Table 1
Sample of objects used this work.
Target | RA (ICRS J2000) | Dec (ICRS J2000) | d (pc) | SpT | M* (M⊙) | log L* (L⊙) | log Lacc (L⊙) | log Ṁ (M⊙ yr−1) | log Lx (erg s−1) | inc (deg) | Ref. |
---|---|---|---|---|---|---|---|---|---|---|---|
AB Aur | 04:55:45.8459 | +30:33:04.2921 | 163 | A0 | 2.2 | 29.88 ± 0.30(‡) | 23 | 1, 2, 2, 5 | |||
GGTau AA/Ab | 04:32:30.3507 | +17:31:40.4941 | 149 | K7 | 0.7 | 0.20 ± 0.20 (*) | 0.024 ± 0.25 | −7.3 ± 0.5 | 29.64 ± 0.30‡ | 36 | 3, †, 3, 5 |
HD 100453 | 11:33:05.5766 | −54:19:28.5471 | 104 | A9 | 1.5 | - | 30 | 2, 2, 2 | |||
HD 100546 | 11:33:25.4409 | −70:11:41.2413 | 110 | B9 | 2.2 | 0.97 ± 0.14 | 29.22 ± 0.30(‡) | 42 | 2, 2, 2, 5 | ||
HD 135344B | 15:15:48.4460 | −37:09:16.0243 | 136 | F5 | 1.6 | - | 12 | 2, 2, 2, 5 | |||
HD 142527 | 15:56:41.8883 | −42:19:23.2483 | 157 | F6 | 2.3 | 29.60 ± 0.30(‡) | 27 | 2, 2, 2, 5 | |||
HD 169142 | 18:24:29.7800 | −29:46:49.3274 | 114 | A5 | 2 | 0.59 ± 0.15 | 28.90 ± 0.30(‡) | 12 | 1, 2, 2, 5 | ||
MWC758 | 05:30:27.5286 | +25:19:57.0763 | 160 | A7 | 1.6 | 29.18 ± 0.09 | 21 | 1, 2, 2, 6 | |||
SR24S | 16:26:58.5134 | −24:45:36.7226 | 114 | K1 | 1.5 | 0.40 ± 0.20(*) | 0.10 ± 0.25 | −7.15 ± 0.5 | - | 46 | 3, †, 3 |
TCha | 11:57:13.5245 | −79:21:31.5305 | 110 | K0 | 1.2 | 0.11 ± 0.20(*) | 0.012 ± 0.25 | −8.4 ± 0.5 | 30.47 ± 0.30(‡) | 73 | 3, †, 3, 5 |
WSB60 | 16:28:16.5129 | −24:36:58.0549 | 137 | M6 | 0.2 | 0.33 ± 0.20(*) | −1.51 ± 0.25 | −7.93 ± 0.35 | - | 28 | 4, 4, 4 |
Notes. Columns show the star coordinates; distance, d; spectral type, SpT; stellar mass, M* ; and luminosity, L*; accretion luminosity, ; accretion rate onto the central star, Ṁ ; X-ray luminosity; and the outer disk inclination, inc. The last column reports the references for the luminosity, accretion luminosity, accretion rates, and X-ray luminosity. Distances are from Gaia DR2 (Gaia Collaboration 2018). The inclination of the outer disks are from Francis & van der Marel (2020) and their typical uncertainty is in the range of a few degrees. (*)The uncertainty on the luminosity for these targets is assumed to be 0.20 dex, based on the typical uncertainty estimated by Wichittanakom et al. (2020). (†)The accretion luminosity on these targets is calculated with Eq. (2) in Wichittanakom et al. (2020), with uncertainties assumed to be 0.25 dex (Manara et al. 2023).(‡) X-ray luminosities derived correcting the fluxes reported in Table 4 in Dionatos et al. (2019) for the distance of each target and assuming a 0.30 dex uncertainty (Güdel et al. 2007).
References: (1) Vioque et al. (2018), (2) Wichittanakom et al. (2020), (3) Francis & van der Marel (2020), (4) Manara et al. (2023), (5) Dionatos et al. (2019), (6) Ryspaeva et al. (2023).
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