Table 4
Model and reference statistical parameters from the simultaneous fit of radial velocities and transit photometry.
Parameter | One planet + GP(a) | Two planets | Two planets + GP | ||
---|---|---|---|---|---|
planet | b | b | c | b | c |
P(d) | 4.052037 ± 0.000004 | 4.052039 ± 0.000005 | 16.04 ± 0.04 | 4.052037 ± 0.000005 | 16.06![]() |
K(m s−1) | 17.6 ± 0.8 | ![]() |
6.9 ± 0.3 | 17.4![]() |
6.3![]() |
e | 0.04 ± 0.02 | ![]() |
0.26 ± 0.06 | 0.04 ± 0.02 | 0.12![]() |
ω (deg) | 219 ± 19 | ![]() |
297 ± 112 | 21 ± 7 | 92![]() |
tperi (d)(b) | 1.80 ± 0.23 | ![]() |
7.3 ± 0.9 | 1.82 ± 0.09 | 14.0![]() |
i(deg) | 87.3 ± 0.2 | ![]() |
… | 87.3 ± 0.2 | … |
Rp ∕R⋆ | 0.0751 ± 0.0009 | ![]() |
… | ![]() |
… |
R⋆ (R⊙) | 0.57 ± 0.02 | 0.58 ± 0.02 | … | 0.57 ± 0.02 | … |
u1 | 0.48 ± 0.08 | 0.5 ± 0.1 | … | 0.47 ± 0.10 | … |
u2 (c) | 0.245 | 0.245 | … | 0.245 | … |
Derived parameters | |||||
a(au) | 0.0417 ± 0.0005 | 0.0417 ± 0.0005 | 0.104 ± 0.001 | 0.0417 ± 0.0005 | 0.104 ± 0.001 |
λ (deg)(b,d) | 336.1 ± 0.8 | 337.0 ± 0.9 | 135 ± 12 | 336.8![]() |
134 ± 27 |
tc (d)(b,e) | 0.38421![]() |
0.38401![]() |
13.22![]() |
0.38419![]() |
13.51![]() |
mp (M⊕) | 30.8 ± 1.5 | 30.7 ± 0.8 | 18.4 ± 1.0 | 30.5 ± 1.2 | 17.2![]() |
a∕R⋆ | 15.9![]() |
15.8![]() |
39.5![]() |
15.7![]() |
39.4![]() |
Rp (R⊕) | 4.7 ± 0.3 | 4.8 ± 0.3 | … | 4.7 ± 0.3 | … |
ρp (g cm−3) | 1.7 ± 0.3 | ![]() |
… | ![]() |
… |
Teq (K)(f) | 700![]() |
703![]() |
444![]() |
706![]() |
445![]() |
Instrumental parameters offset and weighted rms | |||||
CARMENES VIS (m s−1 ] | ![]() |
![]() |
![]() |
||
CARMENES NIR (m s−1) | ![]() |
![]() |
![]() |
||
ESPRESSO (m s−1) | ![]() |
![]() |
![]() |
||
HIRES (m s−1) | ![]() |
![]() |
![]() |
||
PFS (m s−1) | ![]() |
![]() |
![]() |
||
iSHELL (m s−1) | ![]() |
![]() |
![]() |
||
GP hyper parameters | |||||
Variance (m2 s−2) | ![]() |
… | ![]() |
||
τd (d) | ![]() |
… | ![]() |
||
− ln L | 316 | 336 | 303 | ||
Red. χ2 | 0.81 | 2.64 | 1.04 |
Notes. Uncertainties are given as 68% intervals. The planetary parameters of the transiting planet from the different models are within 1-σ of each other, proving the consistency of this signal. Posterior distributions of the parameters are displayed in Fig. 11. The derived values for semi-major axis and planetary mass take the stellar mass uncertainty listed in Table 2 into account. The likelihood − ln L and the reduced χ2 is given for the RV fit. (a) We found the best model to be the one planet + GP model. (b)Reference time is BJD = 2458438. (c)Fixed. (d) Mean longitude. (e) Time of inferior conjunction. (f)Assuming zero albedo and full heat redistribution.
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