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Table A.2
Results from various Markov chains of the three parameters which control the shape of the Rossiter-McLaughlin effect.
V sin I (km s-1) ± | β (°) ± | b (R ⋆ ) ± | ||||||||||||
1 σ | 2 σ | 3 σ | 1 σ | 2 σ | 3 σ | 1 σ | 2 σ | 3 σ | ||||||
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V sin IPrior off | ||||||||||||||
0.82 |
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-1 |
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0.27 |
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V sin IPrior on, 1.35 km s-1 | ||||||||||||||
1.21 |
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-43 |
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0.05 |
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V sin IPrior on, 2.2 km s-1 | ||||||||||||||
2.03 |
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68 |
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0.04 |
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-69 |
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Rossiter-McLaughlin effect not fitted | ||||||||||||||
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0 | (fixed) | 0 | (fixed) | 0.28 |
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Photometry Limited runs | ||||||||||||||
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V sin IPrior off | ||||||||||||||
0.87 |
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4 |
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0.28 | (fixed) | |||||
V sin IPrior on, 1.35 km s-1 | ||||||||||||||
1.15 |
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-15 |
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0.28 | (fixed) | |||||
V sin IPrior on, 2.2 km s-1 | ||||||||||||||
1.37 |
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-44 |
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0.28 | (fixed) | |||||
Notes. These are for circular non drifting orbital solutions.
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