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Table 3

Planetary parameter best-fit values obtained through a joint modelling of Keplerian signals and correlated stellar noise, using Gaussian process regression.

Jump parameter Prior Best-fit value
h [m s−1] (0,10) 1.84
λ [days] (20,150) 36.4
w (0,1) 0.59
θ [days] 46.7
σjit, HIRES-pre [m s−1] 1.48 ± 0.72
σjit, HIRES-post [m s−1] 1.01
σjit, HARPS-N [m s−1] 1.49
γHIRES-pre [m s−1] (–100,100) 2.2 ± 1.6
γHIRES-post [m s−1] (–100,100) 1.9
γHARPS-N [m s−1] (–100,100) 0.5 ± 1.1
Kb [m s−1] Modified scale invariant 1.68
K0 = 1; Kmax = 10
Pb [days] (10.9,12.0) 11.4407
T0,b [BJD-2 450 000] 6995.86
(–1,1) 0.11 ± 0.33
(–1,1) –0.29
Kc [m s−1] Modified scale invariant 2.5
K0 = 1; Kmax = 100
lnPc [ ln days] 8.93
7600 [days]
T0,c [BJD-2 450 000] 10730
(–1,1) 0.10
(–1,1) 0.19
dVrdt [m s−1 day−1] (–0.1,0.1) –0.00024
Derived quantitiesa
eb 0.094
<0.13 (68.3th percentile)
ωb [rad] 0.96
Mp, b sin i (M) 3.03
ap, b (AU) 0.072
ec 0.27
<0.40 (68.3th percentile)
ωc [rad] –1.02
Mp, c sin i (M) 36
ap, c (AU) 5.4

Notes. (a) Derived quantities from the posterior distributions. We used the following equations (assuming Ms + mpMs): ; , where G is the gravitational constant.

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