Table 2.
Data strings.
| Set | HJD′-mid | Δt (d) | mag025 | mag075 | dM/dt | Φl |
|---|---|---|---|---|---|---|
| 01 | 2241.7735 | 148 | 16.778 | 16.760 | 1.77 | 0.95 |
| 02 | 2494.6013 | 340 | 16.836 | 16.845 | 1.38 | 0.27 |
| 03 | 2867.6482 | 401 | 16.792 | 16.790 | 1.90 | 0.75 |
| 04 | 3391.7015 | 641 | 16.814 | 16.813 | 1.46 | 0.43 |
| 05 | 4041.3132 | 653 | 16.807 | 16.803 | 2.00 | 0.26 |
| 06 | 4587.2472 | 433 | 16.808 | 16.780 | 2.72 | 0.96 |
| 07 | 4853.1629 | 95 | 16.817 | 16.818 | 1.43 | 0.30 |
| 08 | 4928.0578 | 55 | 16.860 | 16.851 | 1.22 | 0.40 |
| 09 | 5414.5181 | 273 | 16.754 | 16.734 | 1.85 | 0.02 |
| 10 | 5593.4558 | 118 | 16.789 | 16.734 | 1.43 | 0.25 |
| 11 | 5672.2730 | 38 | 16.804 | 16.760 | 1.47 | 0.35 |
| 12 | 5798.5795 | 151 | 16.814 | 16.820 | 1.08 | 0.52 |
| 13 | 5877.0519 | 58 | 16.833 | 16.837 | 1.40 | 0.62 |
| 14 | 5932.9618 | 55 | 16.842 | 16.800 | 3.71 | 0.69 |
| 15 | 5984.5826 | 40 | 16.803 | 16.763 | 3.33 | 0.76 |
| 16 | 6026.0065 | 59 | 16.757 | 16.770 | 3.04 | 0.81 |
| 17 | 6165.3956 | 144 | 16.733 | 16.728 | 2.31 | 0.99 |
| 18 | 6254.9853 | 133 | 16.751 | 16.728 | 2.09 | 0.10 |
| 19 | 6708.9257 | 310 | 16.802 | 16.752 | 1.00 | 0.69 |
| 20 | 7038.9236 | 180 | 16.743 | 16.721 | 1.92 | 0.11 |
| 21 | 7342.2775 | 532 | 16.801 | 16.770 | 1.80 | 0.50 |
| 22 | 7722.7651 | 148 | 16.767 | 16.735 | 2.08 | 0.99 |
| 23 | 8297.5512 | 369 | 16.790 | 16.764 | 2.17 | 0.73 |
| 24 | 8495.0520 | 157 | 16.750 | 16.730 | 3.24 | 0.98 |
| 25 | 9290.3548 | 1160 | 16.755 | 16.725 | 2.19 | 0.00 |
| 26 | 9905.8385 | 77 | 16.791 | 16.772 | 2.90 | 0.79 |
| 27 | 9985.8180 | 125 | 16.756 | 16.782 | 2.71 | 0.89 |
Notes. Mid of the HJD′ range, the range of days and the magnitudes at orbital phases 0.25 and 0.75 are given, according to the light curve model. Mass transfer rates, normalized to the value of string 19 and discussed in Sect. 3.3, are also given, along with the phases of the long-term cycle Φl according to Eq. (5).
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