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Table 4

Simulated ideal RV mass measurement significances and precisions for MAROON-X, KPF, and SPIRou.

Instrument Nobs Low High Rocky   Water Puffy
Simulated RV mass measurement significance (σ)

4 4 16 11 5 7
MAROON-X 6 5 20 13 7 8
8 5 24 16 7 9
10 6 25 17 10 10

4 2 9 5 3 3
KPF 6 2 10 6 4 4
8 3 12 8 4 4
10 3 13 8 4 5

4 1 3 2 2 2
SPIRou-low 6 2 4 3 2 2
8 1 5 3 2 2
10 2 5 4 2 2

4 2 3 2 2 2
SPIRou-high 6 1 3 2 2 2
8 1 3 2 2 2
10 2 3 2 1 2
Simulated RV mass measurement precision (%)

4 28 6 10 19 15
MAROON-X 6 22 5 8 15 12
8 19 4 6 14 11
10 18 4 6 11 10

4 50 12 20 39 37
KPF 6 45 10 16 30 30
8 37 9 13 27 23
10 34 8 12 27 20

4 76 37 61 69 64
SPIRou-low 6 68 29 49 63 50
8 83 22 41 52 57
10 62 24 32 57 57

4 71 41 60 69 69
SPIRou-high 6 83 43 56 57 67
8 80 40 52 72 55
10 63 44 57 79 71

Notes. The significance of an RV mass measurement is here defined as med(k)/σ(k), where med(k) is the median of the RV semi-amplitude posterior estimate and σ(k) its standard deviation, while the RV measurement precision is σ(k)/med(k). The number of 1 h long exposures used in the simulations is marked by Nobs, and low, high, rocky, water, and puffy refer to different planet mass scenarios leading to RV semiamplitudes of 1.9, 8.3, 5.4, 2.8, and 3.3 m s−1, respectively. For SPIRou, we consider the lower and upper precision limits of 6 and 11 m s−1 per exposure separately. The estimates should be considered somewhat optimistic since they consider only photon noise and do not include the RV signals due to stellar granulation and variability.

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