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Table 4
Radial velocities of KOI 12.
BJD (UTC) | RV | ± 1 σ | |
–2 400 000 | (km s-1) | (km s-1) | |
|
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Run 2012 | 56 103.5518 | –21.87 | 0.48 |
56 104.3650 | –21.26 | 0.48 | |
56 104.3832 | –20.95 | 0.40 | |
56 104.4030 | –20.88 | 0.42 | |
56 104.4201 | –21.86 | 0.39 | |
56 104.4381 | –21.96 | 0.34 | |
56 104.4580 | –22.29 | 0.40 | |
56 104.4766 | –23.00 | 0.39 | |
56 104.4884 | –22.57 | 0.38 | |
56 104.4999 | –22.76 | 0.39 | |
56 104.5110 | –21.90 | 0.37 | |
56 104.5208 | –22.11 | 0.38 | |
56 104.5299 | –22.85 | 0.36 | |
56 104.5387 | –22.98 | 0.38 | |
56 104.5480 | –22.65 | 0.37 | |
56 104.5587 | –22.80 | 0.36 | |
56 104.5675 | –22.39 | 0.37 | |
56 104.5760 | –22.76 | 0.38 | |
56 104.5861 | –22.22 | 0.39 | |
56 104.5982 | –22.38 | 0.37 | |
56 104.6155 | –22.60 | 0.40 | |
56 105.4795 | –22.26 | 0.36 | |
56 105.4886 | –22.07 | 0.38 | |
56 105.4973 | –21.99 | 0.38 | |
56 105.5351 | –22.31 | 0.38 | |
56 105.5453 | –21.99 | 0.38 | |
56 105.5568 | –22.60 | 0.36 | |
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Run 2013 | 56 461.3690 | –24.76 | 0.41 |
56 461.3842 | –24.57 | 0.37 | |
56 461.3992 | –24.35 | 0.38 | |
56 461.4126 | –24.72 | 0.36 | |
56 461.4259 | –25.88 | 0.73 | |
56 461.4409 | –24.35 | 0.39 | |
56 461.4559 | –23.00 | 0.54 | |
56 461.4710 | –23.16 | 0.51 | |
56 461.5313 | –24.25 | 0.36 | |
56 461.5401 | –24.12 | 0.37 | |
56 461.5488 | –24.29 | 0.39 | |
56 461.5575 | –24.02 | 0.38 | |
56 461.5662 | –24.55 | 0.39 | |
56 461.5747 | –24.24 | 0.39 | |
56 461.5831 | –23.93 | 0.39 | |
56 461.5915 | –24.07 | 0.39 | |
56 461.6010 | –24.36 | 0.38 | |
56 462.5911 | –24.24 | 0.69 | |
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Run 2014 | 56 807.5694 | –24.46 | 0.23 |
56 814.4686 | –24.39 | 0.19 |
Notes. Variations in the asymmetric continuum of the CCFs (Fig. 4), instrumental effects, or the presence of a massive distant companion to KOI-12 may cause the differences in systemic velocities between the three runs.
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