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Table A.1

Shock structures in the winds of the central stars of NGC 2392, IC 4593, IC 418, and NGC 6826, determined from fits of the calculated O vi lines to the FUSE observations.

NGC 2392 IC 4593 IC 418 NGC 6826

[LX] = −6.0* [LX] = −6.3* [LX] = −6.6 [LX] = −6.4

r/R Ts(r) r/R Ts(r) r/R Ts(r) r/R Ts(r)

1.20 0.26 1.11 0.05 1.12 0.04 1.09 0.05
1.31 0.35 1.23 0.12 1.32 0.07 1.42 0.14
1.53 0.50 1.38 0.23 1.57 0.13 1.81 0.29
1.75 0.61 1.75 0.51 1.83 0.19 2.20 0.42
2.18 0.76 2.11 0.76 2.38 0.29 3.42 0.68
2.67 0.87 4.18 1.55 3.07 0.38 5.75 0.92
4.29 1.06 5.39 1.77 4.73 0.52 9.34 1.06
8.85 1.23 11.3 2.21 9.27 0.65 18.1 1.19
27.1 1.33 29.1 2.47 27.4 0.76 41.5 1.26
51.4 1.35 52.7 2.55 51.6 0.78 53.2 1.28
75.7 1.36 76.4 2.58 75.8 0.79 76.6 1.29
100. 1.37 100. 2.60 100. 0.80 100. 1.30

Notes. The table lists characteristic values of the radial distributions of the maximum local shock temperatures Ts(r) (in units of 106 K) and the integrated relative X-ray luminosities LX/Lbol (where [LX] = log (LX/Lbol)) emitted by the shock cooling zones embedded in the winds.

(*)

We note that Herald & Bianchi (2011), based on a less elaborate treatment of shock structures, obtained integrated relative X-ray luminosities LX/Lbol which for the central stars of NGC 2392 ([LX] = −4.4) and IC 4593 ([LX] = −4.8) are almost a factor of 100 higher than our values. (Their parameters have also been determined from fits of the calculated O vi lines to the observations.) However, as pointed out by the authors themselves, their results will certainly be revised by the application of a more sophisticated treatment of X-rays, which they state is an ongoing development.

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