Table C.4
He I 10 830 Å triplet equivalent width and XUV (5–504 Å) flux at planet distance.
Planet name | SpT | R* | EWa | FXUV,He | Modelb | Mp | Rp | ρp | References (planet data and He observation) |
---|---|---|---|---|---|---|---|---|---|
(R⊙) | (mÅ) | (W m−2) | (MJ) | (RJ) | (g cm−3) | ||||
GJ 436 b | M2.5V | 0.464±0.011 | <1.4 | 0.14±0.02 | 1 | 0.067±0.001 | 0.374±0.010 | 1.595±0.125 | Trifonov et al. (2018); Nortmann et al. (2018) |
GJ 1214 b | M4.5V | 0.216±0.012 | 33.2±2 8 | ![]() |
1 | 0.026±0.001 | 0.245±0.005 | 2.179±0.170 | Cloutier et al. (2021); Orell-Miquel et al. (2022) |
GJ 3470 b | M1.5V | 0.48±0.04 | 20.7±1.3 | ![]() |
1 | 0.040±0.004 | 0.374±0.053 | 0.940±0.408 | Kosiarek et al. (2019); Palle et al. (2020) |
HAT-P-11 b | K4V | 0.683±0.009 | 12.4±2.4 | 3.23±0.02 | 2 | 0.074±0.005 | 0.389±0.005 | 1.551±0.118 | Yee et al. (2018); Allart et al. (2018) |
HAT-P-18 b | K2V | 0.717±0.026 | 29.2±7.6 | 5.2: | 4 | 0.183±0.034 | 0.947±0.044 | 0.267±0.062 | Knutson et al. (2014); Paragas et al. (2021) |
HAT-P-26 b | K1V | 0.788±0.043 | 19.7±6.4 | <2.3 | 2 | 0.059±0.007 | 0.570±0.010 | 0.392±0.052 | Hartman et al. (2011); Vissapragada et al. (2022) |
HAT-P-32 b | F8V | 1.387±0.067 | 114.0±4.0 | ![]() |
2 | 0.750±0.130 | 1.789±0.025 | 0.162±0.029 | Bonomo et al. (2017); Czesla et al. (2022) |
HAT-P-67 b | F5IV | 2.65±0.12 | 147±25 | 361.0: | 4 | 0.320±0.180 | 2.164±0.010 | 0.039±0.022 | Gully-Santiago et al. (2024) |
HD 73583 b | K4V | 0.71±0.02 | 7.4±0.6 | ![]() |
1 | 0.032±0.011 | 0.249±0.009 | 2.579±0.904 | Barragán et al. (2022); Zhang et al. (2022a) |
HD 189733 b | K2V | 0.805±0.016 | 12.8±0.4 | ![]() |
1 | 1.154±0.025 | 1.138±0.077 | 0.971±0.198 | Paredes et al. (2021); Salz et al. (2018) |
HD 209458 b | G0V | 1.203±0.061 | 5.3±0.5 | ![]() |
1 | 0.685±0.017 | 1.390±0.018 | 0.316±0.015 | Wang & Ford (2011); Alonso-Floriano et al. (2019) |
HD 235088 b | K2V | 0.789±0.022 | 11.1±1.7 | ![]() |
2 | 0.022±0.006 | 0.187±0.018 | 4.172±1.657 | Zhang et al. (2023b); Orell-Miquel et al. (2023) |
HD 283636 b | K0V | 0.636±0.024 | 8.5±1.6 | ![]() |
2 | 0.025±0.006 | 0.205±0.027 | 3.599±1.664 | Zhang et al. (2023b) |
KELT-9 b | A0V | 2.362±0.07 | <1.2 | 0.2: | 5 | 2.880±0.350 | 1.840±0.040 | 0.573±0.079 | Borsa et al. (2019); Nortmann et al. (2018) |
TOI-1268 b | K2V | 0.92±0.06 | 17.7±1.9 | 6.8: | 4 | 0.303±0.026 | 0.810±0.050 | 0.707±0.144 | Šubjak et al. (2022); Orell-Miquel et al. (2024) |
