Table A.1.
Observation IDs of Insight-HXMT in the 2018 outburst.
| ObsID | Time Start (UTC) | Exposure time (s) | MJD | Fluxa | PFb | PF | PF |
|---|---|---|---|---|---|---|---|
| HE/ME/LE | (10−9 erg cm−2 s−1) | (30-60 keV) | (10-30 keV) | (1-10 keV) | |||
| P0114709001 | 2018-04-13 | 2055/1710/1256 | 58221.62 | 4.50 ± 0.20 | 0.45 ± 0.02 | 0.32 ± 0.03 | 0.30 ± 0.05 |
| P0114709002 | 2018-04-14 | 340/1020/299 | 58222.41 | 4.47 ± 0.28 | 0.43 ± 0.05 | 0.35 ± 0.04 | 0.33 ± 0.09 |
| P0114709003 | 2018-04-15 | 4492/4470/3411 | 58223.54 | 4.71 ± 0.38 | 0.39 ± 0.01 | 0.24 ± 0.02 | 0.23 ± 0.03 |
| P0114709004 | 2018-04-16 | 3648/3239/2098 | 58224.15 | 5.20 ± 0.36 | 0.37 ± 0.01 | 0.28 ± 0.02 | 0.28 ± 0.03 |
| P0114709005 | 2018-04-17 | 2778/2670/1436 | 58225.14 | 5.93 ± 0.31 | 0.37 ± 0.01 | 0.25 ± 0.02 | 0.20 ± 0.04 |
| P0114709006 | 2018-04-18 | 2771/2610/1496 | 58226.13 | 6.33 ± 0.29 | 0.36 ± 0.01 | 0.28 ± 0.02 | 0.27 ± 0.04 |
| P0114709007 | 2018-04-19 | 4693/4050/3171 | 58227.52 | 6.60 ± 0.28 | 0.31 ± 0.01 | 0.27 ± 0.01 | 0.24 ± 0.02 |
| P0114709008 | 2018-04-20 | 629/2190/1316 | 58228.31 | 6.89 ± 0.28 | 0.27 ± 0.03 | 0.28 ± 0.02 | 0.29 ± 0.04 |
| P0114709009 | 2018-04-21 | 2186/1980/952 | 58229.12 | 7.00 ± 0.28 | 0.31 ± 0.01 | 0.28 ± 0.02 | 0.27 ± 0.04 |
| P0114709010 | 2018-04-21 | 3247/2790/1518 | 58230.04 | 7.61 ± 0.31 | 0.28 ± 0.01 | 0.28 ± 0.02 | 0.24 ± 0.03 |
| P0114709011 | 2018-04-23 | 1223/2520/837 | 58231.31 | 7.20 ± 0.31 | 0.35 ± 0.02 | 0.26 ± 0.02 | 0.24 ± 0.04 |
| P0114709012 | 2018-04-24 | 3103/2940/1316 | 58232.37 | 7.65 ± 0.30 | 0.26 ± 0.01 | 0.30 ± 0.02 | 0.29 ± 0.03 |
| P0114709013 | 2018-04-25 | 2466/3360/2304 | 58233.48 | 7.78 ± 0.30 | 0.29 ± 0.01 | 0.25 ± 0.01 | 0.26 ± 0.02 |
| P0114709014 | 2018-04-27 | 3687/3419/1473 | 58235.88 | 7.62 ± 0.31 | 0.29 ± 0.01 | 0.26 ± 0.01 | 0.24 ± 0.03 |
| P0114709015 | 2018-04-28 | 945/1800/172 | 58237.09 | 7.70 ± 0.31 | 0.28 ± 0.02 | 0.27 ± 0.02 | 0.33 ± 0.08 |
| P0114709016 | 2018-04-30 | 475/2700/1697 | 58238.48 | 7.85 ± 0.36 | 0.34 ± 0.03 | 0.28 ± 0.02 | 0.26 ± 0.03 |
| P0114709017 | 2018-05-01 | 4545/4500/2094 | 58239.68 | 7.67 ± 0.32 | 0.27 ± 0.01 | 0.29 ± 0.01 | 0.24 ± 0.02 |
| P0114709018 | 2018-05-02 | 2361/2430/636 | 58240.94 | 8.31 ± 0.32 | 0.27 ± 0.01 | 0.28 ± 0.02 | 0.29 ± 0.04 |
| P0114709019 | 2018-05-03 | 3184/3030/1182 | 58241.85 | 8.17 ± 0.31 | 0.27 ± 0.01 | 0.29 ± 0.01 | 0.28 ± 0.03 |
| P0114709020 | 2018-05-04 | 4719/4590/2054 | 58242.66 | 7.95 ± 0.30 | 0.28 ± 0.01 | 0.26 ± 0.01 | 0.25 ± 0.02 |
| P0114709021 | 2018-05-05 | 3423/3329/924 | 58243.77 | 7.95 ± 0.31 | 0.28 ± 0.01 | 0.26 ± 0.01 | 0.28 ± 0.04 |
| P0114709022 | 2018-07-04 | 4359/6080/897 | 58303.37 | 2.16 ± 0.25 | 0.55 ± 0.03 | 0.40 ± 0.02 | 0.29 ± 0.06 |
| P0114709023 | 2018-07-05 | 1079/3000/478 | 58304.26 | 2.18 ± 0.29 | 0.57 ± 0.06 | 0.43 ± 0.03 | 0.51 ± 0.12 |
| P0114709025 | 2018-07-06 | 4173/4110/1436 | 58305.57 | 1.99 ± 0.26 | 0.56 ± 0.03 | 0.43 ± 0.03 | 0.34 ± 0.06 |
| P0114709026 | 2018-07-07 | 2225/2190/897 | 58306.76 | 1.80 ± 0.24 | 0.73 ± 0.06 | 0.41 ± 0.04 | 0.38 ± 0.08 |
| P0114709027 | 2018-07-08 | 970/2130/837 | 58307.82 | 1.80 ± 0.18 | 0.69 ± 0.08 | 0.52 ± 0.05 | 0.49 ± 0.08 |
| P0114709028 | 2018-07-09 | 1278/2909/778 | 58308.89 | 1.97 ± 0.19 | 0.45 ± 0.05 | 0.38 ± 0.04 | 0.36 ± 0.08 |
| P0114709029 | 2018-07-10 | 1098/1710/658 | 58309.74 | 1.99 ± 0.18 | 0.65 ± 0.07 | 0.42 ± 0.05 | 0.47 ± 0.09 |
| P0114709030 | 2018-07-11 | 1916/1800/778 | 58310.66 | 1.44 ± 1.06 | 0.86 ± 0.08 | 0.46 ± 0.05 | 0.36 ± 0.07 |
Notes. a The unabsorbed flux of 2S 1417-624 is computed from the count rate history provided by SWIFT/BAT by multiplying a conversion factor of 1.01 × 10−7 erg cts−1 in 2–140 keV range (see Sect. 4).
b The pulse fraction (PF=(Imax-Imin)/(Imax+Imin)) is calculated from the background-subtracted light curves.
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