Table 6
Orbit parameters and posteriors of Wendelstein-1b, based on separate multiband photometry and RV fitting.
| Wendelstein-1b | |
|---|---|
| Parameter | Result |
| P [d] | 2.663416 ± 0.000001 |
| t0 [BJD_TBD] | 2455367.738464 ± 0.000014 |
| RP [R*] | 0.1698 ± 0.0010 |
| a [a.u.] | 0.0282 ± 0.0015 |
| i [deg] |  |
| e(*) | <0.056 |
| e(**) | <0.012 |
| M [MJ] |  |
| ρ [g cm−3] |  |
| K [m s−1] | 115.56 ± 32.59 |
| Tpl [K] | ≤1884(1σ);2198(3σ) |
| ΔF(g′) | 0.0223 ± 0.0009 |
| ΔF(r′) | 0.0257 ± 0.0006 |
| ΔF(i′) | 0.0269 ± 0.0003 |
| ΔF(z′) | 0.0269 ± 0.0010 |
| ΔF(H) | 0.0275 ± 0.0007 |
| ΔF(Ks) | 0.0281 ± 0.0011 |
| u1(g′) |  |
| u2(g′) |  |
| u1(r′) |  |
| u2(r′) |  |
| u1(i′) |  |
| u2(i′) |  |
| u1(z′) |  |
| u2(z′) |  |
| u1(H) |  |
| u2(H) |  |
| u1(Ks) |  |
| u2(Ks) |  |
Notes. ΔF denotes the flux drop for the corresponding band. The uncertainties were determined via the MCMC processes as described in Sects. 5.1 and 5.2. The quadratic limb darkening coefficients u1 and u2 are given for each photometric band. (*)Upper limit based on transit measurements; (**)upper limit based on RV measurements.
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