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Table 3

Correlations between the investigated planetary and stellar parameters expected to influence the He I observability.

X, Y ρ Spearman Correlation strength p-value
FEUV,δRP/Heq${F_{{\rm{EUV}}}},{\delta _{{R_P}}}/{H_{{\rm{eq}}}}$ 0.0116 ± 0.0029 Null 0.98
FEUV, c 0.1663 ± 0.0029 Low 0.69
Teff,δRP/Heq${T_{{\rm{eff}}}},{\delta _{{R_P}}}/{H_{{\rm{eq}}}}$ −0.0302 ± 0.0028 Null 0.94
Teff, c −0.1665 ± 0.0027 Low 0.70
gP,δRP/Heq${g_{\rm{P}}},{\delta _{{R_P}}}/{H_{{\rm{eq}}}}$ 0.0664 ± 0.0028 Null 0.88
𝑔P,c −0.1886 ± 0.0026 Low 0.65
logRHK,δRP/Heq$\log R_{{\rm{HK}}}^\prime ,{\delta _{{R_P}}}/{H_{{\rm{eq}}}}$ −0.1303 ± 0.0028 Low 0.76
log RHK,c 0.1461 ± 0.0030 Low 0.73

Notes. From left to right: the parameters investigated for the correlation, the Spearman value, the strength of correlation from Kuckartz et al. (2013), and the associated p-value.

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