Table 2
Journal of the X-ray observations.
| XID | ObsID (exp. time) | HJD | φ | Count rates (cts s-1) | |
| 0.5–1.5 keV | 1.5–10.0 keV | ||||
|
|
|||||
| X-1 | 0500030101 (47.6 ks) | 2 454 531.604 | 0.65 | 1.707 ± 0.007 | 0.927 ± 0.005 |
| X-2 | 0790180601 (8.0 ks) | 2 457 480.796 | 0.04 | 0.131 ± 0.005 | 0.054 ± 0.004 |
| S-2 | 00034304002 (0.7 ks) | 2 457 428.242 | 0.52 | 0.0743 ± 0.0145 | 0.0395 ± 0.0100 |
| S-3 | 00034304003 (3.2 ks) | 2 457 429.903 | 0.57 | 0.0592 ± 0.0050 | 0.0403 ± 0.0040 |
| S-4 | 00034304004 (3.4 ks) | 2 457 433.340 | 0.67 | 0.0727 ± 0.0052 | 0.0508 ± 0.0043 |
| S-5 | 00034304005 (2.3 ks) | 2 457 436.002 | 0.75 | 0.0674 ± 0.0059 | 0.0467 ± 0.0049 |
| S-6 | 00034304006 (1.0 ks) | 2 457 438.692 | 0.82 | 0.0863 ± 0.0126 | 0.0462 ± 0.0085 |
| S-7 | 00034304007 (3.7 ks) | 2 457 441.646 | 0.91 | 0.0334 ± 0.0034 | 0.0251 ± 0.0030 |
| S-8 | 00034304008 (2.8 ks) | 2 457 444.605 | 0.99 | 0.0068 ± 0.0018 | 0.0040 ± 0.0014 |
| S-9 | 00034304009 (3.8 ks) | 2 457 447.656 | 0.08 | 0.0070 ± 0.0015 | 0.0035 ± 0.0011 |
| S-10 | 00034304010 (2.8 ks) | 2 457 453.179 | 0.24 | 0.0249 ± 0.0033 | 0.0228 ± 0.0031 |
| S-11 | 00034304011 (2.0 ks) | 2 457 455.908 | 0.32 | 0.0360 ± 0.0056 | 0.0331 ± 0.0052 |
| S-12 | 00034304012 (1.4 ks) | 2 457 456.626 | 0.34 | 0.0484 ± 0.0064 | 0.0429 ± 0.0061 |
| S-13 | 00034304013 (1.4 ks) | 2 457 476.611 | 0.92 | 0.0266 ± 0.0050 | 0.0293 ± 0.0054 |
| S-14 | 00034304014 (1.9 ks) | 2 457 480.297 | 0.03 | 0.0066 ± 0.0020 | 0.0036 ± 0.0016 |
| S-15 | 00034304015 (1.5 ks) | 2 457 484.685 | 0.16 | 0.0136 ± 0.0032 | 0.0158 ± 0.0035 |
| S-16 | 00034304016 (0.8 ks) | 2 457 486.085 | 0.20 | 0.0254 ± 0.0066 | 0.0164 ± 0.0053 |
| S-17 | 00034304017 (0.3 ks) | 2 457 486.887 | 0.22 | 0.0176 ± 0.0089 | 0.0087 ± 0.0063 |
| S-18 | 00034304018 (3.8 ks) | 2 457 494.506 | 0.44 | 0.0518 ± 0.0040 | 0.0349 ± 0.0033 |
Notes. X for XMM-Newton observations and S for Swift exposures. HJD correspond to dates at mid-exposure, and the corresponding phases were calculated using the ephemeris of Paper I; exposure times correspond to on-axis values (for pn if XMM-Newton). The XMM-Newton count rates correspond to the sum of MOS1, MOS2, and pn values. We note that the Swift XID notation follows the ObsID naming scheme (there is thus no S-1 as 00034304001 has zero seconds of useful time).
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