Table A.1
Properties of the singles and multis in the three KOI subsets.
| FGK host stars | Sub-sample | Ns | Nm | [R⊕] |
[R⊕] |
K-S p-value | A-D p-value | M-W p-value |
|---|---|---|---|---|---|---|---|---|
| L24 subset I | Full subset | 1080 | 1055 | 2.19±0.01 | 2.12±0.01 | 0.16±0.11 | 0.04±0.02 | 0.25±0.09 |
| Excl. HJsa | 1029 | 1050 | 2.14±0.01 | 2.12±0.01 | 0.43±0.18 | ≥ 0.25 | 0.62±0.15 | |
| R < 4 R⊕ | 959 | 961 | 2.05±0.02 | 2.03±0.01 | 0.40±0.17 | ≥ 0.25 | 0.87±0.10 | |
| R ≥ 4 R⊕b | 121 | 94 | 8.32±0.24 | 6.41±0.22 | 0.001±0.002 | ≤ 10−3 | 0.001±0.002 | |
| L24 subset II | Full subset | 1080 | 1055 | 2.19±0.01 | 2.13±0.01 | 0.24±0.10 | 0.04±0.02 | 0.36±0.12 |
| Excl. HJsa | 1031 | 1053 | 2.13±0.01 | 2.13±0.01 | 0.26±0.14 | ≥ 0.25 | 0.45±0.13 | |
| R < 4 R⊕ | 966 | 969 | 2.05±0.01 | 2.04±0.01 | 0.27±0.16 | ≥ 0.25 | 0.81±0.14 | |
| R ≥ 4 R⊕b | 114 | 86 | 8.66±0.22 | 6.31±0.14 | <10−3 | ≤ 10−3 | <10−4 | |
| This work’s subset III | Full subset | 1080 | 1055 | 2.11±0.02 | 2.16±0.01 | 0.27±0.15 | 0.18±0.05 | 0.43±0.14 |
| Excl. HJsa | 1036 | 1053 | 2.05±0.02 | 2.16±0.01 | 0.07±0.06 | 0.02±0.01 | 0.02±0.01 | |
| R < 4 R⊕ | 979 | 964 | 1.99±0.02 | 2.05±0.01 | 0.19±0.12 | 0.18±0.06 | 0.18±0.09 | |
| R ≥ 4 R⊕b | 101 | 91 | 7.70±0.23 | 5.98±0.14 | 0.01±0.01 | 0.001±0.002 | 0.001±0.002 | |
Notes. Comparisons of the confirmed singles and multis orbiting FGK stars in each of the three KOI subsets (Sect. 3.4). s and m stand for singles and multis, respectively, while N and
represent the number and the median radii of the planets in each sample, 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 all 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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