.9 ± 0.3
XAFS 1847.7 ± 0.7 2.2 ± 0.8 11.6 ± 2.4 2.0 ± 0.4
XAFS 1863.7 ± 1.0 2.4 ± 1.4 9 ± 2 1.8 ± 0.3
Si xiv 1s − 2p 2005.5 2007.4 ± 0.4 280 ± 60 2.6 ± 0.6 14.4 2.7 ± 0.5
S xvi 1s − 2p 2621.7 2623.4 200 0+4 6.0 ± 1.4 1.2 ± 0.4
Ca xx 1s − 2p 4105.0 4118 ± 8 950 ± 600 13 ± 10 6.0 ± 2.5 2.4 ± 1.1
Fe xxv 1s2 − 1s2p 6700.4 6706 ± 5 250 ± 220 8 ± 8 9.6 ± 2 12 ± 3
Fe xxvi 1s − 2p 6966.2 6978 ± 3 500 ± 130 20.4 ± 5 25.2 ± 3 36 ± 5
Fe xxvi 1s − 3p 8250.2 8273 ± 20 840 ± 730 25 ± 25 10 ± 5 22 ± 12

Notes. An absorbed (tbvarabs) continuum model of thermal disk emission and thermal Comptonization is used.

(a)

Rest-frame energies from Verner et al. (1996).

(b)

Total area of the Gaussian (absolute value), in units of photons/cm-2/s.

(c)

Line equivalent width.

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