Table 4
Results of spectral fits for candidates with zero-duration T90.
| Source ID | Blackbody model | Power law model | ||||
|---|---|---|---|---|---|---|
| T | F0.5–7 keV | C-stat/d.o.f | Γ | F0.5–7 keV | C-stat/d.o.f | |
| (keV) | (erg s−1 cm−2) | (erg s−1 cm−2) | ||||
| XT 040916 | ![]() |
× 10−15
|
1.84/7 | ![]() |
× 10−15
|
0.69/7 |
| XT 111205 | ![]() |
× 10−15
|
1.39/4 | ![]() |
× 10−15
|
0.87/4 |
![]() |
× 10−14
|
2.07/4 | ![]() |
× 10−14
|
1.25/4 | |
| XT 150429 | ![]() |
× 10−15
|
3.06/3 | ![]() |
× 10−15
|
2.8/3 |
| XT 160625 | ![]() |
× 10−13
|
9.84/8 | − | − | − |
Notes. The photon index (Γ) of the power-law model could not be constrained for XT 160625. The second row for XT 111205 includes Galactic absorption fixed at NH = 4.43 × 1021 cm−2, and the corresponding fluxes are unabsorbed. All other results are for models without Galactic absorption. The NH of the other sources are in the range 0.76–1.75×1020 and have a negligible effect on the fits.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.
![Mathematical equation: $\[0.40_{-0.16}^{+0.38}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq5.png)
![Mathematical equation: $\[2.5_{-1.3}^{+2.5}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq6.png)
![Mathematical equation: $\[2.5_{-1.6}^{+1.9}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq7.png)
![Mathematical equation: $\[3.7_{-1.9}^{+4.3}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq8.png)
![Mathematical equation: $\[0.17_{-0.07}^{+0.27}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq9.png)
![Mathematical equation: $\[1.9_{-1.2}^{+3.0}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq10.png)
![Mathematical equation: $\[4.7_{-3.6}^{+3.9}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq11.png)
![Mathematical equation: $\[3.2_{-2.1}^{+13.9}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq12.png)
![Mathematical equation: $\[0.12_{-0.04}^{+0.11}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq13.png)
![Mathematical equation: $\[1.0_{-0.8}^{+1.4}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq14.png)
![Mathematical equation: $\[7.0_{-3.8}^{+3.0}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq15.png)
![Mathematical equation: $\[2.9_{-2.5}^{+14.4}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq16.png)
![Mathematical equation: $\[0.19_{-0.07}^{+0.24}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq17.png)
![Mathematical equation: $\[4.7_{-2.9}^{+7.4}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq18.png)
![Mathematical equation: $\[4.0_{-2.9}^{+2.8}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq19.png)
![Mathematical equation: $\[6.9_{-4.2}^{+9.8}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq20.png)
![Mathematical equation: $\[0.062_{-0.015}^{+0.021}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq21.png)
![Mathematical equation: $\[7.3_{-3.5}^{+5.5}\]$](/articles/aa/full_html/2026/04/aa57261-25/aa57261-25-eq22.png)