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Table 3

Cross-correlation results.

Vrest [km s−1] Kp [km s−1] S/N
gaussian fit max(S/N)-1 gaussian fit max(S/N)-1
CO (GIANO-B) 2.71 ± 0.51 3.006.00+3.00$3.00_{-6.00}^{+3.00}$ 195.00 ± 0.34 195.005.00+5.00$195.00_{-5.00}^{+5.00}$ 10.4
Fe I (GIANO-B) 14.5 ±0.5 / 205.9 ± 0.7 / 4.0
Fe I (HARPS-N) 0.55 ± 0.71 0.004.50+4.50$0.00_{-4.50}^{+4.50}$ 193.59 ± 0.59 196.009.00+5.00$196.00_{-9.00}^{+5.00}$ 3.5
Fe I (ESPRESSO) −0.36 ± 0.40 0.003.00+3.00$0.00_{-3.00}^{+3.00}$ 189.10 ± 0.49 189.005.00+5.00$189.00_{-5.00}^{+5.00}$ 6.2

Notes. For each investigated molecule, the planet’s orbital velocity (Kp), the velocity in the planet’s rest frame (Vrest), and the S/N of the detection are reported. Two types of values (with associated uncertainties) are provided for each measurement: one obtained by fitting a Gaussian to the 1D CC function at the peak position, and one estimated directly from the position of the peak of S/N in the map. In the latter case, the uncertainty is estimated by identifying where the S/N value decreases by 1 unit. Consequently, the number of decimal digits in the table differs according to the method employed to derive the corresponding value. Marginal detection obtained from only one observing night (namely N2). The Kp and Vrest values are computed by using a 2D Gaussian, including a rotation angle to account for the inclined feature of the detection blob (see Sect. 4.1).

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