Table 7
XRT spectroscopy of the three SFXTs in the new monitoring sample (2011−2013 data set).
Name | Spectrum | Mean rate | NH | Γ | k TBB | RBB | Fluxa | Luminosityb | ![]() |
F-testc | Fig. | |||
(2−10 keV) | (2−10 keV) | p | ||||||||||||
(c s-1) | (1022 cm-2) | (eV) | (km) | (10-12) | (1035) | |||||||||
|
||||||||||||||
J08408 | low | 0.05 |
![]() |
![]() |
− | − | 5.6 | 0.078 | 1.7/57 | |||||
low | 0.05 |
![]() |
![]() |
![]() |
![]() |
5.5 | 0.076 | 1.18/55 | 4.4 × 10-5 | 2 | ||||
very lowd | 0.009 |
![]() |
![]() |
− | − | 0.09 | 0.001 | 1.47/194 | ||||||
very lowd | 0.009 |
![]() |
![]() |
![]() |
![]() |
0.19 | 0.003 | 1.18/192 | 6.9 × 10-10 | 2 | ||||
|
||||||||||||||
J16328 | low | 0.08 |
![]() |
![]() |
− | − | 16 | 1.4 | 0.84/110 | 3 | ||||
very lowe | 0.007 |
![]() |
![]() |
− | − | 1.1 | 0.06 | 1.66/242 | ||||||
very low | 0.007 |
![]() |
![]() |
![]() |
![]() |
0.95 | 0.06 | 1.12/240 | 3.1 × 10-21 | 3 | ||||
|
||||||||||||||
J16465 | high | >0.25 |
![]() |
![]() |
− | − | 43 | 9.7 | 1.02/108 | |||||
high | >0.25 |
![]() |
![]() |
![]() |
![]() |
43 | 9.8 | 0.93/106 | 7.5 × 10-3 | 4 | ||||
medium | [0.15−0.25[ |
![]() |
![]() |
− | − | 23 | 5.0 | 1.18/102 | ||||||
medium | [0.15−0.25[ |
![]() |
![]() |
![]() |
![]() |
22 | 5.3 | 1.04/100 | 1.8 × 10-3 | 4 | ||||
low | <0.15 |
![]() |
![]() |
− | − | 8.0 | 1.8 | 1.32/120 | ||||||
low | <0.15 |
![]() |
![]() |
![]() |
![]() |
7.9 | 1.8 | 1.17/118 | 8.1 × 10-4 | 4 |
Notes. Uncertainties are given at a 90% confidence level for one interesting parameter.
Average 2−10 keV luminosities in units of 1035 erg s-1 calculated by adopting the distances of Table 6.
Fit performed with the column density constrained to be higher than the one derived from optical extinction towards the optical counterpart (see Sect 4.3).
Fit performed with the column density constrained to be higher than the Galactic value (see Sect 4.3).
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