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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

V   sin   IPrior off
0.82 -1 0.27
V   sin   IPrior on, 1.35 km s-1
1.21 -43 0.05
V   sin   IPrior on, 2.2 km s-1
2.03   68 0.04
-69
Rossiter-McLaughlin effect not fitted

0 (fixed) 0 (fixed) 0.28
Photometry Limited runs

V   sin   IPrior off
0.87 4 0.28 (fixed)
V   sin   IPrior on, 1.35 km s-1
1.15 -15 0.28 (fixed)
V   sin   IPrior on, 2.2 km s-1
1.37 -44 0.28 (fixed)

Notes. These are for circular non drifting orbital solutions.

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