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Table 3

Sizes of the 2.2 μm continuum and Brγ emission (listed as 2.2 μm/Brγ) towards G034.8211, G282.2988, G287.3716, G301.8147, G231.7986, and G233.8306 based on a single (i.e. Gaussian, disc) brightness distribution fit in LITpro.

Source Model Flux w. 1 Flux w. 2 Flux w. 3 Diameter(†) Flatten ratio PA (minor axis) Red. χ2 Measured size(a)
[2.2 μm/Brγ] (mas) [2.2 μm/Brγ] [2.2 μm/Brγ] [2.2 μm/Brγ] (mas)
(degrees)
G034.8211 Disc n/a 1.0 n/a 5.65 ± 0.08/6.2 ± 0.8 1.50 ± 0.02∕1.5 ± 0.2 34 ± 2/25 ± 10 10/20
Gaussian n/a 1.0 n/a 3.46 ± 0.02/3.42 ± 0.06 1.52 ± 0.01/1.51 ± 0.04 20 ± 1/17 ± 4 20/17 3.47 ± 0.04
Ring n/a 1.0 n/a 6.2 ± 0.4/3 ± 1 1.50 ± 0.1/1.5 ± 0.3 23 ± 14/24 ± 17 30/35
G301.8147 Disc 0.26 ± 0.04 0.22 ± 0.03 0.52 ± 0.08 5.22 ± 0.1/2.27 ± 0.07 n/a n/a 3/6
Gaussian 0.22 ± 0.03 0.28 ± 0.04 0.50 ± 0.08 3.1 ± 0.1/1.42 ± 0.04 n/a n/a 2.8/7 3.0 ± 0.1
Ring 0.22 ± 0.07 0.26 ± 0.06 0.52 ± 0.08 5.2(b)/2.26(b) n/a n/a 3/8
G287.3716 Disc 0.62 ± 0.06 0.38 ± 0.04 n/a 4.42 ± 0.07/3.68 ± 0.4 n/a n/a 1.8/7
Gaussian 0.52 ± 0.05 0.48 ± 0.05 n/a 2.34 ± 0.05/1.28 ± 0.05 n/a n/a 1.76/2.3 2.15 ± 0.03
Ring 0.62 ± 0.09 0.38 ± 0.07 n/a 4.42(b)/2.00 ± 0.01 n/a n/a 1.8/2.6
G282.2988 Disc 0.64 ± 0.15 0.27 ± 0.06 0.09 ± 0.02 3.29 ± 0.07/1.77 ± 0.01 n/a n/a 13/17
Gaussian 0.55 ± 0.10 0.36 ± 0.08 0.09 ± 0.02 1.69 ± 0.04/1.25 ± 0.8 n/a n/a 12/5 2.15 ± 0.02
Ring 0.65 ± 0.20 0.27 ± 0.08 0.09 ± 0.02 3.3(b)/1.5(b) n/a n/a 12/25
G231.7986 Disc n/a 0.91 ± 0.02 0.09 ± 0.02 1.8 ± 0.01 n/a n/a 2 n/a
Gaussian n/a 0.91 ± 0.02 0.09 ± 0.02 1.1 ± 0.01 n/a n/a 2
Ring n/a 0.91 ± 0.02 0.09 ± 0.02 1.4 ± 0.03 n/a n/a 2.2
G233.8306 Disc n/a 0.84 ± 0.05 0.16 ± 0.04 3.6 ± 0.03 n/a n/a 2.3 n/a
Gaussian n/a 0.84 ± 0.05 0.16 ± 0.04 2.15 ± 0.03 n/a n/a 2
Ring n/a 0.84 ± 0.05 0.16 ± 0.04 2.55 ± 0.05 n/a n/a 2.6

Notes. The flux weights 1, 2, and 3 correspond to the fractional flux contributions of the star (point source), dust (disc, Gaussian, or ring), and that of a diffuse emission when a background was added, respectively.A binary component resulted in a better fit to the visibilities (see Sect. 4.2). (a)The measured size of the reconstructed 2.2 μm images (WISARD) as a result of a 2D Gaussian fit (Appendix B). (b)When the fitting procedure resulted in a ring of 0 mas diameter, the ring width was used instead to estimate the size of the emission. (†)For ring brightness distributions this corresponds to the internal diameter of a normalised uniform ring.

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