Table 4.
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Teff for 1RXS J023238.8−371812 allowing different log g, corresponding to different white dwarf masses. These results have been obtained fitting the data including the emission lines as Gaussian profiles, and using three different models for the second component.

Teff (K)Teff (K)Teff (K)
Secondlog g = 8.00log g = 8.35log g = 8.60
componentMWD = 0.6 M⊙MWD = 0.8 M⊙MWD = 1.0 M⊙
Blackbody13 016 ± 2813 540 ± 3413 938 ± 37
Power law13 045 ± 2913 573 ± 3413 972 ± 37
Constant12 949 ± 2313 466 ± 2613 848 ± 28
Average13 003 ± 4913 526 ± 5513 919 ± 64
Teff (K)Teff (K)Teff (K)
Secondlog g = 8.00log g = 8.35log g = 8.60
componentMWD = 0.6 M⊙MWD = 0.8 M⊙MWD = 1.0 M⊙
Blackbody13 016 ± 2813 540 ± 3413 938 ± 37
Power law13 045 ± 2913 573 ± 3413 972 ± 37
Constant12 949 ± 2313 466 ± 2613 848 ± 28
Average13 003 ± 4913 526 ± 5513 919 ± 64
Table 4.
Open in new tab

Teff for 1RXS J023238.8−371812 allowing different log g, corresponding to different white dwarf masses. These results have been obtained fitting the data including the emission lines as Gaussian profiles, and using three different models for the second component.

Teff (K)Teff (K)Teff (K)
Secondlog g = 8.00log g = 8.35log g = 8.60
componentMWD = 0.6 M⊙MWD = 0.8 M⊙MWD = 1.0 M⊙
Blackbody13 016 ± 2813 540 ± 3413 938 ± 37
Power law13 045 ± 2913 573 ± 3413 972 ± 37
Constant12 949 ± 2313 466 ± 2613 848 ± 28
Average13 003 ± 4913 526 ± 5513 919 ± 64
Teff (K)Teff (K)Teff (K)
Secondlog g = 8.00log g = 8.35log g = 8.60
componentMWD = 0.6 M⊙MWD = 0.8 M⊙MWD = 1.0 M⊙
Blackbody13 016 ± 2813 540 ± 3413 938 ± 37
Power law13 045 ± 2913 573 ± 3413 972 ± 37
Constant12 949 ± 2313 466 ± 2613 848 ± 28
Average13 003 ± 4913 526 ± 5513 919 ± 64
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