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Table 3
Final results of the homogeneous reanalysis described in Sect. 5.3 with the corresponding limb-darkening coefficients.
| λ range (nm) | k = Rp∕R⋆ (HST) | α1 | α2 | α3 | α4 |
|---|---|---|---|---|---|
| 350.0–410.0 | 0.14022 ± 0.00110 | 0.7688 | – 1.2583 | 1.8781 | – 0.4346 |
| 410.0–440.0 | 0.13836 ± 0.00088 | 0.6393 | – 0.9882 | 1.9149 | – 0.6358 |
| 440.0–470.0 | 0.13877 ± 0.00067 | 0.5994 | – 0.8784 | 1.8883 | – 0.6953 |
| 470.0–495.0 | 0.13855 ± 0.00071 | 0.5903 | – 0.8136 | 1.8253 | – 0.7031 |
| 495.0–520.0 | 0.13808 ± 0.00077 | 0.5958 | – 0.7606 | 1.7314 | – 0.6821 |
| 520.0–540.0 | 0.13904 ± 0.00077 | 0.6008 | – 0.7129 | 1.6469 | – 0.6631 |
| 540.0–575.0 | 0.13874 ± 0.00062 | 0.6052 | – 0.6577 | 1.5473 | – 0.6385 |
| 550.0–586.8 | 0.13801 ± 0.00108 | 0.6058 | – 0.6380 | 1.5105 | – 0.6276 |
| 586.8–591.8 | 0.13846 ± 0.00268 | 0.6070 | – 0.6002 | 1.4400 | – 0.6068 |
| 591.8–620.0 | 0.13713 ± 0.00115 | 0.6079 | – 0.5701 | 1.3839 | – 0.5903 |
| 620.0–660.0 | 0.13798 ± 0.00094 | 0.6311 | – 0.5640 | 1.2853 | – 0.5517 |
| 660.0–710.0 | 0.13660 ± 0.00085 | 0.6472 | – 0.5788 | 1.2450 | – 0.5319 |
| 710.0–763.4 | 0.13700 ± 0.00105 | 0.6657 | – 0.5959 | 1.1987 | – 0.5092 |
| 763.4–773.4 | 0.14244 ± 0.00255 | 0.6670 | – 0.6063 | 1.1704 | – 0.4953 |
| 773.4–840.0 | 0.13622 ± 0.00098 | 0.6789 | – 0.6034 | 1.1400 | – 0.4821 |
| 840.0–910.0 | 0.13867 ± 0.00111 | 0.6815 | – 0.5972 | 1.0860 | – 0.4587 |
| 910.0–1020.0 | 0.13516 ± 0.00121 | 0.6848 | – 0.5889 | 1.0150 | – 0.4278 |
| Filter | k = Rp∕R⋆ (Ground) | α1 | α2 | α3 | α4 |
| u′ | 0.13803 ± 0.00264 | 0.8321 | – 1.3903 | 1.8601 | – 0.3362 |
| B | 0.13914 ± 0.00055 | 0.6097 | – 0.9264 | 1.9233 | – 0.6819 |
| g′ | 0.13765 ± 0.00050 | 0.5887 | – 0.8286 | 1.8520 | – 0.7091 |
| V | 0.13881 ± 0.00136 | 0.6047 | – 0.6754 | 1.5804 | – 0.6482 |
| r′ | 0.13779 ± 0.00076 | 0.6087 | – 0.5439 | 1.3350 | – 0.5759 |
| R | 0.13816 ± 0.00095 | 0.6293 | – 0.5623 | 1.2899 | – 0.5539 |
| i′ | 0.13872 ± 0.00116 | 0.6775 | – 0.6068 | 1.1691 | – 0.4947 |
| z′ | 0.14071 ± 0.00135 | 0.6849 | – 0.5888 | 1.0138 | – 0.4273 |
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