TOI-1420 b | G6V | 0.923±0.024 | 42.9±5.1 | < 1.4 | 4 | 0.079±0.012 | 1.062±0.027 | 0.082±0.014 | Yoshida et al. (2023); Vissapragada et al. (2024) |
TOI-2018 b | K4V | 0.62±0.01 | 6.8±1.5 | 1.4: | 4 | 0.029±0.007 | 0.203±0.006 | 4.316±1.062 | Dai et al. (2023); Orell-Miquel et al. (2024) |
TOI-2076 b | K0 | 0.761±0.016 | 10.0±0.7 | ![]() |
3 | 0.028:c | 0.293±0.004 | 1.383: | Hedges et al. (2021); Zhang et al. (2023b) |
TOI-2134b | K5V | 0.744±0.027 | 3.3±0.3 | ![]() |
2 | 0.029±0.002 | 0.240±0.014 | 2.575±0.499 | Rescigno et al. (2024); Zhang et al. (2023a) |
WASP-12 b | G0V | 1.657±0.045 | <4.0 | <236.8 | 2 | 1.460±0.270 | 1.884±0.057 | 0.271±0.056 | Turner et al. (2021); Czesla et al. (2024) |
WASP-52 b | K2V | 0.79±0.02 | 39.6±1.4 | ![]() |
1 | 0.460±0.020 | 1.270±0.030 | 0.278±0.023 | Hébrard et al. (2013); Kirk et al. (2022) |
WASP-69 b | K4V | 0.813±0.028 | 28.3±0.9 | ![]() |
2 | 0.260±0.017 | 1.057±0.047 | 0.273±0.041 | Anderson et al. (2014); Nortmann et al. (2018) |
WASP-76b | F7IV-V | 1.73±0.04 | <21.3 | <103.4 | 2 | 0.920±0.030 | 1.830±0.060 | 0.186±0.019 | West et al. (2016); Casasayas-Barris et al. (2021) |
WASP-107 b | K7V | 0.66±0.02 | 87.2±7.6 | ![]() |
2 | 0.120±0.001 | 0.940±0.020 | 0.179±0.012 | Anderson et al. (2017); Allart et al. (2019) |
WASP-177b | K2V | 0.885±0.046 | 6.8±1.6 | 10.9: | 4 | 0.508±0.038 | 1.580±0.660 | 0.160±0.201 | Turner et al. (2019); Kirk et al. (2022) |
V1298 Tau b | K1IV | 1.305±0.07 | <19.0 | ![]() |
1 | 0.64±0.19 | 0.888±0.032 | 0.886±0.096 | Suárez Mascareño et al. (2021); Orell-Miquel et al. (2024) |
V1298 Tau c | K1IV | 1.305±0.07 | <95.8 | ![]() |
1 | 0.062±0.029 | 0.467±0.021 | 0.755±0.368 | Sikora et al. (2023); Orell-Miquel et al. (2024) |
55 Cnc e | G8V | 0.98±0.016 | <0.7 | ![]() |
0.027±0.001 | 0.174±0.003 | 6.396±0.492 | Crida et al. (2018); Zhang et al. (2021) | |
GJ 486 b | M3.5V | 0.328±0.011 | <1.9 | ![]() |
1 | (944±41)e-5 | 0.120±0.006 | 6.809±1.000 | Caballero et al. (2022); Masson et al. (2024) |
GJ 9827 b | K6V | 0.651±0.065 | <1.9 | ![]() |
1 | 0.015±0.001 | 0.136±0.005 | 7.485±1.022 | Kosiarek et al. (2021); Carleo et al. (2021) |
GJ 9827 d | K6V | 0.651±0.065 | <1.2 | ![]() |
1 | 0.011±0.002 | 0.174±0.007 | 2.515±0.540 | Kosiarek et al. (2021); Carleo et al. (2021) |
HD 63433 b | G5V | 0.912±0.034 | <2.0 | ![]() |
1 | <0.068:c | 0.191±0.007 | <12.174 | Mallorquín et al. (2023); Zhang et al. (2022b) |
HD 63433 c | G5V | 0.912±0.034 | <4.2 | ![]() |
1 | 0.048±0.013 | 0.243±0.009 | 4.181±1.220 | Mallorquín et al. (2023); Zhang et al. (2022b) |
