Table 2.
continued.
Parameter | J1038−37 | J1013+01 | J1115−36 | J0339+03 | J1403−32 |
---|---|---|---|---|---|
Spectroscopic measurements of primary star | |||||
Teff (K) | ![]() |
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[Fe/H] (dex) | ![]() |
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log g1 (dex) | ![]() |
![]() |
![]() |
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![]() |
v sin i1 (km s−1) | <5 | ![]() |
![]() |
![]() |
<5 |
Parameters from bagemass iteration | |||||
System age (Gyr) | ![]() |
![]() |
![]() |
![]() |
![]() |
M1 (M⊙) | ![]() |
![]() |
![]() |
![]() |
![]() |
Free parameters in MCMC sampling | |||||
P (d) | ![]() |
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t0 (d) | ![]() |
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D | ![]() |
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W (d) | ![]() |
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b | ![]() |
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K (km s−1) | ![]() |
![]() |
![]() |
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![]() |
fs | 0 (fixed) | 0 (fixed) | ![]() |
0 (fixed) | ![]() |
fc | 0 (fixed) | 0 (fixed) | ![]() |
0 (fixed) | ![]() |
Derived parameters | |||||
M1 (M⊙) | ![]() |
![]() |
![]() |
![]() |
![]() |
R1 (R⊙) | ![]() |
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![]() |
ρ1(ρ⊙) | ![]() |
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![]() |
M2 (M⊙) | ![]() |
![]() |
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R2 (R⊙) | ![]() |
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log g2 (cgs) | ![]() |
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![]() |
fm (M⊙) | ![]() |
![]() |
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![]() |
e | 0 (fixed) | 0 (fixed) | ![]() |
0 (fixed) | ![]() |
a (au) | ![]() |
![]() |
![]() |
![]() |
![]() |
ω (deg) | 0 (fixed) | 0 (fixed) | ![]() |
0 (fixed) | ![]() |
i (deg) | ![]() |
![]() |
![]() |
![]() |
![]() |
Prot, primary (d)(*) | – | ![]() |
![]() |
![]() |
– |
Instruments and fit properties | |||||
Instruments | Eu, COR | TR, COR | TR, SP, W, COR | TR, COR | Eu, COR |
Radial velocity baseline | cubic time | – | – | – | |
Flux baseline | linear time | – | – | linear time | lin. centroid-y(**) |
Notes. The high precision of the orbital period of EBLM J2017+02Ab and EBLM J1115-36Ab is due to the use of the WASP discovery light curves in the fit, together with radial velocities and transits observed with TRAPPIST. (*)Assuming a negligible inclination of the primary star spin axis. (**)Linear baseline in the y-coordinate of the centroid position on the detector.
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