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Table 4

Properties of the singles and multis in the FGK, early-, and late-type M samples.

Spec. type Sub-sample Ns Nm RS~Mathematical equation: $\[\widetilde{R_{S}}\]$ (R) Rm~Mathematical equation: $\[\widetilde{R_{m}}\]$ (R) K–S p-value A–D p-value M–W p-value
FGK Full samp. 1587 1397 2.57 ± 0.02 2.21 ± 0.01 <10−14 ≤10−3 <10−26
Excl. HJsa 1232 1379 2.24 ± 0.01 2.19 ± 0.01 0.26 ± 0.12 0.11 ± 0.04 0.21 ± 0.07
R < 4 R 1099 1258 2.10 ± 0.01 2.09 ± 0.01 0.67 ± 0.17 ≥0.25 0.74 ± 0.15
R ≥ 4 Rb 133 121 6.94 ± 0.20 6.10 ± 0.09 0.12 ± 0.06 0.04 ± 0.03 0.04 ± 0.02

M0-2 Full samp. 87 80 2.08 ± 0.04 1.64 ± 0.04 <10−4 ≤10−3 <10−3
Excl. HJsa 76 80 1.94 ± 0.04 1.64 ± 0.04 0.012 ± 0.009 0.004 ± 0.002 0.016 ± 0.009
R < 4 R 65 79 1.79 ± 0.04 1.62 ± 0.04 0.37 ± 0.13 0.15 ± 0.05 0.27 ± 0.09

M3-9 Full samp. 56 45 1.81 ± 0.07 1.22 ± 0.03 0.003 ± 0.003 ≤10−3 <10−3
Excl. HJsa 48 45 1.53 ± 0.05 1.22 ± 0.03 0.047 ± 0.029 0.017 ± 0.009 0.018 ± 0.10
R < 4 R 48 45 1.53 ± 0.05 1.22 ± 0.03 0.047 ± 0.029 0.017 ± 0.009 0.018 ± 0.10

Notes. s and m stand for singles and multis, respectively, while N and R~Mathematical equation: $\[\widetilde{R}\]$ represent the number and the median radii of the planets in each sample, respectively. Spectral types M0-2 and M3-9 correspond to early- and late-type M dwarfs, respectively. The p-values indicate the significance of the differences between Rs and Rm in each sample, as measured with three tests: the Kolmogorov–Smirnov (K–S), the two-sample Anderson–Darling (A–D), and the Mann-Whitney (M–W) U test. All the reported ±1σ-uncertainties are computed via Monte Carlo simulations (Sect. 3.3). (a)This sub-sample comprises the singles and multis in the sample, after removing the hot Jupiters. (b)This sub-sample contains the giants with R ≥ 4 R, excluding the hot Jupiters.

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