| The Star | |||||
|---|---|---|---|---|---|
| Simbad GAIA 2MASS |
G 41-26 DR2 604215144503584640 J09084885+1151411 |
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| RA | 09:08:48.8546 | DEC | +11:51:41.116 | ||
| Parallax 45.804 mas |
P.M. RA -458.496 mas/y |
P.M. DEC 192.629 mas/y |
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| MagV* 15.43 |
MagR 14.4 |
MagI* 12.326 |
MagJ 10.739 |
MagH 10.17 |
MagK 9.899 |
| MagG 13.796 |
MagGBP 15.563 |
MagGRP 12.528 |
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| *Calculated from GAIA magnitudes. | |||||
|
Ephemeris
- Not verified |
|||||
|---|---|---|---|---|---|
| Hirano et al. 2023 | |||||
| Mid-time 2458100.07116 ± 0.00069 BJDTDB |
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| Period 4.0179694 ± 2.7e-06 days |
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| Transit Parameters | |||||
| Hirano et al. 2023 | |||||
| Rp/Rs 0.0472 ± 0.002 |
a/Rs 29.63 +0.86 -0.91 |
i 89.32 +0.41 -0.41 deg |
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| e - |
ω - deg |
||||
| DepthR* 2.95 mmag |
Duration* 1.02 hours |
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|
*Calculated from the other parameters, using PyLightcurve.
**Adjusted based on the space observations. |
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| Limb Darkening Parameters | |||||
| Hirano et al. 2023 | |||||
| Teff 3173.0 +53.0 -53.0 K |
Log(g) 5.07 +0.03 -0.03 cm/s2 |
Fe/H -0.13 +0.18 -0.18 dex |
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| ExoClock Status | |||||
|---|---|---|---|---|---|
| Observing Priority | HIGH | ||||
| Minimum aperture | 76.71" | ||||
| Total Observations (Recent) | 9 (0) | ||||
| O-C | - | ||||
| ExoClock Observations (Recent) | 0 (0) | ||||
| Space Observations (Recent) | 9 (0) | ||||
| ETD Observations (Recent) | 0 (0) | ||||
| Literature Mid-times (Recent) | 0 (0) | ||||
| Kepler Rp/Rs | 0.0528 ± 0.0011 | ||||
| TESS Rp/Rs | - | ||||
Space Observations |
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| Planet Observation Date |
Mission | O-C minutes |
||
|---|---|---|---|---|
| K2-415b (HIGH) 2018-02-22 | K2 | 209.36 ± 3.46 | ||
| K2-415b (HIGH) 2018-02-06 | K2 | -4.37 ± 2.88 | ||
| K2-415b (HIGH) 2018-01-25 | K2 | -1.76 ± 3.46 | ||
| K2-415b (HIGH) 2018-01-21 | K2 | -9.83 ± 1.37 | ||
| K2-415b (HIGH) 2018-01-17 | K2 | -1.56 ± 1.73 | ||
| K2-415b (HIGH) 2018-01-13 | K2 | -2.33 ± 2.02 | ||
| K2-415b (HIGH) 2017-12-28 | K2 | -1.93 ± 3.46 | ||
| K2-415b (HIGH) 2017-12-12 | K2 | 16.76 ± 3.46 | ||
| K2-415b (HIGH) 2017-12-08 | K2 | -14.79 ± 0.92 | ||