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Table 3

Radial velocities of USco16m25 derived from the cross-correlation function method.

Date HJDa Phase RV1b δRV1 RV2c δRV2 F21 eF21
ddmmyyyy days km s-1 km s-1 km s-1 km s-1

03062015 2 457 176.484357799 0.300 36.29 0.33 +38.83 0.32 0.9664 0.0481
03062015 2 457 176.512210492 0.314 31.37 0.43 +36.85 0.43 0.9818 0.0765
03062015 2 457 176.535586138 0.332 40.79 0.47 +32.96 0.68 0.9906 0.1018
03062015 2 457 176.585451550 0.350 25.71 0.47 +36.41 0.47 0.9813 0.0687
09062015 2 457 182.521620525 0.463 0.56 0.12
09062015 2 457 182.545150519 0.472 1.17 0.10
09062015 2 457 182.587298515 0.487 +0.33 0.12
09062015 2 457 182.609963939 0.495 +1.67 0.13
09062015 2 457 182.632386450 0.503 +4.42 0.14
17062015 2 457 191.411856342 0.629 +27.95 0.14 28.81 0.21 0.9631 0.0357
07072015 2 457 211.460653753 0.767 +45.23 0.29 42.54 0.31 0.9634 0.0247
12072015 2 457 216.423575887 0.534 1.92d 0.17
13072015 2 457 217.422062478 0.889 +25.33 0.19 25.73 0.24 0.9638 0.0525
14072015 2 457 218.508007215 0.276 39.45 0.25 +43.86 0.29 0.9579 0.0562

Notes. RVs are estimated by performing a second-order polynomial fit to the peak of the CCFs. F21 represents the secondary-to-primary flux ratio, F2/F1, given by the ratio of the peaks of the cross-correlation functions of the secondary (F2) and primary (F1) component. The error of this measurement is given by eF21.

(a)

Heliocentric Julian day.

(b)

Radial velocity of the primary.

(c)

Radial velocity of the secondary.

(d)

Discarded RV point during the RV fitting procedure.

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