Table 5
Stellar and planetary parameters for WASP-23 derived from light curve and RV fits to the GROND photometry and RV measurements from Triaud et al. (2011).
Quantity | Symbol | This work | Triaud et al. (2011) |
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|||
Stellar parameters | |||
Mass (M⊙) | M ∗ |
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Radius (R⊙) | R ∗ |
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Luminosity (L⊙) | L ∗ |
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– |
Density (cgs) | ρ ∗ |
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Surface gravity (cgs) | log (g∗) |
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4.4 ± 0.2 |
Effective temperature (K) | T eff |
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5150 ± 100 |
Metallicity | [Fe/H] |
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− 0.05 ± 0.13 |
|
|||
Planetary parameters | |||
Semi-major axis (AU) | a |
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Mass ( MJ) | M P |
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Radius ( RJ) | R P |
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Density (cgs) | ρ P |
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– |
Surface gravity | log (gP) |
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– |
Equilibrium temperaturea (K) | T eq |
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– |
Safronov Number | Θ |
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– |
Incident flux (109 erg s-1 cm-2) | ⟨ F ⟩ |
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– |
Orbital period (day) | P | 2.9444300 ± 0.0000011 |
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Reference transit time (BJD) | T 0 | 2 454 813.68159 ± 0.00042 |
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|
|||
RV parameters | |||
RV semi-amplitude (m/s) | K |
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– |
Mass ratio | MP/M∗ |
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– |
Notes.
Assuming a little redistribution over the surface of the planet, i.e., the area that is reemitting with average temperature Teq is , as in Hansen & Barman (2007).
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