Table C.2
MCMC results for discs with gaps or extended emission fit by a double Gaussian.
| Best Fits | |||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|
| Disc | R1 (au) | R2 (au) | σ1 (au) | σ2 (au) | C | Σc | PA (°) | Δ α (mas) | Δ δ (mas) | i (°) | F* (μ Jy) |
| HD 10647 | 89.2 | 168 | 12 | 48 | 0.659 | −4.433 | 56.93 | 121 | −17 | 79.08 | 128 |
| HD 15115 | 65.8 | 97.54 | 1.6 | 4.75 | 0.26 | −3.40 | 98.466 | 37 | −14 | 86.7 | 23 |
| HD 61005 | 69.7 | 94 | 7.3 | 32.3 | 0.836 | −3.358 | 70.29 | 2 | −16 | 86.2 | 1 |
| HD 92945 | 57.1 | 102.7 | 5.6 | 24.1 | 0.52 | −4.09 | 100.9 | −70 | −87 | 66.3 | 39 |
| HD 109573 | 77.65 | 85 | 2.98 | 24 | 0.979 | −2.77 | 26.52 | 13.8 | −39.9 | 76.54 | 52 |
| HD 121617 | 75.2 | 100 | 6 | 42 | 0.948 | −3.17 | 58.0 | 0 | −2 | 43.9 | 5 |
| HD 131488 | 90.8 | 95.1 | 0.69 | 17.3 | 0.97 | −1.96 | 97.305 | 1.1 | −7.3 | 84.84 | 40 |
| HD 131835 | 68.7 | 104.2 | 4.9 | 44.7 | 0.866 | −2.9 | 58.94 | 1.4 | −5.9 | 74.47 | 4 |
| HD 206893 | 42 | 125 | 6 | 36 | 0.43 | −4.53 | 64 | −50 | 20 | 44 | 17 |
| Medians | |||||||||||
| Disc | R1 (au) | R2 (au) | σ1 (au) | σ2 (au) | C | Σc | PA (°) | Δ α (mas) | Δ δ (mas) | i (°) | F* (μ Jy) |
| HD 10647 | ![]() |
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| HD 15115 | ![]() |
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| HD 61005 | ![]() |
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| HD 92945 | ![]() |
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| HD 109573 | ![]() |
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| HD 121617 | ![]() |
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| HD 131488 | ![]() |
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| HD 131835 | ![]() |
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| HD 206893 | ![]() |
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Notes. The top half of the table describes the best fits, while the bottom half describes the median values and their uncertainties, as calculated from the 16th and 84th percentiles of the posterior distribution. The surface density normalisation Σc is parametrised as an exponent, with 10Σc in units of g cm−2. Although HD 15115, HD 107146, and HD 197481 are included in this table, these discs are better fit by variations of the triple power law or double power law functional forms. These results can be found in Table C.3.
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