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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 89.10.8+0.7$89.1_{-0.8}^{+0.7}$ 1648+6$164_{-8}^{+6}$ 11.90.9+1.0$11.9_{-0.9}^{+1.0}$ 463+3$46_{-3}^{+3}$ 0.6640.010+0.009$0.664_{-0.010}^{+0.009}$ 4.4380.012+0.012$-4.438_{-0.012}^{+0.012}$ 56.930.05+0.06$56.93_{-0.05}^{+0.06}$ 12110+10$121_{-10}^{+10}$ 237+9$-23_{-7}^{+9}$ 79.000.18+0.12$79.00_{-0.18}^{+0.12}$ 13010+10$130_{-10}^{+10}$
HD 15115 65.80.3+0.6$65.8_{-0.3}^{+0.6}$ 97.570.05+0.07$97.57_{-0.05}^{+0.07}$ 2.40.8+1.0$2.4_{-0.8}^{+1.0}$ 4.730.20+0.18$4.73_{-0.20}^{+0.18}$ 0.190.04+0.06$0.19_{-0.04}^{+0.06}$ 3.440.02+0.04$-3.44_{-0.02}^{+0.04}$ 98.4600.013+0.011$98.460_{-0.013}^{+0.011}$ 363+2$36_{-3}^{+2}$ 140.9+0.9$-14_{-0.9}^{+0.9}$ 86.710.02+0.03$86.71_{-0.02}^{+0.03}$ 286+5$28_{-6}^{+5}$
HD 61005 69.40.4+0.5$69.4_{-0.4}^{+0.5}$ 953+2$95_{-3}^{+2}$ 7.40.5+0.5$7.4_{-0.5}^{+0.5}$ 31.71.5+1.6$31.7_{-1.5}^{+1.6}$ 0.8370.012+0.012$0.837_{-0.012}^{+0.012}$ 3.3590.015+0.016$-3.359_{-0.015}^{+0.016}$ 70.290.03+0.02$70.29_{-0.03}^{+0.02}$ 05+5$0_{-5}^{+5}$ 172+2$-17_{-2}^{+2}$ 86.170.07+0.05$86.17_{-0.07}^{+0.05}$ 54+7$5_{-4}^{+7}$
HD 92945 57.00.8+0.8$57.0_{-0.8}^{+0.8}$ 102.71.5+1.5$102.7_{-1.5}^{+1.5}$ 5.51.1+1.2$5.5_{-1.1}^{+1.2}$ 25.11.9+2.0$25.1_{-1.9}^{+2.0}$ 0.520.03+0.04$0.52_{-0.03}^{+0.04}$ 4.100.03+0.04$-4.10_{-0.03}^{+0.04}$ 100.50.5+0.5$100.5_{-0.5}^{+0.5}$ 8030+30$-80_{-30}^{+30}$ 7816+17$-78_{-16}^{+17}$ 66.00.6+0.5$66.0_{-0.6}^{+0.5}$ 3615+15$36_{-15}^{+15}$
HD 109573 77.610.16+0.04$77.61_{-0.16}^{+0.04}$ 841.8+2.1$84_{-1.8}^{+2.1}$ 2.890.19+0.18$2.89_{-0.19}^{+0.18}$ 224+4$22_{-4}^{+4}$ 0.9770.009+0.006$0.977_{-0.009}^{+0.006}$ 2.770.02+0.02$-2.77_{-0.02}^{+0.02}$ 26.510.07+0.05$26.51_{-0.07}^{+0.05}$ 13.90.8+0.8$13.9_{-0.8}^{+0.8}$ 39.61.2+1.2$-39.6_{-1.2}^{+1.2}$ 76.650.09+0.09$76.65_{-0.09}^{+0.09}$ 3817+17$38_{-17}^{+17}$
HD 121617 75.30.3+0.4$75.3_{-0.3}^{+0.4}$ 1035+8$103_{-5}^{+8}$ 60.5+0.5$6_{-0.5}^{+0.5}$ 427+8$42_{-7}^{+8}$ 0.9520.010+0.008$0.952_{-0.010}^{+0.008}$ 3.170.02+0.03$-3.17_{-0.02}^{+0.03}$ 58.30.6+0.6$58.3_{-0.6}^{+0.6}$ 12+2$-1_{-2}^{+2}$ 22+3$-2_{-2}^{+3}$ 44.10.5+0.6$44.1_{-0.5}^{+0.6}$ 128+11$12_{-8}^{+11}$
HD 131488 90.840.08+0.18$90.84_{-0.08}^{+0.18}$ 96.10.7+0.6$96.1_{-0.7}^{+0.6}$ 0.960.19+0.28$0.96_{-0.19}^{+0.28}$ 19.31.3+1.9$19.3_{-1.3}^{+1.9}$ 0.9660.006+0.006$0.966_{-0.006}^{+0.006}$ 2.080.10+0.08$-2.08_{-0.10}^{+0.08}$ 97.3010.029+0.012$97.301_{-0.029}^{+0.012}$ 1.20.6+0.6$1.2_{-0.6}^{+0.6}$ 7.10.3+0.3$-7.1_{-0.3}^{+0.3}$ 84.870.03+0.06$84.87_{-0.03}^{+0.06}$ 388+8$38_{-8}^{+8}$
HD 131835 68.50.4+0.4$68.5_{-0.4}^{+0.4}$ 105.81.7+2.0$105.8_{-1.7}^{+2.0}$ 4.90.6+0.6$4.9_{-0.6}^{+0.6}$ 43.51.5+1.3$43.5_{-1.5}^{+1.3}$ 0.8690.010+0.011$0.869_{-0.010}^{+0.011}$ 2.9390.04+0.04$-2.939_{-0.04}^{+0.04}$ 58.950.18+0.18$58.95_{-0.18}^{+0.18}$ 1.61.8+1.8$1.6_{-1.8}^{+1.8}$ 5.61.4+1.3$-5.6_{-1.4}^{+1.3}$ 74.410.20+0.20$74.41_{-0.20}^{+0.20}$ 107+11$10_{-7}^{+11}$
HD 206893 425+5$42_{-5}^{+5}$ 1263+4$126_{-3}^{+4}$ 64+9$6_{-4}^{+9}$ 363+4$36_{-3}^{+4}$ 0.380.17+0.22$0.38_{-0.17}^{+0.22}$ 4.570.12+0.20$-4.57_{-0.12}^{+0.20}$ 623+3$62_{-3}^{+3}$ 1060+60$-10_{-60}^{+60}$ 3050+50$30_{-50}^{+50}$ 462+3$46_{-2}^{+3}$ 146+6$14_{-6}^{+6}$

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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