Table 10
Posterior values of all parameters used for HD 189567.
HD 189567 | |||
---|---|---|---|
Parameter | Units | ||
Offset and drift | |||
γH03 | m s−1 | −10 475.76 ± 0.18 | |
γH15 | m s−1 | −10 463.8 ± 1.4 | |
α1 | m s−1 yr−1 | 0.24 ± 0.10 | |
α2 | m s−1 yr−2 | 0.06 ± 0.02 | |
α3 | m s−1 yr−3 | −0.007 ± 0.004 | |
A (†) | m s−1 | 3.54 ± 0.36 | |
Noise | |||
σH03 | m s−1 | 1.97 ± 0.09 | |
σH15 | m s−1 | 1.0 ± 0.9 | |
σ(O−C) | m s−1 | 1.84 | |
Keplerians | |||
HD 189567 b | HD 189567 c | ||
P | day | 14.288 ± 0.002 | 33.688 ± 0.025 |
K | m s−1 | 2.53 ± 0.18 | 1.6 ± 0.2 |
e | <0.101; <0.189 (‡) | 0.16 ± 0.09 | |
ω | deg | –(‡) | 219 ± 58 |
λ0 | deg | −57 ± 5 | 196 ± 7 |
TPeriastron | BJD | 2 455 509 ± 3 | 2 455 502 ± 5 |
m sini | M⊕ | 8.5 ± 0.6 | 7.0 ± 0.9 |
a | AU | 0.111 ± 0.002 | 0.197 ± 0.003 |
Ref. Epoch | BJD | 2 455 500 |
Notes. We give the values of the mode and the 1σ confidence interval of the posterior distribution from the MCMC. (†)Linear parameter fitted on the FWHM using an Epanechnikov kernel with a high pass filter at a timescale of 1.5 yr. (‡) Eccentricity does not differ significantly from zero; the 68 and 95% upper limits are reported. The argument of periastron ω is therefore unconstrained.
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