HD 97658 b | K1V | 0.73±0.02 | <0.9 | ![]() |
1 | 0.025±0.002 | 0.200±0.009 | 3.782±0.558 | Van Grootel et al. (2014); Kasper et al. (2020) |
K2-100b | G0V | 1.22±0.02 | <5.7 | ![]() |
2 | 0.069±0.019 | 0.346±0.014 | 2.054±0.635 | Barragán et al. (2019); Gaidos et al. (2020) |
K2-105b | G8V | 0.91±0.01 | <23.3 | 1.2: | 4 | 0.094±0.060 | 0.301±0.011 | 4.275±2.768 | Narita et al. (2017); Zhang et al. (2023b) |
K2-136c | K5V | 0.66±0.02 | <25.0 | ![]() |
2 | 0.022:c | 0.260±0.010 | 1.552: | Mann et al. (2018); Gaidos et al. (2021) |
Kepler-25 c | F6V | 1.31 ±0.02 | <18.6 | 1.5: | 4 | 0.048±0.004 | 0.465±0.006 | 0.591±0.060 | Mills et al. (2019); Zhang etal. (2023b) |
Kepler-68 b | G1V | 1.24±0.02 | <7.2 | < 0.8 | 4 | 0.024±0.004 | 0.206±0.065 | 3.415±3.287 | Mills et al. (2019); Zhang etal. (2023b) |
TOI-1807b | K3V | 0.68±0.015 | <2.8 | 207.30±59.90 | 3 | 0.008±0.002 | 0.122±0.009 | 5.498±1.630 | Nardiello et al. (2022); Masson et al. (2024) |
TOI-3757 b | M0V | 0.62±0.01 | <73.0 | < 12.7 | 4 | 0.268±0.028 | 1.071±0.040 | 0.271±0.041 | Kanodia et al. (2022) |
TRAPPIST-1 b | M8V | 0.119±0.001 | <3.5 | ![]() |
2 | (43.2±2.2)e-4 | 0.100±0.001 | 5.429±0.336 | Agol et al. (2021); Krishnamurthy et al. (2021) |
TRAPPIST-1 e | M8V | 0.119±0.001 | <10.5 | 0.11±0.01 | 2 | (218±7)e-5 | 0.082±0.001 | 4.889±0.264 | Agol et al. (2021); Krishnamurthy et al. (2021) |
TRAPPIST-1 f | M8V | 0.119±0.001 | <4.1 | 0.07±0.00 | 2 | (327±10)e-5 | 0.093±0.001 | 5.004±0.244 | Agol et al. (2021); Krishnamurthy et al. (2021) |
WASP-47 d | G9V | 1.14±0.01 | <32.9 | 1.1: | 4 | 0.041±0.005 | 0.319±0.004 | 1.575±0.190 | Vanderburg et al. (2017); Zhang et al. (2023b) |
WASP-48 b | F8IV | 1.75±0.09 | <25 | 207.9: | 4 | 0.984±0.085 | 1.670±0.100 | 0.262±0.052 | Enoch et al. (2011); Bennett et al. (2023) |
WASP-80 b | K7V | 0.63±0.15 | <21 | ![]() |
2 | 0.554±0.040 | 0.952±0.027 | 0.796±0.089 | Triaud et al. (2013); Fossati et al. (2022) |
WASP-127b | G5V | 1.39±0.03 | <6.8 | < 16.8 | 2 | 0.180±0.020 | 1.370±0.040 | 0.087±0.012 | Lam et al. (2017); dos Santos et al. (2020) |
Notes. (a) Equivalent width of the net transmission planetary signal.(b) Model employed to calculate XUV flux (see text): coronal model with (1) and without (2) UV data; X vs. EUV relation (3); X-rays vs Prot relation (4); and blackbody emission (5).(c) No error bars associated with the mass are used in the plot of these objects.
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