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Table 2

He I measurements.

Target Roche lobe (Rp) ɡp (m s−2) Excess of absorption (%) Heq (km) δRP/Heq${{{\delta _{{R_{\rm{P}}}}}} \mathord{\left/ {\vphantom {{{\delta _{{R_{\rm{P}}}}}} {{{\rm{H}}_{{\rm{eq}}}}}}} \right. \kern-\nulldelimiterspace} {{{\rm{H}}_{{\rm{eq}}}}}}$ F5−504 Å (103 erg s−1 cm−2) 3σ (1010 g s−1)
HAT-P-3b 3.6 7 17.5 <1.9 2 92 7.968 7.772
HAT-P-33b 2.167 5.1 <1. 2231 33 6.195 8.205
HAT-P- 9b 3.207 21.5 <0.6 629 61 1.51 5.702
HD893 5b 8.213 7.8 <0.7 855 76 0.2 3.899
K2-105b 11.202 23.6 <2.33 219 378 1.69 6.028
Kepler-25c 8.1 8 5.3 <1.86 1192 82 1.019 65.26
Kepler-68b 8.722 15.2 <0.72 533 112 1.176 8.13
WASP- 7d 9.565 10.9 <3.29 533 230 0.577 7.85

Notes. From left to right: Roche lobe (estimated following Eggleton 1983), planet’s surface gravity, excess of absorption, atmospheric scale heights (computed by assuming µ = 1.3, Sect. 7), δRP/Heq${{{\delta _{{{\rm{R}}_{\rm{P}}}}}} \mathord{\left/ {\vphantom {{{\delta _{{{\rm{R}}_{\rm{P}}}}}} {{{\rm{H}}_{{\rm{eq}}}}}}} \right. \kern-\nulldelimiterspace} {{{\rm{H}}_{{\rm{eq}}}}}}$ (i.e. the 3σ upper limits), the stellar XUV flux at the planet position, and the mass-loss rates computed with the p-winds code at 3σ.

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